Sample records for p-i-n detector diodes

  1. Dead layer on silicon p-i-n diode charged-particle detectors

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Wall, B. L.; Amsbaugh, John F.; Beglarian, A.

    Abstract Semiconductor detectors in general have a dead layer at their surfaces that is either a result of natural or induced passivation, or is formed during the process of making a contact. Charged particles passing through this region produce ionization that is incompletely collected and recorded, which leads to departures from the ideal in both energy deposition and resolution. The silicon p-i-n diode used in the KATRIN neutrinomass experiment has such a dead layer. We have constructed a detailed Monte Carlo model for the passage of electrons from vacuum into a silicon detector, and compared the measured energy spectra tomore » the predicted ones for a range of energies from 12 to 20 keV. The comparison provides experimental evidence that a substantial fraction of the ionization produced in the "dead" layer evidently escapes by discussion, with 46% being collected in the depletion zone and the balance being neutralized at the contact or by bulk recombination. The most elementary model of a thinner dead layer from which no charge is collected is strongly disfavored.« less

  2. Characterization of Si p-i-n diode for scanning transmission ion microanalysis of biological samples

    NASA Astrophysics Data System (ADS)

    Devès, G.; Matsuyama, S.; Barbotteau, Y.; Ishii, K.; Ortega, R.

    2006-05-01

    The performance of a silicon p-i-n diode (Hamamatsu S1223-01) for the detection of charged particles was investigated and compared with the response of a standard passivated implanted planar silicon (PIPS) detector. The photodiode was characterized by ion beam induced charge collection with a micrometer spatial resolution using proton and alpha particle beams in the 1-3MeV energy range. Results indicate that homogeneity, energy resolution, and reproducibility of detection of charged particles enable the use of the low cost silicon p-i-n device as a replacement of conventional PIPS detector during scanning transmission ion microanalysis experiments. The Si p-i-n diode detection setup was successfully applied to scanning transmission ion microscopy determination of subcellular compartments on human cancer cultured cells.

  3. Strain tunable light emitting diodes with germanium P-I-N heterojunctions

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Lagally, Max G; Sanchez Perez, Jose Roberto

    Tunable p-i-n diodes comprising Ge heterojunction structures are provided. Also provided are methods for making and using the tunable p-i-n diodes. Tunability is provided by adjusting the tensile strain in the p-i-n heterojunction structure, which enables the diodes to emit radiation over a range of wavelengths.

  4. Thermal characterization of gallium nitride p-i-n diodes

    NASA Astrophysics Data System (ADS)

    Dallas, J.; Pavlidis, G.; Chatterjee, B.; Lundh, J. S.; Ji, M.; Kim, J.; Kao, T.; Detchprohm, T.; Dupuis, R. D.; Shen, S.; Graham, S.; Choi, S.

    2018-02-01

    In this study, various thermal characterization techniques and multi-physics modeling were applied to understand the thermal characteristics of GaN vertical and quasi-vertical power diodes. Optical thermography techniques typically used for lateral GaN device temperature assessment including infrared thermography, thermoreflectance thermal imaging, and Raman thermometry were applied to GaN p-i-n diodes to determine if each technique is capable of providing insight into the thermal characteristics of vertical devices. Of these techniques, thermoreflectance thermal imaging and nanoparticle assisted Raman thermometry proved to yield accurate results and are the preferred methods of thermal characterization of vertical GaN diodes. Along with this, steady state and transient thermoreflectance measurements were performed on vertical and quasi-vertical GaN p-i-n diodes employing GaN and Sapphire substrates, respectively. Electro-thermal modeling was performed to validate measurement results and to demonstrate the effect of current crowding on the thermal response of quasi-vertical diodes. In terms of mitigating the self-heating effect, both the steady state and transient measurements demonstrated the superiority of the tested GaN-on-GaN vertical diode compared to the tested GaN-on-Sapphire quasi-vertical structure.

  5. A recoil-proton spectrometer based on a p-i-n diode implementing pulse-shape discrimination.

    PubMed

    Agosteo, S; D'Angelo, G; Fazzi, A; Foglio Para, A; Pola, A; Ventura, L; Zotto, P

    2004-01-01

    A recoil-proton spectrometer was created by coupling a p-i-n diode with a polyethylene converter. The maximum detectable energy, imposed by the thickness of the totally depleted layer, is approximately 6 MeV. The minimum detectable energy is limited by the contribution of secondary electrons generated by photons in the detector assembly. This limit is approximately 1.5 MeV at full-depletion voltage and was decreased using pulse-shape discrimination. The diode was set up in the 'reverse-injection' configuration (i.e. with the N+ layer adjacent to the converter). This configuration provides longer collection times for the electron-hole pairs generated by the recoil-protons. The pulse-shape discrimination was based on the zero-crossing time of bipolar signals from a (CR)2-(RC)2 filter. The detector was characterised using monoenergetic neutrons generated in the Van De Graaff CN accelerator at the INFN-Laboratori Nazionali di Legnaro. The energy limit for discrimination proved to be approximately 900 keV.

  6. Carbon nanotube intramolecular p-i-n junction diodes with symmetric and asymmetric contacts

    PubMed Central

    Chen, Changxin; Liao, Chenghao; Wei, Liangming; Zhong, Hanqing; He, Rong; Liu, Qinran; Liu, Xiaodong; Lai, Yunfeng; Song, Chuanjuan; Jin, Tiening; Zhang, Yafei

    2016-01-01

    A p-i-n junction diode based on the selectively doped single-walled carbon nanotube (SWCNT) had been investigated, in which two opposite ends of individual SWCNT channel were doped into the p- and n-type SWCNT respectively while the middle segment of SWCNT was kept as the intrinsic. The symmetric and asymmetric contacts were used to fabricate the p-i-n junction diodes respectively and studied the effect of the contact on the device characteristics. It was shown that a low reverse saturation current of ~20 pA could be achieved by these both diodes. We found that the use of the asymmetric contact can effectively improve the performance of the p-i-n diode, with the rectification ratio enhanced from ~102 for the device with the Au/Au symmetric contact to >103 for the one with the Pd/Al asymmetric contact. The improvement of the device performance by the asymmetric-contact structure was attributed to the decrease of the effective Schottky-barrier height at the contacts under forward bias, increasing the forward current of the diode. The p-i-n diode with asymmetric contact also had a higher rectification ratio than its counterpart before doping the SWCNT channel, which is because that the p-i-n junction in the device decreased the reverse saturated current. PMID:26915400

  7. Characterization of an Mg-implanted GaN p-i-n Diode

    DTIC Science & Technology

    2016-03-31

    unintentionally doped GaN layer was grown by metal organic chemical vapor deposition (MOCVD) on a n+ Ga -face c-oriented GaN substrate. The as-grown MOCVD film...their proper lattice sites. In the case of Mg implanted GaN , the Mg must replace Ga to result in p-type material. In many other semiconductor...Characterization of an Mg-implanted GaN p-i-n Diode Travis J. Anderson, Jordan D. Greenlee, Boris N. Feigelson, Karl D. Hobart, and Francis J

  8. A p-i-n junction diode based on locally doped carbon nanotube network

    PubMed Central

    Liu, Xiaodong; Chen, Changxin; Wei, Liangming; Hu, Nantao; Song, Chuanjuan; Liao, Chenghao; He, Rong; Dong, Xusheng; Wang, Ying; Liu, Qinran; Zhang, Yafei

    2016-01-01

    A p-i-n junction diode constructed by the locally doped network of single-walled carbon nanotubes (SWNTs) was investigated. In this diode, the two opposite ends of the SWNT-network channel were selectively doped by triethyloxonium hexachloroantimonate (OA) and polyethylenimine (PEI) to obtain the air-stable p- and n-type SWNTs respectively while the central area of the SWNT-network remained intrinsic state, resulting in the formation of a p-i-n junction with a strong built-in electronic field in the SWNTs. The results showed that the forward current and the rectification ratio of the diode increased as the doping degree increased. The forward current of the device could also be increased by decreasing the channel length. A high-performance p-i-n junction diode with a high rectification ratio (~104), large forward current (~12.2 μA) and low reverse saturated current (~1.8 nA) was achieved with the OA and PEI doping time of 5 h and 18 h for a channel length of ~6 μm. PMID:26996610

  9. A p-i-n junction diode based on locally doped carbon nanotube network.

    PubMed

    Liu, Xiaodong; Chen, Changxin; Wei, Liangming; Hu, Nantao; Song, Chuanjuan; Liao, Chenghao; He, Rong; Dong, Xusheng; Wang, Ying; Liu, Qinran; Zhang, Yafei

    2016-03-21

    A p-i-n junction diode constructed by the locally doped network of single-walled carbon nanotubes (SWNTs) was investigated. In this diode, the two opposite ends of the SWNT-network channel were selectively doped by triethyloxonium hexachloroantimonate (OA) and polyethylenimine (PEI) to obtain the air-stable p- and n-type SWNTs respectively while the central area of the SWNT-network remained intrinsic state, resulting in the formation of a p-i-n junction with a strong built-in electronic field in the SWNTs. The results showed that the forward current and the rectification ratio of the diode increased as the doping degree increased. The forward current of the device could also be increased by decreasing the channel length. A high-performance p-i-n junction diode with a high rectification ratio (~10(4)), large forward current (~12.2 μA) and low reverse saturated current (~1.8 nA) was achieved with the OA and PEI doping time of 5 h and 18 h for a channel length of ~6 μm.

  10. A p-i-n junction diode based on locally doped carbon nanotube network

    NASA Astrophysics Data System (ADS)

    Liu, Xiaodong; Chen, Changxin; Wei, Liangming; Hu, Nantao; Song, Chuanjuan; Liao, Chenghao; He, Rong; Dong, Xusheng; Wang, Ying; Liu, Qinran; Zhang, Yafei

    2016-03-01

    A p-i-n junction diode constructed by the locally doped network of single-walled carbon nanotubes (SWNTs) was investigated. In this diode, the two opposite ends of the SWNT-network channel were selectively doped by triethyloxonium hexachloroantimonate (OA) and polyethylenimine (PEI) to obtain the air-stable p- and n-type SWNTs respectively while the central area of the SWNT-network remained intrinsic state, resulting in the formation of a p-i-n junction with a strong built-in electronic field in the SWNTs. The results showed that the forward current and the rectification ratio of the diode increased as the doping degree increased. The forward current of the device could also be increased by decreasing the channel length. A high-performance p-i-n junction diode with a high rectification ratio (~104), large forward current (~12.2 μA) and low reverse saturated current (~1.8 nA) was achieved with the OA and PEI doping time of 5 h and 18 h for a channel length of ~6 μm.

  11. Semiconductor P-I-N detector

    DOEpatents

    Sudharsanan, Rengarajan; Karam, Nasser H.

    2001-01-01

    A semiconductor P-I-N detector including an intrinsic wafer, a P-doped layer, an N-doped layer, and a boundary layer for reducing the diffusion of dopants into the intrinsic wafer. The boundary layer is positioned between one of the doped regions and the intrinsic wafer. The intrinsic wafer can be composed of CdZnTe or CdTe, the P-doped layer can be composed of ZnTe doped with copper, and the N-doped layer can be composed of CdS doped with indium. The boundary layers is formed of an undoped semiconductor material. The boundary layer can be deposited onto the underlying intrinsic wafer. The doped regions are then typically formed by a deposition process or by doping a section of the deposited boundary layer.

  12. Design and characterization of GaN p-i-n diodes for betavoltaic devices

    NASA Astrophysics Data System (ADS)

    Khan, Muhammad R.; Smith, Joshua R.; Tompkins, Randy P.; Kelley, Stephen; Litz, Marc; Russo, John; Leathersich, Jeff; Shahedipour-Sandvik, Fatemeh (Shadi); Jones, Kenneth A.; Iliadis, Agis

    2017-10-01

    The performance of gallium nitride (GaN) p-i-n diodes were investigated for use as a betavoltaic device. Dark IV measurements showed a turn on-voltage of approximately 3.2 V, specific-on-resistance of 15.1 mΩ cm2 and a reverse leakage current of -0.14 mA/cm2 at -10 V. A clear photo-response was observed when IV curves were measured under a light source at a wavelength of 310 nm (4.0 eV). In addition, GaN p-i-n diodes were tested under an electron-beam in order to simulate common beta radiation sources ranging from that of 3H (5.6 keV average) to 63Ni (17 keV average). From this data, we estimated output powers of 53 nW and 750 nW with overall efficiencies of 0.96% and 4.4% for our device at incident electron energies of 5.6 keV and 17 keV corresponding to 3H and 63Ni beta sources respectively.

  13. Performance and breakdown characteristics of irradiated vertical power GaN P-i-N diodes

    DOE PAGES

    King, M. P.; Armstrong, A. M.; Dickerson, J. R.; ...

    2015-10-29

    Electrical performance and defect characterization of vertical GaN P-i-N diodes before and after irradiation with 2.5 MeV protons and neutrons is investigated. Devices exhibit increase in specific on-resistance following irradiation with protons and neutrons, indicating displacement damage introduces defects into the p-GaN and n- drift regions of the device that impact on-state device performance. The breakdown voltage of these devices, initially above 1700 V, is observed to decrease only slightly for particle fluence <; 10 13 cm -2. Furthermore, the unipolar figure of merit for power devices indicates that while the on-resistance and breakdown voltage degrade with irradiation, vertical GaNmore » P-i-Ns remain superior to the performance of the best available, unirradiated silicon devices and on-par with unirradiated modern SiC-based power devices.« less

  14. Driving force of stacking-fault formation in SiC p-i-n diodes.

    PubMed

    Ha, S; Skowronski, M; Sumakeris, J J; Paisley, M J; Das, M K

    2004-04-30

    The driving force of stacking-fault expansion in SiC p-i-n diodes was investigated using optical emission microscopy and transmission electron microscopy. The stacking-fault expansion and properties of the partial dislocations were inconsistent with any stress as the driving force. A thermodynamic free energy difference between the perfect and a faulted structure is suggested as a plausible driving force in the tested diodes, indicating that hexagonal polytypes of silicon carbide are metastable at room temperature.

  15. Characterization of Lateral Structure of the p-i-n Diode for Thin-Film Silicon Solar Cell.

    PubMed

    Kiaee, Zohreh; Joo, Seung Ki

    2018-03-01

    The lateral structure of the p-i-n diode was characterized for thin-film silicon solar cell application. The structure can benefit from a wide intrinsic layer, which can improve efficiency without increasing cell thickness. Compared with conventional thin-film p-i-n cells, the p-i-n diode lateral structure exploited direct light irradiation on the absorber layer, one-side contact, and bifacial irradiation. Considering the effect of different carrier lifetimes and recombinations, we calculated efficiency parameters by using a commercially available simulation program as a function of intrinsic layer width, as well as the distance between p/i or n/i junctions to contacts. We then obtained excellent parameter values of 706.52 mV open-circuit voltage, 24.16 mA/Cm2 short-circuit current, 82.66% fill factor, and 14.11% efficiency from a lateral cell (thickness = 3 μm; intrinsic layer width = 53 μm) in monofacial irradiation mode (i.e., only sunlight from the front side was considered). Simulation results of the cell without using rear-side reflector in bifacial irradiation mode showed 11.26% front and 9.72% rear efficiencies. Our findings confirmed that the laterally structured p-i-n cell can be a potentially powerful means for producing highly efficient, thin-film silicon solar cells.

  16. 4H-SiC p i n diodes grown by sublimation epitaxy in vacuum (SEV) and their application as microwave diodes

    NASA Astrophysics Data System (ADS)

    Camara, N.; Zekentes, K.; Zelenin, V. V.; Abramov, P. L.; Kirillov, A. V.; Romanov, L. P.; Boltovets, N. S.; Krivutsa, V. A.; Thuaire, A.; Bano, E.; Tsoi, E.; Lebedev, A. A.

    2008-02-01

    Sublimation epitaxy under vacuum (SEV) was investigated as a method for growing 4H-SiC epitaxial structures for p-i-n diode fabrication. The SEV-grown 4H-SiC material was investigated with scanning electron microscopy (SEM), atomic force microscopy (AFM), x-ray diffraction, photo-luminescence spectroscopy (PL), cathodo-luminescence (CL) spectroscopy, photocurrent method for carrier diffusion length determination, electro-luminescence microscopy (EL), deep level transient spectroscopy (DLTS), C-V profiling and Hall-effect measurements. When possible, the same investigation techniques were used in parallel with similar layers grown by chemical vapour deposition (CVD) epitaxy and the physical properties of the two kind of epitaxied layers were compared. p-i-n diodes were fabricated in parallel on SEV and CVD-grown layers and showed close electrical performances in dc mode in term of capacitance, resistance and transient time switching, despite the lower mobility and the diffusion length of the SEV-grown layers. X-band microwave switches based on the SEV-grown p-i-n diodes have been demonstrated with insertion loss lower than 4 dB and an isolation higher than 17 dB. These single-pole single-throw (SPST) switches were able to handle a pulsed power up to 1800 W in isolation mode, similar to the value obtained with switches incorporating diodes with CVD-grown layers.

  17. Current-voltage characteristics of n-AlMgZnO/p-GaN junction diodes

    NASA Astrophysics Data System (ADS)

    Hsueh, Kuang-Po; Cheng, Po-Wei; Cheng, Yi-Chang; Sheu, Jinn-Kong; Yeh, Yu-Hsiang; Chiu, Hsien-Chin; Wang, Hsiang-Chun

    2013-03-01

    This study investigates the temperature dependence of the current-voltage (I-V) characteristics of Al-doped MgxZn1-xO/p-GaN junction diodes. Specifically, this study reports the deposition of n-type Al-doped MgxZn1-xO (AMZO) films on p-GaN using a radio-frequency (RF) magnetron sputtering system followed by annealing at 700, 800, 900, and 1000 °C in a nitrogen ambient for 60 seconds, respectively. The AMZO/GaN films were thereafter analyzed using Hall measurement and the x-ray diffraction (XRD) patterns. The XRD results show that the diffraction angles of the annealed AMZO films remain the same as that of GaN without shifting. The n-AMZO/p-GaN diode with 900 °C annealing had the lowest leakage current in forward and reverse bias. However, the leakage current of the diodes did not change significantly with an increase in annealing temperatures. These findings show that the n-AMZO/p-GaN junction diode is feasible for GaN-based heterojunction bipolar transistors (HBTs) and UV light-emitting diodes (LEDs).

  18. CONDENSED MATTER: ELECTRONIC STRUCTURE, ELECTRICAL, MAGNETIC, AND OPTICAL PROPERTIES: Research on reverse recovery characteristics of SiGeC p-i-n diodes

    NASA Astrophysics Data System (ADS)

    Gao, Yong; Liu, Jing; Yang, Yuan

    2008-12-01

    This paper analyses the reverse recovery characteristics and mechanism of SiGeC p-i-n diodes. Based on the integrated systems engineering (ISE) data, the critical physical models of SiGeC diodes are proposed. Based on hetero-junction band gap engineering, the softness factor increases over six times, reverse recovery time is over 30% short and there is a 20% decrease in peak reverse recovery current for SiGeC diodes with 20% of germanium and 0.5% of carbon, compared to Si diodes. Those advantages of SiGeC p-i-n diodes are more obvious at high temperature. Compared to lifetime control, SiGeC technique is more suitable for improving diode properties and the tradeoff between reverse recovery time and forward voltage drop can be easily achieved in SiGeC diodes. Furthermore, the high thermal-stability of SiGeC diodes reduces the costs of further process steps and offers more freedoms to device design.

  19. Lead Halide Perovskite Photovoltaic as a Model p-i-n Diode.

    PubMed

    Miyano, Kenjiro; Tripathi, Neeti; Yanagida, Masatoshi; Shirai, Yasuhiro

    2016-02-16

    The lead halide perovskite photovoltaic cells, especially the iodide compound CH3NH3PbI3 family, exhibited enormous progress in the energy conversion efficiency in the past few years. Although the first attempt to use the perovskite was as a sensitizer in a dye-sensitized solar cell, it has been recognized at the early stage of the development that the working of the perovskite photovoltaics is akin to that of the inorganic thin film solar cells. In fact, theoretically perovskite is always treated as an ordinary direct band gap semiconductor and hence the perovskite photovoltaics as a p-i-n diode. Despite this recognition, research effort along this line of thought is still in pieces and incomplete. Different measurements have been applied to different types of devices (different not only in the materials but also in the cell structures), making it difficult to have a coherent picture. To make the situation worse, the perovskite photovoltaics have been plagued by the irreproducible optoelectronic properties, most notably the sweep direction dependent current-voltage relationship, the hysteresis problem. Under such circumstances, it is naturally very difficult to analyze the data. Therefore, we set out to make hysteresis-free samples and apply time-tested models and numerical tools developed in the field of inorganic semiconductors. A series of electrical measurements have been performed on one type of CH3NH3PbI3 photovoltaic cells, in which a special attention was paid to ensure that their electronic reproducibility was better than the fitting error in the numerical analysis. The data can be quantitatively explained in terms of the established models of inorganic semiconductors: current/voltage relationship can be very well described by a two-diode model, while impedance spectroscopy revealed the presence of a thick intrinsic layer with the help of a numerical solver, SCAPS, developed for thin film solar cell analysis. These results point to that CH3NH3PbI3 is an

  20. Fabrication of p-Si/n-ZnO:Al heterojunction diode and determination of electrical parameters

    NASA Astrophysics Data System (ADS)

    Ilican, Saliha; Gorgun, Kamuran; Aksoy, Seval; Caglar, Yasemin; Caglar, Mujdat

    2018-03-01

    We present a fundamental experimental study of a microwave assisted chemical bath deposition (MW-CBD) method for Al doped ZnO films. Field emission scanning electron microscopy (FESEM) and X-ray diffraction (XRD) spectroscopy were used to analyze the microstructures and crystalline structures of these films, respectively. The p-Si/n-ZnO:Al heterojunction diodes were fabricated. The current-voltage (I-V) characteristics of these diodes were measured at room temperature. The important electrical parameters such as series resistance, the ideality factor and the barrier height were determined by performing plots from the forward bias I-V characteristics using different methods. The obtained results indicate that Al doping improve the electrical properties of the p-Si/n-ZnO diode. The best rectification properties were observed in the p-Si/n-ZnO:5%Al heterojunction diode, so only capacitance-voltage (C-V) measurements of this diode were taken. Electrical parameter values such as series resistance, the built-in potential and the acceptor concentration calculated for this heterojunction diode.

  1. Single n+-i-n+ InP nanowires for highly sensitive terahertz detection.

    PubMed

    Peng, Kun; Parkinson, Patrick; Gao, Qian; Boland, Jessica L; Li, Ziyuan; Wang, Fan; Mokkapati, Sudha; Fu, Lan; Johnston, Michael B; Tan, Hark Hoe; Jagadish, Chennupati

    2017-03-24

    Developing single-nanowire terahertz (THz) electronics and employing them as sub-wavelength components for highly-integrated THz time-domain spectroscopy (THz-TDS) applications is a promising approach to achieve future low-cost, highly integrable and high-resolution THz tools, which are desirable in many areas spanning from security, industry, environmental monitoring and medical diagnostics to fundamental science. In this work, we present the design and growth of n + -i-n + InP nanowires. The axial doping profile of the n + -i-n + InP nanowires has been calibrated and characterized using combined optical and electrical approaches to achieve nanowire devices with low contact resistances, on which the highly-sensitive InP single-nanowire photoconductive THz detectors have been demonstrated. While the n + -i-n + InP nanowire detector has a only pA-level response current, it has a 2.5 times improved signal-to-noise ratio compared with the undoped InP nanowire detector and is comparable to traditional bulk THz detectors. This performance indicates a promising path to nanowire-based THz electronics for future commercial applications.

  2. P-n junction diodes with polarization induced p-type graded InxGa1-xN layer

    NASA Astrophysics Data System (ADS)

    Enatsu, Yuuki; Gupta, Chirag; Keller, Stacia; Nakamura, Shuji; Mishra, Umesh K.

    2017-10-01

    In this study, p-n junction diodes with polarization induced p-type layer are demonstrated on Ga polar (0001) bulk GaN substrates. A quasi-p-type region is obtained by linearly grading the indium composition in un-doped InxGa1-xN layers from 0% to 5%, taking advantage of the piezoelectric and spontaneous polarization fields which exist in group III-nitride heterostructures grown in the typical (0001) or c-direction. The un-doped graded InxGa1-xN layers needed to be capped with a thin Mg-doped InxGa1-xN layer to make good ohmic contacts and to reduce the on-resistance of the p-n diodes. The Pol-p-n junction diodes exhibited similar characteristics compared to reference samples with traditional p-GaN:Mg layers. A rise in breakdown voltage from 30 to 110 V was observed when the thickness of the graded InGaN layer was increased from 100 to 600 nm at the same grade composition.

  3. p-n Junction Diodes Fabricated on Si-Si/Ge Heteroepitaxial Films

    NASA Technical Reports Server (NTRS)

    Das, K.; Mazumder, M. D. A.; Hall, H.; Alterovitz, Samuel A. (Technical Monitor)

    2000-01-01

    A set of photolithographic masks was designed for the fabrication of diodes in the Si-Si/Ge material system. Fabrication was performed on samples obtained from two different wafers: (1) a complete HBT structure with an n (Si emitter), p (Si/Ge base), and an n/n+ (Si collector/sub-collector) deposited epitaxially (MBE) on a high resistivity p-Si substrate, (2) an HBT structure where epitaxial growth was terminated after the p-type base (Si/Ge) layer deposition. Two different process runs were attempted for the fabrication of Si-Si/Ge (n-p) and Si/Ge-Si (p-n) junction diodes formed between the emitter-base and base-collector layers, respectively, of the Si-Si/Ge-Si HBT structure. One of the processes employed a plasma etching step to expose the p-layer in the structure (1) and to expose the e-layer in structure (2). The Contact metallization used for these diodes was a Cu-based metallization scheme that was developed during the first year of the grant. The plasma-etched base-collector diodes on structure (2) exhibited well-behaved diode-like characteristics. However, the plasma-etched emitter-base diodes demonstrated back-to-back diode characteristics. These back-to back characteristics were probably due to complete etching of the base-layer, yielding a p-n-p diode. The deep implantation process yielded rectifying diodes with asymmetric forward and reverse characteristics. The ideality factor of these diodes were between 1.6 -2.1, indicating that the quality of the MBE grown epitaxial films was not sufficiently high, and also incomplete annealing of the implantation damage. Further study will be conducted on CVD grown films, which are expected to have higher epitaxial quality.

  4. Flexible amorphous silicon PIN diode x-ray detectors

    NASA Astrophysics Data System (ADS)

    Marrs, Michael; Bawolek, Edward; Smith, Joseph T.; Raupp, Gregory B.; Morton, David

    2013-05-01

    A low temperature amorphous silicon (a-Si) thin film transistor (TFT) and amorphous silicon PIN photodiode technology for flexible passive pixel detector arrays has been developed using active matrix display technology. The flexible detector arrays can be conformed to non-planar surfaces with the potential to detect x-rays or other radiation with an appropriate conversion layer. The thin, lightweight, and robust backplanes may enable the use of highly portable x-ray detectors for use in the battlefield or in remote locations. We have fabricated detector arrays up to 200 millimeters along the diagonal on a Gen II (370 mm x 470 mm rectangular substrate) using plasma enhanced chemical vapor deposition (PECVD) a-Si as the active layer and PECVD silicon nitride (SiN) as the gate dielectric and passivation. The a-Si based TFTs exhibited an effective saturation mobility of 0.7 cm2/V-s, which is adequate for most sensing applications. The PIN diode material was fabricated using a low stress amorphous silicon (a-Si) PECVD process. The PIN diode dark current was 1.7 pA/mm2, the diode ideality factor was 1.36, and the diode fill factor was 0.73. We report on the critical steps in the evolution of the backplane process from qualification of the low temperature (180°C) TFT and PIN diode process on the 150 mm pilot line, the transfer of the process to flexible plastic substrates, and finally a discussion and demonstration of the scale-up to the Gen II (370 x 470 mm) panel scale pilot line.

  5. Improved ultraviolet emission performance from polarization-engineered n-ZnO/p-GaN heterojunction diode

    NASA Astrophysics Data System (ADS)

    Jiang, Junyan; Zhang, Yuantao; Chi, Chen; Shi, Zhifeng; Yan, Long; Li, Pengchong; Zhang, Baolin; Du, Guotong

    2016-02-01

    O-polar ZnO films were grown on N-polar p-GaN/sapphire substrates by photo-assisted metal-organic chemical vapor deposition, and further heterojunction light-emitting diodes based O-polar n-ZnO/N-polar p-GaN were proposed and fabricated. It is experimentally demonstrated that the interface polarization of O-polar n-ZnO/N-polar p-GaN heterojunction can shift the location of the depletion region from the interface deep into the ZnO side. When a forward bias is applied to the proposed diode, a strong and high-purity ultraviolet emission located at 385 nm can be observed. Compared with conventional Zn-polar n-ZnO/Ga-polar p-GaN heterostructure diode, the ultraviolet emission intensity of the proposed heterojunction diode is greatly enhanced due to the presence of polarization-induced inversion layer at the ZnO side of the heterojunction interface. This work provides an innovative path for the design and development of ZnO-based ultraviolet diode.

  6. Application of AXUV diode detectors at ASDEX Upgrade

    NASA Astrophysics Data System (ADS)

    Bernert, M.; Eich, T.; Burckhart, A.; Fuchs, J. C.; Giannone, L.; Kallenbach, A.; McDermott, R. M.; Sieglin, B.

    2014-03-01

    In the ASDEX Upgrade tokamak, a radiation measurement for a wide spectral range, based on semiconductor detectors, with 256 lines of sight and a time resolution of 5μs was recently installed. In combination with the foil based bolometry, it is now possible to estimate the absolutely calibrated radiated power of the plasma on fast timescales. This work introduces this diagnostic based on AXUV (Absolute eXtended UltraViolet) n-on-p diodes made by International Radiation Detectors, Inc. The measurement and the degradation of the diodes in a tokamak environment is shown. Even though the AXUV diodes are developed to have a constant sensitivity for all photon energies (1 eV-8 keV), degradation leads to a photon energy dependence of the sensitivity. The foil bolometry, which is restricted to a time resolution of less than 1 kHz, offers a basis for a time dependent calibration of the diodes. The measurements of the quasi-calibrated diodes are compared with the foil bolometry and found to be accurate on the kHz time scale. Therefore, it is assumed, that the corrected values are also valid for the highest time resolution (200 kHz). With this improved diagnostic setup, the radiation induced by edge localized modes is analyzed on fast timescales.

  7. The Influence of High-Energy Electrons Irradiation on Surface of n-GaP and on Au/n-GaP/Al Schottky Barrier Diode

    NASA Astrophysics Data System (ADS)

    Demir, K. Çinar; Kurudirek, S. V.; Oz, S.; Biber, M.; Aydoğan, Ş.; Şahin, Y.; Coşkun, C.

    We fabricated 25 Au/n-GaP/Al Schottky devices and investigated the influence of high electron irradiation, which has 12MeV on the devices, at room temperature. The X-ray diffraction patterns, scanning electron microscopic images and Raman spectra of a gallium phosphide (GaP) semiconductor before and after electron irradiation have been analyzed. Furthermore, some electrical measurements of the devices were carried out through the current-voltage (I-V) and capacitance-voltage (C-V) measurements. From the I-V characteristics, experimental ideality factor n and barrier height Φ values of these Schottky diodes have been determined before and after irradiation, respectively. The results have also been analyzed statically, and a gauss distribution has been obtained. The built-in potential Vbi, barrier height Φ, Fermi level EF and donor concentration Nd values have been determined from the reverse bias C-V and C-2-V curves of Au/n-GaP/Al Schottky barrier diodes at 100kHz before and after 12MeV electron irradiation. Furthermore, we obtained the series resistance values of Au/n-GaP/Al Schottky barrier diodes with the help of different methods. Experimental results confirmed that the electrical characterization of the device changed with the electron irradiation.

  8. Strong room temperature electroluminescence from lateral p-SiGe/i-Ge/n-SiGe heterojunction diodes on silicon-on-insulator substrate

    NASA Astrophysics Data System (ADS)

    Lin, Guangyang; Yi, Xiaohui; Li, Cheng; Chen, Ningli; Zhang, Lu; Chen, Songyan; Huang, Wei; Wang, Jianyuan; Xiong, Xihuan; Sun, Jiaming

    2016-10-01

    A lateral p-Si0.05Ge0.95/i-Ge/n-Si0.05Ge0.95 heterojunction light emitting diode on a silicon-on-insulator (SOI) substrate was proposed, which is profitable to achieve higher luminous extraction compared to vertical junctions. Due to the high carrier injection ratio of heterostructures and optical reflection at the SiO2/Si interface of the SOI, strong room temperature electroluminescence (EL) at around 1600 nm from the direct bandgap of i-Ge with 0.30% tensile strain was observed. The EL peak intensity of the lateral heterojunction is enhanced by ˜4 folds with a larger peak energy than that of the vertical Ge p-i-n homojunction, suggesting that the light emitting efficiency of the lateral heterojunction is effectively improved. The EL peak intensity of the lateral heterojunction, which increases quadratically with injection current density, becomes stronger for diodes with a wider i-Ge region. The CMOS compatible fabrication process of the lateral heterojunctions paves the way for the integration of the light source with the Ge metal-oxide-semiconductor field-effect-transistor.

  9. On the output factor measurements of the CyberKnife iris collimator small fields: Experimental determination of the k{sub Q{sub c{sub l{sub i{sub n,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub i}{sub n},f{sub m}{sub s}{sub r}}}}}}}}} correction factors for microchamber and diode detectors

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Pantelis, E.; Moutsatsos, A.; Zourari, K.

    Purpose: To measure the output factors (OFs) of the small fields formed by the variable aperture collimator system (iris) of a CyberKnife (CK) robotic radiosurgery system, and determine the k{sub Q{sub c{sub l{sub i{sub n,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub i}{sub n},f{sub m}{sub s}{sub r}}}}}}}}} correction factors for a microchamber and four diode detectors. Methods: OF measurements were performed using a PTW PinPoint 31014 microchamber, four diode detectors (PTW-60017, -60012, -60008, and the SunNuclear EDGE detector), TLD-100 microcubes, alanine dosimeters, EBT films, and polymer gels for the 5 mm, 7.5 mm, 10 mm, 12.5 mm, and 15 mm irismore » collimators at 650 mm, 800 mm, and 1000 mm source to detector distance (SDD). The alanine OF measurements were corrected for volume averaging effects using the 3D dose distributions registered in polymer gel dosimeters. k{sub Q{sub c{sub l{sub i{sub n,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub i}{sub n},f{sub m}{sub s}{sub r}}}}}}}}} correction factors for the PinPoint microchamber and the diode dosimeters were calculated through comparison against corresponding polymer gel, EBT, alanine, and TLD results. Results: Experimental OF results are presented for the array of dosimetric systems used. The PinPoint microchamber was found to underestimate small field OFs, and a k{sub Q{sub c{sub l{sub i{sub n,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub i}{sub n},f{sub m}{sub s}{sub r}}}}}}}}} correction factor ranging from 1.127 {+-} 0.022 (for the 5 mm iris collimator) to 1.004 {+-} 0.010 (for the 15 mm iris collimator) was determined at the reference SDD of 800 mm. The PinPoint k{sub Q{sub c{sub l{sub i{sub n,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub i}{sub n},f{sub m}{sub s}{sub r}}}}}}}}} correction factor was also found to increase with decreasing SDD; k{sub Q{sub c{sub l{sub i{sub n,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub i}{sub n},f{sub m}{sub s}{sub r}}}}}}}}} values equal to 1.220 {+-} 0.028 and 1

  10. p - n junction diodes fabricated from isolated electrospun fibers of (P(NDI2ODT2)) and an inorganic p-doped semiconductor

    NASA Astrophysics Data System (ADS)

    Rosado, Alexander; Pinto, Nicholas

    2013-03-01

    A simple method to fabricate, under ambient conditions and within seconds, p - n diodes using an individual electrospun poly{[N, N'-bis(2-octyldodecyl)-naphthalene-1,4,5,8-bis(dicarboximide)-2,6-diyl]-alt-5,5'-(2,2'-bithiophene)}-(P(NDI2ODT2)) fiber and a commercially available p-doped Si/SiO2 substrate is presented. Band bending at the fiber/Si+ interface leads to asymmetric I-V characteristic curves resembling that of a diode. The diode turn-on voltage was in the range 1V and was unaffected via UV light irradiation. The rectification ratio however could be tuned reversibly thereby making this device multifunctional. In addition to being a rectifier, the advantage of our design is the complete exposure of the rectifying junction to the surrounding environment. This has the advantage of making them attractive candidates in the potential fabrication of low power, sensitive and rapid response photo-sensors. NSF

  11. Analysis of different forward current-voltage behaviours of Al implanted 4H-SiC vertical p-i-n diodes

    NASA Astrophysics Data System (ADS)

    Megherbi, M. L.; Pezzimenti, F.; Dehimi, L.; Rao, S.; Della Corte, F. G.

    2015-07-01

    In this work different experimental current-voltage behaviours of several Al implanted 4H-SiC p-i-n diodes are investigated by means of numerical simulations in a wide range of currents and temperatures. Some devices for which recombination and tunneling are the dominant current processes at all biases are classified as "leaky" diodes. The well behaved diodes, instead, show good rectifying characteristics with a current conduction due to tunneling below 1.7 V, recombination between 1.7 V and 2.5 V, and diffusion processes above 2.5 V. At higher current regimes, a series resistance in excess of 1 mΩ cm2 becomes the main current limiting factor. Depending on the relative weight between the contact resistances and the internal diode resistance, different temperature dependencies of the current are obtained. A good agreement between numerical and measured data is achieved employing temperature-dependent carrier lifetime and mobility as fitting parameters.

  12. Edge-emitting ultraviolet n-ZnO:Al/i-ZnO/p-GaN heterojunction light-emitting diode with a rib waveguide.

    PubMed

    Liang, H K; Yu, S F; Yang, H Y

    2010-02-15

    An edge-emitting ultraviolet n-ZnO:Al/i-ZnO/p-GaN heterojunction light-emitting diode with a rib waveguide is fabricated by filtered cathodic vacuum arc technique at low deposition temperature (approximately 150 degrees C). Electroluminescence with emission peak at 387 nm is observed. Good correlation between electro- and photo- luminescence spectra suggests that the i-ZnO layer of the heterojunction supports radiative excitonic recombination. Furthermore, it is found that the emission intensity can be enhanced by approximately 5 times due to the presence of the rib waveguide. Only fundamental TE and TM polarizations are supported inside the rib waveguide and the intensity of TE polarization is approximately 2.2 time larger than that of TM polarization.

  13. The underlying micro-mechanism of performance enhancement of non-polar n-ZnO/p-AlGaN ultraviolet light emitting diode with i-ZnO inserted layer

    NASA Astrophysics Data System (ADS)

    Jiang, Fan; Chen, Jingwen; Bi, Han; Li, Luying; Jing, Wenkui; Zhang, Jun; Dai, Jiangnan; Che, Renchao; Chen, Changqing; Gao, Yihua

    2018-01-01

    Non-polar a-plane n-ZnO/p-AlGaN and n-ZnO/i-ZnO/p-AlGaN heterojunction film light-emitting diodes (LEDs) are fabricated with good crystalline quality. The optical measurements show obvious performance enhancement with i-ZnO layer insertion. Off-axis electron holography reveals a potential drop of ˜1.5 V across the heterojunctions with typical p-n junction characteristics. It is found that the electrostatic potentials are inclined and the corresponding electrostatic fields are opposite to each other in n-ZnO and p-AlGaN regions. The electrostatic fields are mainly attributed to strain induced piezoelectric polarizations. After an insertion of an i-ZnO layer into the p-n heterojunction, comparatively flat electrostatic potential generates in the intrinsic ZnO region and contributes to faster movements of the injected electrons and holes, making the i-ZnO layer more conductive to the radiative recombination with enhanced exciton recombination possibilities and at last the LED performance enhancement.

  14. Photon detector configured to employ the Gunn effect and method of use

    DOEpatents

    Cich, Michael J

    2015-03-17

    Embodiments disclosed herein relate to photon detectors configured to employ the Gunn effect for detecting high-energy photons (e.g., x-rays and gamma rays) and methods of use. In an embodiment, a photon detector for detecting high-energy photons is disclosed. The photon detector includes a p-i-n semiconductor diode having a p-type semiconductor region, an n-type semiconductor region, and a compensated i-region disposed between the p-type semiconductor region and the n-type semiconductor region. The compensated i-region and has a width of about 100 .mu.m to about 400 .mu.m and is configured to exhibit the Gunn effect when the p-i-n semiconductor diode is forward biased a sufficient amount. The compensated i-region is doped to include a free carrier concentration of less than about 10.sup.10 cm.sup.-3.

  15. n-ZnO/p-GaN heterojunction light-emitting diodes featuring a buried polarization-induced tunneling junction

    NASA Astrophysics Data System (ADS)

    Li, Ling; Zhang, Yuantao; Yan, Long; Jiang, Junyan; Han, Xu; Deng, Gaoqiang; Chi, Chen; Song, Junfeng

    2016-12-01

    n-ZnO/p-GaN heterojunction light-emitting diodes with a p-GaN/Al0.1Ga0.9N/n+-GaN polarization-induced tunneling junction (PITJ) were fabricated by metal-organic chemical vapor deposition. An intense and sharp ultraviolet emission centered at ˜396 nm was observed under forward bias. Compared with the n-ZnO/p-GaN reference diode without PITJ, the light intensity of the proposed diode is increased by ˜1.4-folds due to the improved current spreading. More importantly, the studied diode operates continuously for eight hours with the decay of only ˜3.5% under 20 mA, suggesting a remarkable operating stability. The results demonstrate the feasibility of using PITJ as hole injection layer for high-performance ZnO-based light-emitting devices.

  16. Temperature dependent characterization of gallium arsenide X-ray mesa p-i-n photodiodes

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Lioliou, G., E-mail: G.Lioliou@sussex.ac.uk; Barnett, A. M.; Meng, X.

    2016-03-28

    Electrical characterization of two GaAs p{sup +}-i-n{sup +} mesa X-ray photodiodes over the temperature range 0 °C to 120 °C together with characterization of one of the diodes as an X-ray detector over the temperature range 0 °C to 60 °C is reported as part of the development of photon counting X-ray spectroscopic systems for harsh environments. The randomly selected diodes were fully etched and unpassivated. The diodes were 200 μm in diameter and had 7 μm thick i layers. The leakage current density was found to increase from (3 ± 1) nA/cm{sup −2} at 0 °C to (24.36 ± 0.05) μA/cm{sup −2} at 120 °C for D1 and from a current density smallermore » than the uncertainty (0.2 ± 1.2) nA/cm{sup −2} at 0 °C to (9.39 ± 0.02) μA/cm{sup −2} at 120 °C for D2 at the maximum investigated reverse bias (15 V). The best energy resolution (FWHM at 5.9 keV) was achieved at 5 V reverse bias, at each temperature; 730 eV at 0 °C, 750 eV at 20 °C, 770 eV at 40 °C, and 840 eV at 60 °C. It was found that the parallel white noise was the main source of the photopeak broadening only when the detector operated at 60 °C, at 5 V, 10 V, and 15 V reverse bias and at long shaping times (>5 μs), whereas the sum of the dielectric noise and charge trapping noise was the dominant source of noise for all the other spectra.« less

  17. Direct formation of InN-codoped p-ZnO/n-GaN heterojunction diode by solgel spin-coating scheme.

    PubMed

    Huang, Chun-Ying; Lee, Ya-Ju; Lin, Tai-Yuan; Chang, Shao-Lun; Lian, Jan-Tian; Lin, Hsiu-Mei; Chen, Nie-Chuan; Yang, Ying-Jay

    2014-02-15

    In this work p-ZnO/n-GaN heterojunction diodes were directly formed on the Si substrate by a combination of cost-effective solgel spin-coating and thermal annealing treatment. Spin-coated n-ZnO films on InN/GaN/Si wafers were converted to p-type polarity after thermal treatment of proper annealing durations. X-ray diffraction (XRD) analysis reveals that InN-codoped ZnO films have grown as the standard hexagonal wurtzite structure with a preferential orientation in the (002) direction. The intensity of the (002) peak decreases for a further extended annealing duration, indicating the greater incorporation of dopants, also confirmed by x-ray photoelectron spectroscopy and low-temperature photoluminescence. Hall and resistivity measurements validate that our p-type ZnO film has a high carrier concentration of 3.73×10¹⁷ cm⁻³, a high mobility of 210 cm²/Vs, and a low resistivity of 0.079 Ωcm. As a result, the proposed p-ZnO/n-GaN heterojunction diode displays a well-behaving current rectification of a typical p-n junction, and the measured current versus voltage (I-V) characteristic is hence well described by the modified Shockley equation. The research on the fabrication of p-ZnO/n-GaN heterojunctions shown here generates useful advances in the production of cost-effective ZnO-based optoelectronic devices.

  18. Zn doping induced conductivity transformation in NiO films for realization of p-n homo junction diode

    NASA Astrophysics Data System (ADS)

    Dewan, Sheetal; Tomar, Monika; Tandon, R. P.; Gupta, Vinay

    2017-06-01

    Mixed transition metal oxide, zinc doped NiO, Z n x N i 1 - x O (x = 0, 0.01, 0.02, 0.05, and 0.10), thin films have been fabricated by the RF magnetron sputtering technique in an oxygen deficit ambience at a growth temperature of 400 °C. The present report highlights the effect of Zn doping in NiO thin films on its structural, optical, and electrical properties. Optical transmission enhancement and band gap engineering in a-axis oriented NiO films have been demonstrated via Zn substitution. Hall effect measurements of the prepared samples revealed a transition from p-type to n-type conductivity in NiO at 2% Zn doping. A NiO based transparent p-n homojunction diode has been fabricated successfully, and the conduction mechanism dominating the diode properties is reported in detail. Current-voltage (I-V) characteristics of the homojunction diode are found to obey the Space Charge Limited Conduction mechanism with non-ideal square law behaviour.

  19. Adiabatic wavelength redshift by dynamic carrier depletion using p -i -n -diode-loaded photonic crystal waveguides

    NASA Astrophysics Data System (ADS)

    Kondo, K.; Baba, T.

    2018-03-01

    We demonstrate an adiabatic wavelength redshift using dynamic carrier depletion. Free carriers are first induced through two-photon absorption of a control pulse and then extracted by a reverse-biased p-i-n diode formed on a Si photonic crystal waveguide, resulting in rapid carrier depletion. A copropagating signal pulse is redshifted by the consequent increase in refractive index. We experimentally evaluated the dynamics of the carrier depletion by the pump-probe method and explored suitable conditions for adiabatic redshift. The signal's redshift was observed, and was confirmed to originate in the dynamic carrier depletion. The redshift was experimentally determined as 0.21 nm.

  20. Vertically p-n-junctioned GaN nano-wire array diode fabricated on Si(111) using MOCVD.

    PubMed

    Park, Ji-Hyeon; Kim, Min-Hee; Kissinger, Suthan; Lee, Cheul-Ro

    2013-04-07

    We demonstrate the fabrication of n-GaN:Si/p-GaN:Mg nanowire arrays on (111) silicon substrate by metal organic chemical vapor deposition (MOCVD) method .The nanowires were grown by a newly developed two-step growth process. The diameter of as-grown nanowires ranges from 300-400 nm with a density of 6-7 × 10(7) cm(-2). The p- and n-type doping of the nanowires is achieved with Mg and Si dopant species. Structural characterization by X-ray diffraction (XRD) and high-resolution transmission electron microscopy (HRTEM) indicates that the nanowires are relatively defect-free. The room-temperature photoluminescence emission with a strong peak at 370 nm indicates that the n-GaN:Si/p-GaN:Mg nanowire arrays have potential application in light-emitting nanodevices. The cathodoluminscence (CL) spectrum clearly shows a distinct optical transition of GaN nanodiodes. The nano-n-GaN:Si/p-GaN:Mg diodes were further completed using a sputter coating approach to deposit Au/Ni metal contacts. The polysilazane filler has been etched by a wet chemical etching process. The n-GaN:Si/p-GaN:Mg nanowire diode was fabricated for different Mg source flow rates. The current-voltage (I-V) measurements reveal excellent rectifying properties with an obvious turn-on voltage at 1.6 V for a Mg flow rate of 5 sccm (standard cubic centimeters per minute).

  1. Vertically p-n-junctioned GaN nano-wire array diode fabricated on Si(111) using MOCVD

    NASA Astrophysics Data System (ADS)

    Park, Ji-Hyeon; Kim, Min-Hee; Kissinger, Suthan; Lee, Cheul-Ro

    2013-03-01

    We demonstrate the fabrication of n-GaN:Si/p-GaN:Mg nanowire arrays on (111) silicon substrate by metal organic chemical vapor deposition (MOCVD) method .The nanowires were grown by a newly developed two-step growth process. The diameter of as-grown nanowires ranges from 300-400 nm with a density of 6-7 × 107 cm-2. The p- and n-type doping of the nanowires is achieved with Mg and Si dopant species. Structural characterization by X-ray diffraction (XRD) and high-resolution transmission electron microscopy (HRTEM) indicates that the nanowires are relatively defect-free. The room-temperature photoluminescence emission with a strong peak at 370 nm indicates that the n-GaN:Si/p-GaN:Mg nanowire arrays have potential application in light-emitting nanodevices. The cathodoluminscence (CL) spectrum clearly shows a distinct optical transition of GaN nanodiodes. The nano-n-GaN:Si/p-GaN:Mg diodes were further completed using a sputter coating approach to deposit Au/Ni metal contacts. The polysilazane filler has been etched by a wet chemical etching process. The n-GaN:Si/p-GaN:Mg nanowire diode was fabricated for different Mg source flow rates. The current-voltage (I-V) measurements reveal excellent rectifying properties with an obvious turn-on voltage at 1.6 V for a Mg flow rate of 5 sccm (standard cubic centimeters per minute).

  2. Gate-tunable carbon nanotube-MoS2 heterojunction p-n diode.

    PubMed

    Jariwala, Deep; Sangwan, Vinod K; Wu, Chung-Chiang; Prabhumirashi, Pradyumna L; Geier, Michael L; Marks, Tobin J; Lauhon, Lincoln J; Hersam, Mark C

    2013-11-05

    The p-n junction diode and field-effect transistor are the two most ubiquitous building blocks of modern electronics and optoelectronics. In recent years, the emergence of reduced dimensionality materials has suggested that these components can be scaled down to atomic thicknesses. Although high-performance field-effect devices have been achieved from monolayered materials and their heterostructures, a p-n heterojunction diode derived from ultrathin materials is notably absent and constrains the fabrication of complex electronic and optoelectronic circuits. Here we demonstrate a gate-tunable p-n heterojunction diode using semiconducting single-walled carbon nanotubes (SWCNTs) and single-layer molybdenum disulfide as p-type and n-type semiconductors, respectively. The vertical stacking of these two direct band gap semiconductors forms a heterojunction with electrical characteristics that can be tuned with an applied gate bias to achieve a wide range of charge transport behavior ranging from insulating to rectifying with forward-to-reverse bias current ratios exceeding 10(4). This heterojunction diode also responds strongly to optical irradiation with an external quantum efficiency of 25% and fast photoresponse <15 μs. Because SWCNTs have a diverse range of electrical properties as a function of chirality and an increasing number of atomically thin 2D nanomaterials are being isolated, the gate-tunable p-n heterojunction concept presented here should be widely generalizable to realize diverse ultrathin, high-performance electronics and optoelectronics.

  3. Gate-tunable carbon nanotube–MoS2 heterojunction p-n diode

    PubMed Central

    Jariwala, Deep; Sangwan, Vinod K.; Wu, Chung-Chiang; Prabhumirashi, Pradyumna L.; Geier, Michael L.; Marks, Tobin J.; Lauhon, Lincoln J.; Hersam, Mark C.

    2013-01-01

    The p-n junction diode and field-effect transistor are the two most ubiquitous building blocks of modern electronics and optoelectronics. In recent years, the emergence of reduced dimensionality materials has suggested that these components can be scaled down to atomic thicknesses. Although high-performance field-effect devices have been achieved from monolayered materials and their heterostructures, a p-n heterojunction diode derived from ultrathin materials is notably absent and constrains the fabrication of complex electronic and optoelectronic circuits. Here we demonstrate a gate-tunable p-n heterojunction diode using semiconducting single-walled carbon nanotubes (SWCNTs) and single-layer molybdenum disulfide as p-type and n-type semiconductors, respectively. The vertical stacking of these two direct band gap semiconductors forms a heterojunction with electrical characteristics that can be tuned with an applied gate bias to achieve a wide range of charge transport behavior ranging from insulating to rectifying with forward-to-reverse bias current ratios exceeding 104. This heterojunction diode also responds strongly to optical irradiation with an external quantum efficiency of 25% and fast photoresponse <15 μs. Because SWCNTs have a diverse range of electrical properties as a function of chirality and an increasing number of atomically thin 2D nanomaterials are being isolated, the gate-tunable p-n heterojunction concept presented here should be widely generalizable to realize diverse ultrathin, high-performance electronics and optoelectronics. PMID:24145425

  4. Transparent CH{sub 3}NH{sub 3}SnCl{sub 3}/Al-ZnO p-n heterojunction diode

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Kumar, Sunil, E-mail: skbgudha@gmail.com; Ansari, Mohd Zubair; Khare, Neeraj

    2016-05-23

    A p-type Organic inorganic tin chloride (CH{sub 3}NH{sub 3}SnCl{sub 3}) perovskite thin film has been synthesized by solution method. An n-type 1% Al doped ZnO (AZO) film has been deposited on FTO substrate by ultrasonic assisted chemical vapor deposition technique. A transparent CH{sub 3}NH{sub 3}SnCl{sub 3}/AZO p-n heterojunction diode has been fabricated by spin coating technique. CH{sub 3}NH{sub 3}SnCl{sub 3}/AZO p-n heterojunction shows 75% transparency in the visible region. I-V characteristic of CH{sub 3}NH{sub 3}SnCl{sub 3}/AZO p-n heterojunction shows rectifying behavior of the diode. The diode parameters calculated as ideality factor η=2.754 and barrier height Φ= 0.76 eV. The resultmore » demonstrates the potentiality of CH{sub 3}NH{sub 3}SnCl{sub 3}/AZO p-n heterojunction for transparent electronics.« less

  5. Modification of electrical properties of Au/n-type InP Schottky diode with a high-k Ba0.6Sr0.4TiO3 interlayer

    NASA Astrophysics Data System (ADS)

    Thapaswini, P. Prabhu; Padma, R.; Balaram, N.; Bindu, B.; Rajagopal Reddy, V.

    2016-05-01

    Au/Ba0.6Sr0.4TiO3 (BST)/n-InP metal/insulator/semiconductor (MIS) Schottky diodes have been analyzed by current-voltage (I-V) and capacitance-voltage (C-V) measurements. The surface morphology of the BST films on InP is fairly smooth. The Au/BST/n-InP MIS Schottky diode shows better rectification ratio and low leakage current compared to the conventional Au/n-InP metal-semiconductor (MS) Schottky diode. Higher barrier height is achieved for the MIS Schottky diode compared to the MS Schottky diode. The Norde and Cheung's methods are employed to determine the barrier height, ideality factor and series resistance. The interface state density (NSS) is determined from the forward bias I-V data for both the MS and MIS Schottky diodes. Results reveal that the NSS of the MIS Schottky diode is lower than that of the MS Schottky diode. The Poole-Frenkel emission is found dominating the reverse current in both Au/n-InP MS and Au/BST/n-InP MIS Schottky diodes, indicating the presence of structural defects and trap levels in the dielectric film.

  6. Fabrication and characterization of n-ZnO nanonails array/p(+)-GaN heterojunction diode.

    PubMed

    Zhu, G Y; Chen, G F; Li, J T; Shi, Z L; Lin, Y; Ding, T; Xu, X Y; Dai, J; Xu, C X

    2012-10-01

    A novel heterojunctional structure of n-ZnO nanonails array/p(+)-GaN light-emitting diode was fabricated by Chemical Vapor Deposition method. A broad electroluminescence spectrum shows two peaks centered at 435 nm and 478 nm at room temperature, respectively. By comparing the photoluminescence and electroluminescence spectra, together with analyzing the energy band structure of heterojunction light emitting diode, it suggested that the electroluminescence peak located at 435 nm originates from Mg acceptor level of p(+)-GaN layer, whereas the electroluminescence peak located at 478 nm originates from the defects of n-ZnO nanonails array.

  7. The millimeter wave super-Schottky diode detector

    NASA Technical Reports Server (NTRS)

    Silver, A. H.; Pedersen, R. J.; Mccoll, M.; Dickman, R. L.; Wilson, W. J.

    1981-01-01

    The 31 and 92 GHz measurements of the superconductor-Schottky diode extended to millimeter wavelengths by a redesign of the semiconductor interface are reported. Diodes were fabricated by pulse electroplating Pb on 2 x 10 to the 19th/cu cm p-Ga-As etched with HCl; a thin Au overplate is deposited to protect the Pb film from degradation and to improve its lifetime. The noise performance was almost ideal at 31 and 92 GHz; it was concluded that this diode is a quantum-limited-detector at 31 GHz, with excessive parasitic losses at 92 GHz.

  8. Origin analysis of expanded stacking faults by applying forward current to 4H-SiC p-i-n diodes

    NASA Astrophysics Data System (ADS)

    Hayashi, Shohei; Naijo, Takanori; Yamashita, Tamotsu; Miyazato, Masaki; Ryo, Mina; Fujisawa, Hiroyuki; Miyajima, Masaaki; Senzaki, Junji; Kato, Tomohisa; Yonezawa, Yoshiyuki; Kojima, Kazutoshi; Okumura, Hajime

    2017-08-01

    Stacking faults expanded by the application of forward current to 4H-SiC p-i-n diodes were observed using a transmission electron microscope to investigate the expansion origin. It was experimentally confirmed that long-zonal-shaped stacking faults expanded from basal-plane dislocations converted into threading edge dislocations. In addition, stacking fault expansion clearly penetrated into the substrate to a greater depth than the dislocation conversion point. This downward expansion of stacking faults strongly depends on the degree of high-density minority carrier injection.

  9. Improved InGaN/GaN light-emitting diodes with a p-GaN/n-GaN/p-GaN/n-GaN/p-GaN current-spreading layer.

    PubMed

    Zhang, Zi-Hui; Tan, Swee Tiam; Liu, Wei; Ju, Zhengang; Zheng, Ke; Kyaw, Zabu; Ji, Yun; Hasanov, Namig; Sun, Xiao Wei; Demir, Hilmi Volkan

    2013-02-25

    This work reports both experimental and theoretical studies on the InGaN/GaN light-emitting diodes (LEDs) with optical output power and external quantum efficiency (EQE) levels substantially enhanced by incorporating p-GaN/n-GaN/p-GaN/n-GaN/p-GaN (PNPNP-GaN) current spreading layers in p-GaN. Each thin n-GaN layer sandwiched in the PNPNP-GaN structure is completely depleted due to the built-in electric field in the PNPNP-GaN junctions, and the ionized donors in these n-GaN layers serve as the hole spreaders. As a result, the electrical performance of the proposed device is improved and the optical output power and EQE are enhanced.

  10. Polarization-enhanced InGaN/GaN-based hybrid tunnel junction contacts to GaN p-n diodes and InGaN LEDs

    NASA Astrophysics Data System (ADS)

    Mughal, Asad J.; Young, Erin C.; Alhassan, Abdullah I.; Back, Joonho; Nakamura, Shuji; Speck, James S.; DenBaars, Steven P.

    2017-12-01

    Improved turn-on voltages and reduced series resistances were realized by depositing highly Si-doped n-type GaN using molecular beam epitaxy on polarization-enhanced p-type InGaN contact layers grown using metal-organic chemical vapor deposition. We compared the effects of different Si doping concentrations and the addition of p-type InGaN on the forward voltages of p-n diodes and light-emitting diodes, and found that increasing the Si concentrations from 1.9 × 1020 to 4.6 × 1020 cm-3 and including a highly doped p-type InGaN at the junction both contributed to reductions in the depletion width, the series resistance of 4.2 × 10-3-3.4 × 10-3 Ω·cm2, and the turn-on voltages of the diodes.

  11. Characterization of gallium arsenide X-ray mesa p-i-n photodiodes at room temperature

    NASA Astrophysics Data System (ADS)

    Lioliou, G.; Meng, X.; Ng, J. S.; Barnett, A. M.

    2016-03-01

    Two GaAs mesa p+-i-n+ photodiodes intended for photon counting X-ray spectroscopy, having an i layer thickness of 7 μm and diameter of 200 μm, have been characterized electrically, for their responsivity at the wavelength range 580 nm to 980 nm and one of them for its performance at detection of soft X-rays, at room temperature. Dark current and capacitance measurements as a function of applied forward and reverse bias are presented. The results show low leakage current densities, in the range of nA/cm2 at the maximum internal electric field (22 kV/cm). The unintentional doping concentration of the i layer, calculated from capacitance measurements, was found to be <1014 cm-3. Photocurrent measurements were performed under visible and near infrared light illumination for both diodes. The analysis of these measurements suggests the presence of a non-active (dead) layer (0.16 μm thickness) at the p+ side top contact interface, where the photogenerated carriers do not contribute to the photocurrent, possibly due to recombination. One of the diodes, D1, was also characterized as detector for room temperature photon counting X-ray spectroscopy; the best energy resolution achieved (FWHM) at 5.9 keV was 745 eV. The noise analysis of the system, based on spectra obtained at different shaping times and applied reverse biases, showed that the dominant source of noise is the dielectric noise. It was also calculated that there was at least (165±24) eV charge trapping noise at 0 V.

  12. 5.0 kV breakdown-voltage vertical GaN p-n junction diodes

    NASA Astrophysics Data System (ADS)

    Ohta, Hiroshi; Hayashi, Kentaro; Horikiri, Fumimasa; Yoshino, Michitaka; Nakamura, Tohru; Mishima, Tomoyoshi

    2018-04-01

    A high breakdown voltage of 5.0 kV has been achieved for the first time in vertical GaN p-n junction diodes by using our newly developed guard-ring structures. A resistance device was inserted between the main diode portion and the guard-ring portion in a ring-shaped p-n diode to generate a voltage drop over the resistance device by leakage current flowing through the guard-ring portion under negatively biased conditions before breakdown. The voltage at the outer mesa edge of the guard-ring portion, where the electric field intensity is highest and the destructive breakdown usually occurs, is decreased by the voltage drop, so the electric field concentration in the portion is reduced. By adopting this structure, the breakdown voltage (V B) is raised by about 200 V. Combined with a low measured on-resistance (R on) of 1.25 mΩ cm2, Baliga’s figure of merit (V\\text{B}2/R\\text{on}) was as high as 20 GW/cm2.

  13. High breakdown single-crystal GaN p-n diodes by molecular beam epitaxy

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Qi, Meng; Zhao, Yuning; Yan, Xiaodong

    2015-12-07

    Molecular beam epitaxy grown GaN p-n vertical diodes are demonstrated on single-crystal GaN substrates. A low leakage current <3 nA/cm{sup 2} is obtained with reverse bias voltage up to −20 V. With a 400 nm thick n-drift region, an on-resistance of 0.23 mΩ cm{sup 2} is achieved, with a breakdown voltage corresponding to a peak electric field of ∼3.1 MV/cm in GaN. Single-crystal GaN substrates with very low dislocation densities enable the low leakage current and the high breakdown field in the diodes, showing significant potential for MBE growth to attain near-intrinsic performance when the density of dislocations is low.

  14. Dual-Gated MoTe2/MoS2 van der Waals Heterojunction p-n Diode

    NASA Astrophysics Data System (ADS)

    Rai, Amritesh; Movva, Hema C. P.; Kang, Sangwoo; Larentis, Stefano; Roy, Anupam; Tutuc, Emanuel; Banerjee, Sanjay K.

    2D materials are promising for future electronic and optoelectronic applications. In this regard, it is important to realize p-n diodes, the most fundamental building block of all modern semiconductor devices, based on these 2D materials. While it is challenging to achieve homojunction diodes in 2D semiconductors due to lack of reliable selective doping techniques, it is relatively easier to achieve diode-like behavior in van der Waals (vdW) heterostructures comprising different 2D semiconductors. Here, we demonstrate dual-gated vdW heterojunction p-n diodes based on p-type MoTe2 and n-type MoS2, with hBN as the top and bottom gate dielectric. The heterostructure stack is assembled using a polymer-based `dry-transfer' technique. Pt contact is used for hole injection in MoTe2, whereas Ag is used for electron injection in MoS2. The dual-gates allow for independent electrostatic tuning of the carriers in MoTe2 and MoS2. Room temperature interlayer current-voltage characteristics reveal a strong gate-tunable rectification behavior. At low temperatures, the diode turn-on voltage increases, whereas the reverse saturation current decreases, in accordance with conventional p-n diode behavior. Dual-Gated MoTe2/MoS2 van der Waals Heterojunction p-n Diode.

  15. Performance analyses of Schottky diodes with Au/Pd contacts on n-ZnO thin films as UV detectors

    NASA Astrophysics Data System (ADS)

    Varma, Tarun; Periasamy, C.; Boolchandani, Dharmendar

    2017-12-01

    In this paper, we report fabrication and performance analyses of UV detectors based on ZnO thin film Schottky diodes with Au and Pd contacts. RF magnetron sputtering technique has been used to deposit the nano-crystalline ZnO thin film, at room temperature. Characterization techniques such as XRD, AFM and SEM provided valuable information related to the micro-structural & optical properties of the thin film. The results show that the prepared thin film has good crystalline orientation and minimal surface roughness, with an optical bandgap of 3.1 eV. I-V and C-V characteristics were evaluated that indicate non-linear behaviour of the diodes with rectification ratios (IF/IR) of 19 and 427, at ± 4 V, for Au/ZnO and Pd/ZnO Schottky diodes, respectively. The fabricated Schottky diodes when exposed to a UV light of 365 nm wavelength, at an applied bias of -2 V, exhibited responsivity of 10.16 and 22.7 A/W, for Au and Pd Schottky contacts, respectively. The Pd based Schottky photo-detectors were found to exhibit better performance with superior values of detectivity and photoconductive gain of 1.95 × 1010 cm Hz0.5/W & 77.18, over those obtained for the Au based detectors which were observed to be 1.23 × 1010 cm Hz0.5/W & 34.5, respectively.

  16. Fully porous GaN p-n junction diodes fabricated by chemical vapor deposition.

    PubMed

    Bilousov, Oleksandr V; Carvajal, Joan J; Geaney, Hugh; Zubialevich, Vitaly Z; Parbrook, Peter J; Martínez, Oscar; Jiménez, Juan; Díaz, Francesc; Aguiló, Magdalena; O'Dwyer, Colm

    2014-10-22

    Porous GaN based LEDs produced by corrosion etching techniques demonstrated enhanced light extraction efficiency in the past. However, these fabrication techniques require further postgrown processing steps, which increases the price of the final system. Also, the penetration depth of these etching techniques is limited, and affects not only the semiconductor but also the other elements constituting the LED when applied to the final device. In this paper, we present the fabrication of fully porous GaN p-n junctions directly during growth, using a sequential chemical vapor deposition (CVD) process to produce the different layers that form the p-n junction. We characterized their diode behavior from room temperature to 673 K and demonstrated their ability as current rectifiers, thus proving the potential of these fully porous p-n junctions for diode and LEDs applications. The electrical and luminescence characterization confirm that high electronic quality porous structures can be obtained by this method, and we believe this investigation can be extended to other III-N materials for the development of white light LEDs, or to reduce reflection losses and narrowing the output light cone for improved LED external quantum efficiencies.

  17. Recent technological developments on LGAD and iLGAD detectors for tracking and timing applications

    NASA Astrophysics Data System (ADS)

    Pellegrini, G.; Baselga, M.; Carulla, M.; Fadeyev, V.; Fernández-Martínez, P.; García, M. Fernández; Flores, D.; Galloway, Z.; Gallrapp, C.; Hidalgo, S.; Liang, Z.; Merlos, A.; Moll, M.; Quirion, D.; Sadrozinski, H.; Stricker, M.; Vila, I.

    2016-09-01

    This paper reports the latest technological development on the Low Gain Avalanche Detector (LGAD) and introduces a new architecture of these detectors called inverse-LGAD (iLGAD). Both approaches are based on the standard Avalanche Photo Diodes (APD) concept, commonly used in optical and X-ray detection applications, including an internal multiplication of the charge generated by radiation. The multiplication is inherent to the basic n++-p+-p structure, where the doping profile of the p+ layer is optimized to achieve high field and high impact ionization at the junction. The LGAD structures are optimized for applications such as tracking or timing detectors for high energy physics experiments or medical applications where time resolution lower than 30 ps is required. Detailed TCAD device simulations together with the electrical and charge collection measurements are presented through this work.

  18. Generation of High-Voltage Pulses by Sharp-Recovery SiC Drift Diodes ( n-Base versus p-Base Diodes)

    NASA Astrophysics Data System (ADS)

    Ivanov, P. A.; Grekhov, I. V.

    2018-01-01

    The time characteristics of pulse generators based on sharp-recovery 4 H : SiC drift diodes have been calculated. It has been found that the speed of n-base 4 H-SiC diodes is superior to that of p-base diodes with the amplitude and initial pedestal in the output voltage (<5% of the amplitude) versus the time curve being the same.

  19. Heterojunction p-Cu2O/n-Ga2O3 diode with high breakdown voltage

    NASA Astrophysics Data System (ADS)

    Watahiki, Tatsuro; Yuda, Yohei; Furukawa, Akihiko; Yamamuka, Mikio; Takiguchi, Yuki; Miyajima, Shinsuke

    2017-11-01

    Heterojunction p-Cu2O/n-β-Ga2O3 diodes were fabricated on an epitaxially grown β-Ga2O3(001) layer. The reverse breakdown voltage of these p-n diodes reached 1.49 kV with a specific on-resistance of 8.2 mΩ cm2. The leakage current of the p-n diodes was lower than that of the Schottky barrier diode due to the higher barrier height against the electron. The ideality factor of the p-n diode was 1.31. It indicated that some portion of the recombination current at the interface contributed to the forward current, but the diffusion current was the dominant. The forward current more than 100 A/cm2 indicated the lower conduction band offset at the hetero-interface between Cu2O and Ga2O3 layers than that predicted from the bulk properties, resulting in such a high forward current without limitation. These results open the possibility of advanced device structures for wide bandgap Ga2O3 to achieve higher breakdown voltage and lower on-resistance.

  20. Greatly improved 3C-SiC p-n junction diodes grown by chemical vapor deposition

    NASA Technical Reports Server (NTRS)

    Neudeck, Philip G.; Larkin, David J.; Starr, Jonathan E.; Powell, J. A.; Salupo, Carl S.; Matus, Lawrence G.

    1993-01-01

    This paper reports the fabrication and initial electrical characterization of greatly improved 3C-SiC (beta-SiC) p-n junction diodes. These diodes, which were grown on commercially available 6H-SiC substrates by chemical vapor deposition, demonstrate rectification to -200 V at room temperature, representing a fourfold improvement in reported 3C-SiC diode blocking voltage. The reverse leakage currents and saturation current densities measured on these diodes also show significant improvement compared to previously reported 3C-SiC p-n junction diodes. When placed under sufficient forward bias, the diodes emit significantly bright green-yellow light. These results should lead to substantial advancements in 3C-SiC transistor performance.

  1. Titanium-dioxide nanotube p-n homojunction diode

    NASA Astrophysics Data System (ADS)

    Alivov, Yahya; Ding, Yuchen; Singh, Vivek; Nagpal, Prashant

    2014-12-01

    Application of semiconductors in functional optoelectronic devices requires precise control over their doping and formation of junction between p- and n-doped semiconductors. While doped thin films have led to several semiconductor devices, need for high-surface area nanostructured devices for photovoltaic, photoelectrochemical, and photocatalytic applications has been hindered by lack of desired doping in nanostructures. Here, we show titanium-dioxide (TiO2) nanotubes doped with nitrogen (N) and niobium (Nb) as acceptors and donors, respectively, and formation of TiO2 nanotubes p-n homojunction. This TiO2:N/TiO2:Nb homojunction showed distinct diode-like behaviour with rectification ratio of 1115 at ±5 V and exhibited good photoresponse for ultraviolet light (λ = 365 nm) with sensitivity of 0.19 A/W at reverse bias of -5 V. These results can have important implications for development of nanostructured metal-oxide solar-cells, photodiodes, LED's, photocatalysts, and photoelectrochemical devices.

  2. Electrical and optical characteristics of n-Zno/p-GaN hetero-junction diode fabricated by ultra-high vacuum sputter.

    PubMed

    Cho, Seong Gook; Lee, Dong Uk; Kim, Eun Kyu

    2013-09-01

    We investigated the electrical and optical properties of n-ZnO/p-GaN hetero-junction diode fabricated by an ultra-high vacuum radio frequency magnetron sputter. A physical relationship between the rotation rate during deposition process and post annealing conditions after deposited ZnO layer on p-GaN layer was discussed. When the rotation rates during deposition process of n-ZnO layer were 5 rpm and 15 rpm, the full width at half maximum of photoluminescence spectra of ZnO layer on the p-GaN layer was about 106 and 133 meV, respectively. Also, the ratio of deep level emission to near band edge emission was dramatically increased as increasing the rotation rate from 5 to 15 rpm. The n-ZnO/p-GaN hetero-junction diode grown at 5 rpm has a higher ratio of forward to reverse currents than the diode grown at 15 rpm. Also, the 600 degrees C-annealed diodes with 5 rpm showed good rectifying behavior with the barrier height of 0.74 eV, the ideality factor of 12.2, and the forward to reverse current ratio of 614 at +/- 8 V.

  3. Single n-GaN microwire/p-Silicon thin film heterojunction light-emitting diode.

    PubMed

    Ahn, Jaehui; Mastro, Michael A; Klein, Paul B; Hite, Jennifer K; Feigelson, Boris; Eddy, Charles R; Kim, Jihyun

    2011-10-24

    The emission and waveguiding properties of individual GaN microwires as well as devices based on an n-GaN microwire/p-Si (100) junction were studied for relevance in optoelectronics and optical circuits. Pulsed photoluminescence of the GaN microwire excited in the transverse or longitudinal direction demonstrated gain. These n-type GaN microwires were positioned mechanically or by dielectrophoretic force onto pre-patterned electrodes on a p-type Si (100) substrate. Electroluminescence from this p-n point junction was characteristic of a heterostructure light-emitting diode. Additionally, waveguiding was observed along the length of the microwire for light originating from photoluminescence as well as from electroluminescence generated at the p-n junction. © 2011 Optical Society of America

  4. Effects of Be acceptors on the spin polarization of carriers in p-i-n resonant tunneling diodes

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Awan, I. T.; Galvão Gobato, Y.; Galeti, H. V. A.

    In this paper, we have investigated the effect of Be acceptors on the electroluminescence and the spin polarization in GaAs/AlAs p-i-n resonant tunneling diodes. The quantum well emission comprise two main lines separated by ∼20 meV attributed to excitonic and Be-related transitions, which intensities show remarkably abrupt variations at critical voltages, particularly at the electron resonant peak where it shows a high-frequency bistability. The circular-polarization degree of the quantum-well electroluminescence also shows strong and abrupt variations at the critical bias voltages and it attains relatively large values (of ∼−75% at 15 T). These effects may be explored to design novel devices formore » spintronic applications such as a high-frequency spin-oscillators.« less

  5. Deep diode arrays for X-ray detection

    NASA Technical Reports Server (NTRS)

    Zemel, J. N.

    1984-01-01

    Temperature gradient zone melting process was used to form p-n junctions in bulk of high purity silicon wafers. These diodes were patterned to form arrays for X-ray spectrometers. The whole fabrication processes for these X-ray detectors are reviewed in detail. The p-n junctions were evaluated by (1) the dark diode I-V measurements, (2) the diode C sub I - V measurements, and (3) the MOS C-V measurements. The results showed that these junctions were linearly graded in charge distribution with low reverse bias leakage current flowing through them (few nA at -10 volts). The X-ray detection experiments showed that an FWHM of 500 eV was obtained from these diodes with a small bias of just -5 volts (for X-ray source Fe55). A theoretical model was proposed to explain the extra peaks found in the energy spectra and a very interesting point - cross talk effect was pointed out. This might be a solution to the problem of making really high resolution X-ray spectrometers.

  6. n-B-pi-p Superlattice Infrared Detector

    NASA Technical Reports Server (NTRS)

    Ting, David Z.; Bandara, Sumith V.; Hill, Cory J.; Gunapala, Sarath D.

    2011-01-01

    A specially designed barrier (B) is inserted at the n-pi junction [where most GR (generation-recombination) processes take place] in the standard n-pi-p structure to substantially reduce generation-recombination dark currents. The resulting n-Bpi- p structure also has reduced tunneling dark currents, thereby solving some of the limitations to which current type II strained layer superlattice infrared detectors are prone. This innovation is compatible with common read-out integrated circuits (ROICs).

  7. Constant-current regulator improves tunnel diode threshold-detector performance

    NASA Technical Reports Server (NTRS)

    Cancro, C. A.

    1965-01-01

    Grounded-base transistor is placed in a tunnel diode threshold detector circuit, and a bias voltage is applied to the tunnel diode. This provides the threshold detector with maximum voltage output and overload protection.

  8. The Novel Preparation of P-N Junction Mesa Diodes by Silicon-Wafer Direct Bonding (SDB)

    NASA Astrophysics Data System (ADS)

    Yeh, Ching-Fa; Hwangleu, Shyang

    1992-05-01

    The key processes of silicon-wafer direct bonding (SDB), including hydrophilic surface formation and optimal two-step heat treatment, have been developed However, H2SO4/H2O2 solution being a strong oxidized acid solution, native oxide is found to have grown on the wafer surface as soon as a wafer is treated in this solution. In the case of a wafer further treated in diluted HF solution after hydrophilic surface formation, it is shown that the wafer surface can not only be cleaned of its native oxide but also remains hydrophilic, and can provide excellent voidless bonding. The N+/P and N/P combination junction mesa diodes fabricated on the wafers prepared by these novel SDB technologies are examined. The ideality factor n of the N/P mesa diode is 2.4˜2.8 for the voltage range 0.2˜0.3 V; hence, the lowering of the ideality factor n is evidently achieved. As for the N+/P mesa diode, the ideality factor n shows a value of 1.10˜1.30 for the voltage range 0.2˜0.6 V; the low value of n is attributed to an autodoping phenomenon which has caused the junction interface to form in the P-silicon bulk. However, the fact that the sustaining voltage of the N/P mesa diode showed a value greater than 520 V reveals the effectiveness of our novel SDB processes.

  9. Spatial response of synthetic microDiamond and diode detectors measured with kilovoltage synchrotron radiation.

    PubMed

    Butler, Duncan J; Beveridge, Toby; Lehmann, Joerg; Oliver, Christopher P; Stevenson, Andrew W; Livingstone, Jayde

    2018-02-01

    To map the spatial response of four solid-state radiation detectors of types commonly used for radiotherapy dosimetry. PTW model 60016 Diode P, 60017 Diode E, 60018 Diode SRS, and 60019 microDiamond detectors were radiographed using a high resolution conventional X-ray system. Their spatial response was then investigated using a 0.1 mm diameter beam of 95 keV average energy photons generated by a synchrotron. The detectors were scanned through the beam while their signal was recorded as a function of position, to map the response. These 2D response maps were created in both the end-on and side-on orientations. The results show the location and size of the active region. End-on, the active area was determined to be centrally located and within 0.2 mm of the manufacturer's specified diameter. The active areas of the 60016 Diode P, 60017 Diode E, 60018 Diode SRS detectors are uniform to within approximately 5%. The 60019 microDiamond showed local variations up to 30%. The extra-cameral signal in the microDiamond was calculated from the side-on scan to be approximately 8% of the signal from the active element. The spatial response of four solid-state detectors has been measured. The technique yielded information about the location and uniformity of the active area, and the extra-cameral signal, for the beam quality used. © 2017 Commonwealth of Australia. Medical Physics © 2017 American Association of Physicists in Medicine. This work is copyright. Apart from any use as permitted under the Copyright Act 1968, no part may be reproduced without prior written permission. Requests and enquiries concerning reproduction and rights should be directed in the first instance to John Wiley & Sons Ltd of The Atrium, Southern Gate, Chichester, West Sussex P019 8SQ UNITED KINGDOM; alternatively to ARPANSA.

  10. Low absorption loss p-AlGaN superlattice cladding layer for current-injection deep ultraviolet laser diodes

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Martens, M.; Kuhn, C.; Ziffer, E.

    2016-04-11

    Current injection into AlGaN-based laser diode structures with high aluminum mole fractions for deep ultraviolet emission is investigated. The electrical characteristics of laser diode structures with different p-AlGaN short period superlattice (SPSL) cladding layers with various aluminum mole fractions are compared. The heterostructures contain all elements that are needed for a current-injection laser diode including cladding and waveguide layers as well as an AlGaN quantum well active region emitting near 270 nm. We found that with increasing aluminum content in the p-AlGaN cladding, the diode turn-on voltage increases, while the series resistance slightly decreases. By introducing an SPSL instead of bulkmore » layers, the operating voltage is significantly reduced. A gain guided broad area laser diode structure with transparent p-Al{sub 0.70}Ga{sub 0.30}N waveguide layers and a transparent p-cladding with an average aluminum content of 81% was designed for strong confinement of the transverse optical mode and low optical losses. Using an optimized SPSL, this diode could sustain current densities of more than 4.5 kA/cm{sup 2}.« less

  11. Lattice-Matched p-GaAsSb/n-InP Backward Diodes Operating at Zero Bias for Millimeter-Wave Applications

    NASA Astrophysics Data System (ADS)

    Takahashi, Tsuyoshi; Sato, Masaru; Nakasha, Yasuhiro; Hara, Naoki

    2012-09-01

    Backward diodes consisting of a heterojunction of p-GaAs0.51Sb0.49/n-InP, which was lattice matched to an InP substrate, were fabricated for the first time and investigated for their characteristics. The lattice-matched heterojunction is effective in preventing surface defects after crystal growth of the diodes. The backward diodes indicated a curvature coefficient of -17.6 V-1, which is sufficiently large for zero-bias operation. Voltage sensitivity of 338 V/W was obtained at 94 GHz by use of the circular mesa diode of 2.0 µm diameter. Optimum voltage sensitivity of 1603 V/W was estimated when the input impedance was completely matched with the diodes.

  12. Modular multi-element high energy particle detector

    DOEpatents

    Coon, Darryl D.; Elliott, John P.

    1990-01-02

    Multi-element high energy particle detector modules comprise a planar heavy metal carrier of tungsten alloy with planar detector units uniformly distributed over one planar surface. The detector units are secured to the heavy metal carrier by electrically conductive adhesive so that the carrier serves as a common ground. The other surface of each planar detector unit is electrically connected to a feedthrough electrical terminal extending through the carrier for front or rear readout. The feedthrough electrical terminals comprise sockets at one face of the carrier and mating pins porjecting from the other face, so that any number of modules may be plugged together to create a stack of modules of any desired number of radiation lengths. The detector units each comprise four, preferably rectangular, p-i-n diode chips arranged around the associated feedthrough terminal to form a square detector unit providing at least 90% detector element coverage of the carrier. Integral spacers projecting from the carriers extend at least partially along the boundaries between detector units to space the p-i-n diode chips from adjacent carriers in a stack. The spacers along the perimeters of the modules are one-half the width of the interior spacers so that when stacks of modules are arranged side by side to form a large array of any size or shape, distribution of the detector units is uniform over the entire array.

  13. Unveiling the composite structures of emissive consolidated p-i-n junction nanocells for white light emission.

    PubMed

    Lee, Kyu Seung; Shim, Jaeho; Lee, Hyunbok; Yim, Sang-Youp; Angadi, Basavaraj; Lim, Byungkwon; Son, Dong Ick

    2018-06-08

    Hybrid organic-Red-Green-Blue (RGB) color quantum dots were incorporated into consolidated p(polymer)-i(RGB quantum dots)-n(small molecules) junction structures to fabricate a single active layer for a light emitting diode device for white electroluminescence. The semiconductor RGB quantum dots, as an intrinsic material, were electrostatically bonded between functional groups of the p-type polymer organic material core surface and the n-type small molecular organic material shell surface. The ZnCdSe/ZnS and CdSe/ZnS quantum dots distributed uniformly and isotropically surrounding the polymer core which in turn was surrounded by small molecular organic materials. In the present study, we have identified the mechanisms of chemical synthesis and interactions of the p-i-n junction nanocell structure through modeling studies by DFT calculations. We have also investigated optical, structural and electrical properties along with the carrier transport mechanism of the light emitting diodes which have a single active layer of consolidated p-i-n junction nanocells for white electroluminescence.

  14. Room temperature current-voltage (I-V) characteristics of Ag/InGaN/n-Si Schottky barrier diode

    NASA Astrophysics Data System (ADS)

    Erdoğan, Erman; Kundakçı, Mutlu

    2017-02-01

    Metal-semiconductors (MSs) or Schottky barrier diodes (SBDs) have a significant potential in the integrated device technology. In the present paper, electrical characterization of Ag/InGaN/n-Si Schottky diode have been systematically carried out by simple Thermionic method (TE) and Norde function based on the I-V characteristics. Ag ohmic and schottky contacts are deposited on InGaN/n-Si film by thermal evaporation technique under a vacuum pressure of 1×10-5 mbar. Ideality factor, barrier height and series resistance values of this diode are determined from I-V curve. These parameters are calculated by TE and Norde methods and findings are given in a comparetive manner. The results show the consistency for both method and also good agreement with other results obtained in the literature. The value of ideality factor and barrier height have been determined to be 2.84 and 0.78 eV at room temperature using simple TE method. The value of barrier height obtained with Norde method is calculated as 0.79 eV.

  15. Enhancement of breakdown voltage for fully-vertical GaN-on-Si p-n diode by using strained layer superlattice as drift layer

    NASA Astrophysics Data System (ADS)

    Mase, Suguru; Hamada, Takeaki; Freedsman, Joseph J.; Egawa, Takashi

    2018-06-01

    We have demonstrated a vertical GaN-on-Si p-n diode with breakdown voltage (BV) as high as 839 V by using a low Si-doped strained layer superlattice (SLS). The p-n vertical diode fabricated by using the n‑-SLS layer as a part of the drift layer showed a remarkable enhancement in BV, when compared with the conventional n‑-GaN drift layer of similar thickness. The vertical GaN-on-Si p-n diodes with 2.3 μm-thick n‑-GaN drift layer and 3.0 μm-thick n‑-SLS layer exhibited a differential on-resistance of 4.0 Ω · cm2 and a BV of 839 V.

  16. Estimating p-n Diode Bulk Parameters, Bandgap Energy and Absolute Zero by a Simple Experiment

    ERIC Educational Resources Information Center

    Ocaya, R. O.; Dejene, F. B.

    2007-01-01

    This paper presents a straightforward but interesting experimental method for p-n diode characterization. The method differs substantially from many approaches in diode characterization by offering much tighter control over the temperature and current variables. The method allows the determination of important diode constants such as temperature…

  17. Black phosphorus-monolayer MoS2 van der Waals heterojunction p-n diode.

    PubMed

    Deng, Yexin; Luo, Zhe; Conrad, Nathan J; Liu, Han; Gong, Yongji; Najmaei, Sina; Ajayan, Pulickel M; Lou, Jun; Xu, Xianfan; Ye, Peide D

    2014-08-26

    Phosphorene, a elemental 2D material, which is the monolayer of black phosphorus, has been mechanically exfoliated recently. In its bulk form, black phosphorus shows high carrier mobility (∼10,000 cm(2)/V·s) and a ∼0.3 eV direct band gap. Well-behaved p-type field-effect transistors with mobilities of up to 1000 cm(2)/V·s, as well as phototransistors, have been demonstrated on few-layer black phosphorus, showing its promise for electronics and optoelectronics applications due to its high hole mobility and thickness-dependent direct band gap. However, p–n junctions, the basic building blocks of modern electronic and optoelectronic devices, have not yet been realized based on black phosphorus. In this paper, we demonstrate a gate-tunable p–n diode based on a p-type black phosphorus/n-type monolayer MoS2 van der Waals p–n heterojunction. Upon illumination, these ultrathin p–n diodes show a maximum photodetection responsivity of 418 mA/W at the wavelength of 633 nm and photovoltaic energy conversion with an external quantum efficiency of 0.3%. These p–n diodes show promise for broad-band photodetection and solar energy harvesting.

  18. Impact of dislocation densities on n+/p and p+/n junction GaAs diodes and solar cells on SiGe virtual substrates

    NASA Astrophysics Data System (ADS)

    Andre, C. L.; Wilt, D. M.; Pitera, A. J.; Lee, M. L.; Fitzgerald, E. A.; Ringel, S. A.

    2005-07-01

    Recent experimental measurements have shown that in GaAs with elevated threading dislocation densities (TDDs) the electron lifetime is much lower than the hole lifetime [C. L. Andre, J. J. Boeckl, D. M. Wilt, A. J. Pitera, M. L. Lee, E. A. Fitzgerald, B. M. Keyes, and S. A. Ringel, Appl. Phys. Lett. 84, 3884 (2004)]. This lower electron lifetime suggests an increase in depletion region recombination and thus in the reverse saturation current (J0 for an n+/p diode compared with a p+/n diode at a given TDD. To confirm this, GaAs diodes of both polarities were grown on compositionally graded Ge /Si1-xGex/Si (SiGe) substrates with a TDD of 1×106cm-2. It is shown that the ratio of measured J0 values is consistent with the inverse ratio of the expected lifetimes. Using a TDD-dependent lifetime in solar cell current-voltage models we found that the Voc, for a given short-circuit current, also exhibits a poorer TDD tolerance for GaAs n+/p solar cells compared with GaAs p+/n solar cells. Experimentally, the open-circuit voltage (Voc) for the n+/p GaAs solar cell grown on a SiGe substrate with a TDD of ˜1×106cm-2 was ˜880mV which was significantly lower than the ˜980mV measured for a p+/n GaAs solar cell grown on SiGe at the same TDD and was consistent with the solar cell modeling results reported in this paper. We conclude that p+/n polarity GaAs junctions demonstrate superior dislocation tolerance than n+/p configured GaAs junctions, which is important for optimization of lattice-mismatched III-V devices.

  19. Fabrication of n-ZnO:Al/p-Si(100) heterojunction diode and its characterization

    NASA Astrophysics Data System (ADS)

    Parvathy Venu, M.; Dharmaprakash, S. M.; Byrappa, K.

    2018-04-01

    Aluminum doped ZnO (n-ZnO:Al) nanostructured thin films were grown on ZnO seed layer coated p-Si(100) substrate employing hydrothermal technique. X-ray diffraction pattern revealed that the ZnO:Al film possess hexagonal wurtzite structure with preferential orientation along (002) direction. Photoluminescence of the sample displayed near band edge emission peak in the ultra-violet region and defect level emission peak in the visible region. The as grown thin film was used in the fabrication of n-ZnO:Al/p-Si heterojunction diode and the room temperature current-voltage (I-V) and capacitance-voltage (C-V) characteristics were studied. The heterojunction exhibited fairly good rectification with an ideality of 2.49 and reverse saturation current of 2 nA. The barrier height was found to be 0.668 eV from the I-V measurements. The C-V measurements showed a decrease in the capacitance of the heterojunction with an increase in the reverse bias voltage.

  20. Investigation of gate-diode degradation in normally-off p-GaN/AlGaN/GaN high-electron-mobility transistors

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Ťapajna, M., E-mail: milan.tapajna@savba.sk; Kuzmík, J.; Hilt, O.

    2015-11-09

    Gate diode conduction mechanisms were analyzed in normally-off p-GaN/AlGaN/GaN high-electron mobility transistors grown on Si wafers before and after forward bias stresses. Electrical characterization of the gate diodes indicates forward current to be limited by channel electrons injected through the AlGaN/p-GaN triangular barrier promoted by traps. On the other hand, reverse current was found to be consistent with carrier generation-recombination processes in the AlGaN layer. Soft breakdown observed after ∼10{sup 5 }s during forward bias stress at gate voltage of 7 V was attributed to formation of conductive channel in p-GaN/AlGaN gate stack via trap generation and percolation mechanism, likely due tomore » coexistence of high electric field and high forward current density. Possible enhancement of localized conductive channels originating from spatial inhomogeneities is proposed to be responsible for the degradation.« less

  1. Determination of the k{sub Q{sub c{sub l{sub i{sub n,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub i}{sub n},f{sub m}{sub s}{sub r}}}}}}}}} correction factors for detectors used with an 800 MU/min CyberKnife{sup ®} system equipped with fixed collimators and a study of detector response to small photon beams using a Monte Carlo method

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Moignier, C., E-mail: cyril.moignier@free.fr; Huet, C.; Makovicka, L.

    Purpose: In a previous work, output ratio (OR{sub det}) measurements were performed for the 800 MU/min CyberKnife{sup ®} at the Oscar Lambret Center (COL, France) using several commercially available detectors as well as using two passive dosimeters (EBT2 radiochromic film and micro-LiF TLD-700). The primary aim of the present work was to determine by Monte Carlo calculations the output factor in water (OF{sub MC,w}) and the k{sub Q{sub c{sub l{sub i{sub n,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub i}{sub n},f{sub m}{sub s}{sub r}}}}}}}}} correction factors. The secondary aim was to study the detector response in small beams using Monte Carlomore » simulation. Methods: The LINAC head of the CyberKnife{sup ®} was modeled using the PENELOPE Monte Carlo code system. The primary electron beam was modeled using a monoenergetic source with a radial gaussian distribution. The model was adjusted by comparisons between calculated and measured lateral profiles and tissue-phantom ratios obtained with the largest field. In addition, the PTW 60016 and 60017 diodes, PTW 60003 diamond, and micro-LiF were modeled. Output ratios with modeled detectors (OR{sub MC,det}) and OF{sub MC,w} were calculated and compared to measurements, in order to validate the model for smallest fields and to calculate k{sub Q{sub c{sub l{sub i{sub n,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub i}{sub n},f{sub m}{sub s}{sub r}}}}}}}}} correction factors, respectively. For the study of the influence of detector characteristics on their response in small beams; first, the impact of the atomic composition and the mass density of silicon, LiF, and diamond materials were investigated; second, the material, the volume averaging, and the coating effects of detecting material on the detector responses were estimated. Finally, the influence of the size of silicon chip on diode response was investigated. Results: Looking at measurement ratios (uncorrected output factors) compared to the OF{sub MC,w}, the PTW

  2. Controlled electroluminescence of n-ZnMgO/p-GaN light-emitting diodes

    NASA Astrophysics Data System (ADS)

    Goh, E. S. M.; Yang, H. Y.; Han, Z. J.; Chen, T. P.; Ostrikov, K.

    2012-12-01

    Effective control of room-temperature electroluminescence of n-ZnMgO/p-GaN light-emitting diodes (LEDs) over both emission intensity and wavelength is demonstrated. With varied Mg concentration, the intensity of LEDs in the near-ultraviolet region is increased due to the effective radiative recombination in the ZnMgO layer. Furthermore, the emission wavelength is shifted to the green/yellow spectral region by employing an indium-tin-oxide thin film as the dopant source, where thermally activated indium diffusion creates extra deep defect levels for carrier recombination. These results clearly demonstrate the effectiveness of controlled metal incorporation in achieving high energy efficiency and spectral tunability of the n-ZnMgO/p-GaN LED devices.

  3. Trap assisted space charge conduction in p-NiO/n-ZnO heterojunction diode

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Tyagi, Manisha; Tomar, Monika; Gupta, Vinay, E-mail: drguptavinay@gmail.com

    2015-06-15

    Highlights: • p-NiO/n-ZnO heterojunction diode with enhanced junction parameters has been prepared. • Temperature dependent I–V throw insight into the involved conduction mechanism. • SCLC with exponential trap distribution was found to be the dominant mechanism. • C–V measurement at different frequencies support the presence of traps. - Abstract: The development of short-wavelength p–n junction is essentially important for the realization of transparent electronics for next-generation optoelectronic devices. In the present work, a p–n heterojunction diode based on p-NiO/n-ZnO has been prepared under the optimised growth conditions exhibiting improved electrical and junction parameters. The fabricated heterojunction gives typical current–voltage (I–V)more » characteristics with good rectifying behaviour (rectification ratio ≈ 10{sup 4} at 2 V). The temperature dependent current–voltage characteristics of heterojunction diode have been studied and origin of conduction mechanism is identified. The space-charge limited conduction with exponential trap distribution having deep level trap is found to be the dominant conduction mechanism in the fabricated p–n heterojunction diode. The conduction and valence band discontinuities for NiO/ZnO heterostructure have been determined from the capacitance–voltage (C–V) measurements.« less

  4. Modular multi-element high energy particle detector

    DOEpatents

    Coon, D.D.; Elliott, J.P.

    1990-01-02

    Multi-element high energy particle detector modules comprise a planar heavy metal carrier of tungsten alloy with planar detector units uniformly distributed over one planar surface. The detector units are secured to the heavy metal carrier by electrically conductive adhesive so that the carrier serves as a common ground. The other surface of each planar detector unit is electrically connected to a feedthrough electrical terminal extending through the carrier for front or rear readout. The feedthrough electrical terminals comprise sockets at one face of the carrier and mating pins projecting from the other face, so that any number of modules may be plugged together to create a stack of modules of any desired number of radiation lengths. The detector units each comprise four, preferably rectangular, p-i-n diode chips arranged around the associated feedthrough terminal to form a square detector unit providing at least 90% detector element coverage of the carrier. Integral spacers projecting from the carriers extend at least partially along the boundaries between detector units to space the p-i-n diode chips from adjacent carriers in a stack. The spacers along the perimeters of the modules are one-half the width of the interior spacers so that when stacks of modules are arranged side by side to form a large array of any size or shape, distribution of the detector units is uniform over the entire array. 5 figs.

  5. Room temperature electroluminescence from n-ZnO:Ga/ i-ZnO/ p-GaN:Mg heterojunction device grown by PLD

    NASA Astrophysics Data System (ADS)

    Zhang, Lichun; Li, Qingshan; Wang, Feifei; Qu, Chong; Zhao, Fengzhou

    2014-05-01

    The n-ZnO:Ga/ p-GaN:Mg and n-ZnO:Ga/ i-ZnO/ p-GaN:Mg heterojunction light emitting diodes (LEDs) were fabricated by the pulsed laser deposition (PLD) technique. The blue electroluminescence (EL) of the n-ZnO:Ga/ p-GaN:Mg heterojunction LEDs is emitted mainly from the p-GaN layer instead of the n-ZnO:Ga layer, for the reason that the electron injection from n-ZnO:Ga prevailed over the hole injection from p-GaN:Mg due to the higher carrier concentration and carrier mobility in n-ZnO:Ga. On the other hand, the n-ZnO:Ga/ i-ZnO/ p-GaN:Mg heterojunction LEDs exhibited dominant ultraviolet-blue emission. The reason for this difference is attributed to the inserted undoped i-ZnO layer between n-ZnO:Ga and p-GaN:Mg, in which the holes from p-GaN:Mg and the electrons from n-ZnO:Ga are recombined.

  6. Low cost, p-ZnO/n-Si, rectifying, nano heterojunction diode: Fabrication and electrical characterization.

    PubMed

    Kabra, Vinay; Aamir, Lubna; Malik, M M

    2014-01-01

    A low cost, highly rectifying, nano heterojunction (p-ZnO/n-Si) diode was fabricated using solution-processed, p-type, ZnO nanoparticles and an n-type Si substrate. p-type ZnO nanoparticles were synthesized using a chemical synthesis route and characterized by XRD and a Hall effect measurement system. The device was fabricated by forming thin film of synthesized p-ZnO nanoparticles on an n-Si substrate using a dip coating technique. The device was then characterized by current-voltage (I-V) and capacitance-voltage (C-V) measurements. The effect of UV illumination on the I-V characteristics was also explored and indicated the formation of a highly rectifying, nano heterojunction with a rectification ratio of 101 at 3 V, which increased nearly 2.5 times (232 at 3 V) under UV illumination. However, the cut-in voltage decreases from 1.5 V to 0.9 V under UV illumination. The fabricated device could be used in switches, rectifiers, clipper and clamper circuits, BJTs, MOSFETs and other electronic circuitry.

  7. Efficiency and droop improvement in a blue InGaN-based light emitting diode with a p-InGaN layer inserted in the GaN barriers

    NASA Astrophysics Data System (ADS)

    Wang, Xing-Fu; Tong, Jin-Hui; Zhao, Bi-Jun; Chen, Xin; Ren, Zhi-Wei; Li, Dan-Wei; Zhuo, Xiang-Jing; Zhang, Jun; Yi, Han-Xiang; Li, Shu-Ti

    2013-09-01

    The advantages of a blue InGaN-based light-emitting diode with a p-InGaN layer inserted in the GaN barriers is studied. The carrier concentration in the quantum well, radiative recombination rate in the active region, output power, and internal quantum efficiency are investigated. The simulation results show that the InGaN-based light-emitting diode with a p-InGaN layer inserted in the barriers has better performance over its conventional counterpart and the light emitting diode with p-GaN inserted in the barriers. The improvement is due to enhanced Mg acceptor activation and enhanced hole injection into the quantum wells.

  8. Optimizing photon-pair generation electronically using a p-i-n diode incorporated in a silicon microring resonator

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Savanier, Marc, E-mail: msavanier@eng.ucsd.edu; Kumar, Ranjeet; Mookherjea, Shayan, E-mail: smookherjea@eng.ucsd.edu

    Silicon photonic microchips may be useful for compact, inexpensive, room-temperature optically pumped photon-pair sources, which unlike conventional photon-pair generators based on crystals or optical fibers, can be manufactured using CMOS-compatible processes on silicon wafers. It has been shown that photon pairs can be created in simple structures such as microring resonators at a rate of a few hundred kilohertz using less than a milliwatt of optical pump power, based on the process of spontaneous four-wave mixing. To create a practical photon-pair source, however, also requires some way of monitoring the device and aligning the pump wavelength when the temperature varies,more » since silicon resonators are highly sensitive to temperature. In fact, monitoring photodiodes are standard components in classical laser diodes, but the incorporation of germanium or InGaAs photodiodes would raise the cost and fabrication complexity. Here, we present a simple and effective all-electronic technique for finding the optimum operating point for the microring used to generate photon pairs, based on measuring the reverse-biased current in a silicon p-i-n junction diode fabricated across the waveguide that constitutes the silicon microring. We show that by monitoring the current, and using it to tune the pump laser wavelength, the photon-pair generation properties of the microring can be preserved over a temperature range of more than 30 °C.« less

  9. Analysis of the auger recombination rate in P+N-n-N-N HgCdTe detectors for HOT applications

    NASA Astrophysics Data System (ADS)

    Schuster, J.; Tennant, W. E.; Bellotti, E.; Wijewarnasuriya, P. S.

    2016-05-01

    Infrared (IR) photon detectors must be cryogenically cooled to provide the highest possible performance, usually to temperatures at or below ~ 150K. Such low operating temperatures (Top) impose very stringent requirements on cryogenic coolers. As such, there is a constant push in the industry to engineer new detector architectures that operate at higher temperatures, so called higher operating temperature (HOT) detectors. The ultimate goal for HOT detectors is room temperature operation. While this is not currently possibly for photon detectors, significant increases in Top are nonetheless beneficial in terms of reduced size, weight, power and cost (SWAP-C). The most common HgCdTe IR detector architecture is the P+n heterostructure photodiode (where a capital letter indicates a wide band gap relative to the active layer or "AL"). A variant of this architecture, the P+N-n-N-N heterostructure photodiode, should have a near identical photo-response to the P+n heterostructure, but with significantly lower dark diffusion current. The P+N-n-N-N heterostructure utilizes a very low doped AL, surrounded on both sides by wide-gap layers. The low doping in the AL, allows the AL to be fully depleted, which drastically reduces the Auger recombination rate in that layer. Minimizing the Auger recombination rate reduces the intrinsic dark diffusion current, thereby increasing Top. Note when we use the term "recombination rate" for photodiodes, we are actually referring to the net generation and recombination of minority carriers (and corresponding dark currents) by the Auger process. For these benefits to be realized, these devices must be intrinsically limited and well passivated. The focus of this proceeding is on studying the fundamental physics of the intrinsic dark currents in ideal P+N-n-N-N heterostructures, namely Auger recombination. Due to the complexity of these devices, specifically the presence of multiple heterojunctions, numerical device modeling techniques must be

  10. Design and experimental testing of air slab caps which convert commercial electron diodes into dual purpose, correction-free diodes for small field dosimetry

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Charles, P. H., E-mail: paulcharles111@gmail.com; Cranmer-Sargison, G.; Thwaites, D. I.

    2014-10-15

    Purpose: Two diodes which do not require correction factors for small field relative output measurements are designed and validated using experimental methodology. This was achieved by adding an air layer above the active volume of the diode detectors, which canceled out the increase in response of the diodes in small fields relative to standard field sizes. Methods: Due to the increased density of silicon and other components within a diode, additional electrons are created. In very small fields, a very small air gap acts as an effective filter of electrons with a high angle of incidence. The aim was tomore » design a diode that balanced these perturbations to give a response similar to a water-only geometry. Three thicknesses of air were placed at the proximal end of a PTW 60017 electron diode (PTWe) using an adjustable “air cap”. A set of output ratios (OR{sub Det}{sup f{sub c}{sub l}{sub i}{sub n}}) for square field sizes of side length down to 5 mm was measured using each air thickness and compared to OR{sub Det}{sup f{sub c}{sub l}{sub i}{sub n}} measured using an IBA stereotactic field diode (SFD). k{sub Q{sub c{sub l{sub i{sub n,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub i}{sub n},f{sub m}{sub s}{sub r}}}}}}}}} was transferred from the SFD to the PTWe diode and plotted as a function of air gap thickness for each field size. This enabled the optimal air gap thickness to be obtained by observing which thickness of air was required such that k{sub Q{sub c{sub l{sub i{sub n,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub i}{sub n},f{sub m}{sub s}{sub r}}}}}}}}} was equal to 1.00 at all field sizes. A similar procedure was used to find the optimal air thickness required to make a modified Sun Nuclear EDGE detector (EDGEe) which is “correction-free” in small field relative dosimetry. In addition, the feasibility of experimentally transferring k{sub Q{sub c{sub l{sub i{sub n,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub i}{sub n},f{sub m}{sub s}{sub r

  11. Characterization of zero-bias microwave diode power detectors at cryogenic temperature.

    PubMed

    Giordano, Vincent; Fluhr, Christophe; Dubois, Benoît; Rubiola, Enrico

    2016-08-01

    We present the characterization of commercial tunnel diode low-level microwave power detectors at room and cryogenic temperatures. The sensitivity as well as the output voltage noise of the tunnel diodes is measured as functions of the applied microwave power. We highlight strong variations of the diode characteristics when the applied microwave power is higher than a few microwatts. For a diode operating at 4 K, the differential gain increases from 1000 V/W to about 4500 V/W when the power passes from -30 dBm to -20 dBm. The diode white noise floor is equivalent to a Noise Equivalent Power of 0.8 pW/Hz and 8 pW/Hz at 4 K and 300 K, respectively. Its flicker noise is equivalent to a relative amplitude noise power spectral density Sα(1 Hz) = - 120 dB/Hz at 4 K. Flicker noise is 10 dB higher at room temperature.

  12. Perimeter Governed Minority Carrier Lifetimes in 4H-SiC p(+)-n Diodes Measured by Reverse Recovery Switching Transient Analysis

    NASA Technical Reports Server (NTRS)

    Neudeck, Philip G.

    1998-01-01

    Minority carrier lifetimes in epitaxial 4H-SiC p(+)-n junction diodes were measured via an analysis of reverse recovery switching characteristics. Behavior of reverse recovery storage time (t(s)) as a function of initial ON-state forward current (I(F)) and OFF-state reverse current (I(R)) followed well-documented trends which have been observed for decades in silicon p-n rectifiers. Average minority carrier (hole) lifetimes (tau(p)) calculated from plots of t(s) vs I(R)/I(F) strongly decreased with decreasing device area. Bulk and perimeter components of average hole lifetimes were separated by plotting 1/tau(p) as a function of device perimeter-to- area ratio (P/A). This plot reveals that perimeter recombination is dominant in these devices, whose areas are all less than 1 sq mm. The bulk minority carrier (hole) lifetime extracted from the 1/tau(p) vs P/A plot is approximately 0.7 micro-s, well above the 60 ns to 300 ns average iit'eptimes obtained when perimeter recombination effects are ignored in the analysis. Given the fact that there has been little previous investigation of bipolar diode and transistor performance as a function of perimeter-to-area ratio, this work raises the possibility that perimeter recombination may be partly responsible for poor effective minority carrier lifetimes and limited performance obtained in many previous SiC bipolar junction devices.

  13. Correlation between dislocations and leakage current of p-n diodes on a free-standing GaN substrate

    NASA Astrophysics Data System (ADS)

    Usami, Shigeyoshi; Ando, Yuto; Tanaka, Atsushi; Nagamatsu, Kentaro; Deki, Manato; Kushimoto, Maki; Nitta, Shugo; Honda, Yoshio; Amano, Hiroshi; Sugawara, Yoshihiro; Yao, Yong-Zhao; Ishikawa, Yukari

    2018-04-01

    Dislocations that cause a reverse leakage current in vertical p-n diodes on a GaN free-standing substrate were investigated. Under a high reverse bias, dot-like leakage spots were observed using an emission microscope. Subsequent cathodoluminescence (CL) observations revealed that the leakage spots coincided with part of the CL dark spots, indicating that some types of dislocation cause reverse leakage. When etch pits were formed on the dislocations by KOH etching, three sizes of etch pits were obtained (large, medium, and small). Among these etch pits, only the medium pits coincided with leakage spots. Additionally, transmission electron microscopy observations revealed that pure screw dislocations are present under the leakage spots. The results revealed that 1c pure screw dislocations are related to the reverse leakage in vertical p-n diodes.

  14. Organic/Inorganic Hybrid p-n Junction with PEDOT Nanoparticles for Light-Emitting Diode

    NASA Astrophysics Data System (ADS)

    Kim, M. S.; Jin, S. M.; Cho, M. Y.; Choi, H. Y.; Kim, G. S.; Jeon, S. M.; Yim, K. G.; Kim, H. G.; Shim, K. B.; Kang, B. K.; Kim, Y.; Lee, D. Y.; Kim, J. S.; Kim, J. S.; Leem, J. Y.

    2011-12-01

    A heavily Si-doped GaN/polymer hybrid structure with p-type poly(3,4-ethylene-dioxythiophene):beta-1,3-glucan (PEDOT nanoparticle) interface layer has been fabricated. The Si-doped GaN thin film with carrier concentration of 1×1019 cm-3 was grown by metal-organic chemical vapor deposition (MOCVD). The PEDOT nanoparticle with various sizes ranging from 60 to 120 nm was synthesized via a miniemulsion polymerization process. The electrical conductivity of the PEDOT nanoparticle is less than 1.2 S/cm. The current-voltage (I-V) characteristic of the hybrid structure shows diode-like behavior. The I-V characteristic was examined in the framework of the thermionic emission model. The ideality factor and barrier height of the hybrid structure were obtained as 5.6 and 0.41 eV, respectively. The value of ideality factor is decreased by inserting the PEDOT nanoparticle interface layer.

  15. Spectral perturbations from silicon diode detector encapsulation and shielding in photon fields.

    PubMed

    Eklund, Karin; Ahnesjö, Anders

    2010-11-01

    Silicon diodes are widely used as detectors for relative dose measurements in radiotherapy. The common manufacturing practice is to encapsulate the diodes in plastic for protection and to facilitate mounting in scanning devices. Diodes intended for use in photon fields commonly also have a shield of a high atomic number material (usually tungsten) integrated into the encapsulation to selectively absorb low-energy photons to which silicon diodes would otherwise over-response. However, new response models based on cavity theories and spectra calculations have been proposed for direct correction of the readout from unshielded (e.g., "electron") diodes used in photon fields. This raises the question whether it is correct to assume that the spectrum in a water phantom at the location of the detector cavity is not perturbed by the detector encapsulation materials. The aim of this work is to investigate the spectral effects of typical encapsulations, including shielding, used for clinical diodes. The effects of detector encapsulation of an unshielded and a shielded commercial diode on the spectra at the detector cavity location are studied through Monte Carlo simulations with PENELOPE-2005. Variance reduction based on correlated sampling is applied to reduce the CPU time needed for the simulations. The use of correlated sampling is found to be efficient and to not introduce any significant bias to the results. Compared to reference spectra calculated in water, the encapsulation for an unshielded diode is demonstrated to not perturb the spectrum, while a tungsten shielded diode caused not only the desired decrease in low-energy scattered photons but also a large increase of the primary electron fluence. Measurements with a shielded diode in a 6 MV photon beam proved that the shielding does not completely remove the field-size dependence of the detector response caused by the over-response from low-energy photons. Response factors of a properly corrected unshielded diode

  16. Solid State pH Sensor Based on Light Emitting Diodes (LED) As Detector Platform

    PubMed Central

    Lau, King Tong; Shepherd, R.; Diamond, Danny; Diamond, Dermot

    2006-01-01

    A low-power, high sensitivity, very low-cost light emitting diode (LED)-based device developed for low-cost sensor networks was modified with bromocresol green membrane to work as a solid-state pH sensor. In this approach, a reverse-biased LED functioning as a photodiode is coupled with a second LED configured in conventional emission mode. A simple timer circuit measures how long (in microsecond) it takes for the photocurrent generated on the detector LED to discharge its capacitance from logic 1 (+5 V) to logic 0 (+1.7 V). The entire instrument provides an inherently digital output of light intensity measurements for a few cents. A light dependent resistor (LDR) modified with similar sensor membrane was also used as a comparison method. Both the LED sensor and the LDR sensor responded to various pH buffer solutions in a similar way to obtain sigmoidal curves expected of the dye. The pKa value obtained for the sensors was found to agree with the literature value.

  17. Integrated Amorphous Silicon p-i-n Temperature Sensor for CMOS Photonics.

    PubMed

    Rao, Sandro; Pangallo, Giovanni; Della Corte, Francesco Giuseppe

    2016-01-06

    Hydrogenated amorphous silicon (a-Si:H) shows interesting optoelectronic and technological properties that make it suitable for the fabrication of passive and active micro-photonic devices, compatible moreover with standard microelectronic devices on a microchip. A temperature sensor based on a hydrogenated amorphous silicon p-i-n diode integrated in an optical waveguide for silicon photonics applications is presented here. The linear dependence of the voltage drop across the forward-biased diode on temperature, in a range from 30 °C up to 170 °C, has been used for thermal sensing. A high sensitivity of 11.9 mV/°C in the bias current range of 34-40 nA has been measured. The proposed device is particularly suitable for the continuous temperature monitoring of CMOS-compatible photonic integrated circuits, where the behavior of the on-chip active and passive devices are strongly dependent on their operating temperature.

  18. Solar-energy conversion and light emission in an atomic monolayer p-n diode.

    PubMed

    Pospischil, Andreas; Furchi, Marco M; Mueller, Thomas

    2014-04-01

    The limitations of the bulk semiconductors currently used in electronic devices-rigidity, heavy weight and high costs--have recently shifted the research efforts to two-dimensional atomic crystals such as graphene and atomically thin transition-metal dichalcogenides. These materials have the potential to be produced at low cost and in large areas, while maintaining high material quality. These properties, as well as their flexibility, make two-dimensional atomic crystals attractive for applications such as solar cells or display panels. The basic building blocks of optoelectronic devices are p-n junction diodes, but they have not yet been demonstrated in a two-dimensional material. Here, we report a p-n junction diode based on an electrostatically doped tungsten diselenide (WSe2) monolayer. We present applications as a photovoltaic solar cell, a photodiode and a light-emitting diode, and obtain light-power conversion and electroluminescence efficiencies of ∼ 0.5% and ∼ 0.1%, respectively. Given recent advances in the large-scale production of two-dimensional crystals, we expect them to profoundly impact future developments in solar, lighting and display technologies.

  19. Advantages of an InGaN-based light emitting diode with a p-InGaN/p-GaN superlattice hole accumulation layer

    NASA Astrophysics Data System (ADS)

    Liu, Chao; Ren, Zhi-Wei; Chen, Xin; Zhao, Bi-Jun; Wang, Xing-Fu; Yin, Yi-An; Li, Shu-Ti

    2013-05-01

    P-InGaN/p-GaN superlattices (SLs) are developed for a hole accumulation layer (HAL) of a blue light emitting diode (LED). Free hole concentration as high as 2.6 × 1018 cm-3 is achieved by adjusting the Cp2Mg flow rate during the growth of p-InGaN/p-GaN SLs. The p-InGaN/p-GaN SLs with appropriate Cp2Mg flow rates are then incorporated between the multi-quantum well and AlGaN electron blocking layer as an HAL, which leads to the enhancement of light output power by 29% at 200 mA, compared with the traditional LED without such SL HAL. Meanwhile, the efficiency droop is also effectively alleviated in the LED with the SL HAL. The improved performance is attributed to the increased hole injection efficiency, and the reduced electron leakage by inserting the p-type SL HAL.

  20. Perimeter Governed Minority Carrier Lifetimes in 4H-SiC p+n Diodes Measured by Reverse Recovery Switching Transient Analysis

    NASA Technical Reports Server (NTRS)

    Neudeck, Philip G.

    1998-01-01

    Minority carrier lifetimes in epitaxial 4H-SiC p-n junction diodes were measured via an analysis of reverse recovery switching characteristics. Behavior of reverse recovery storage time (t(sub s)) as a function of initial ON-state forward current (I(sub f)) and OFF-state reverse current (I(sub R)) followed well-documented trends which have been observed for decades in silicon p-n rectifiers. Average minority carrier (hole) lifetimes (tau(sub p)) calculated from plots of t(sub s) vs I(sub R)/I(sub F) strongly decreased with decreasing device area. Bulk and perimeter components of average hole lifetimes were separated by plotting tau(sub p) as a function of device perimeter-to-area ratio (P/A). This plot reveals that perimeter recombination is dominant in these devices, whose areas are all less than 1 square mm. The bulk minority carrier (hole) lifetime extracted from the 1/Tau(sub p) vs P/A plot is approximately 0.7 microns, well above the 60 ns to 300 ns average lifetimes obtained when perimeter recombination effects are ignored in the analysis. Given the fact that there has been little previous investigation of bipolar diode and transistor performance as a function of perimeter-to-area ratio, this work raises the possibility that perimeter recombination may be partly responsible for poor effective minority carrier lifetimes and limited performance obtained in many previous SiC bipolar junction devices.

  1. Localized surface plasmon-enhanced ultraviolet electroluminescence from n-ZnO/i-ZnO/p-GaN heterojunction light-emitting diodes via optimizing the thickness of MgO spacer layer

    NASA Astrophysics Data System (ADS)

    Liu, W. Z.; Xu, H. Y.; Zhang, L. X.; Zhang, C.; Ma, J. G.; Wang, J. N.; Liu, Y. C.

    2012-10-01

    Localized surface plasmon (LSP)-enhanced ultraviolet light-emitting diodes were manufactured by introducing Ag nanoparticles and MgO spacer layer into n-ZnO/i-ZnO/p-GaN heterostructures. By optimizing the MgO thickness, which can suppress the undesired charge transfer and nonradiative Förster resonant energy transfer between Ag and ZnO, a 7-fold electroluminescence enhancement was achieved. Time-resolved and temperature-dependent photoluminescence measurements reveal that both spontaneous emission rate and internal quantum efficiency are increased as a result of coupling between ZnO excitons and Ag LSPs, and simple calculations, based on experimental data, also indicate that most of LSP's energy can be converted into the photon energy.

  2. Commissioning a p-type silicon diode for use in clinical electron beams.

    PubMed

    Eveling, J N; Morgan, A M; Pitchford, W G

    1999-01-01

    Commissioning measurements were carried out on a p-type silicon diode detector for use in patient monitoring in high energy electron beams. Characteristics specific to the diode were examined. The variation in diode sensitivity with dose per pulse was found to be less than 1% over a range 0.069-0.237 mGy/pulse. The diode exhibited a sensitivity variation with accumulated dose of 10% per kGy and a sensitivity variation with surface temperature of 0.26%/degree C. The dependence of the diode response on the direction of the incident electron beam was investigated. Results were found to exceed the manufacturer's specifications. Output factors measured with the diode agree to within 1.5% of those measured with an NACP-02 air ionization chamber. The detector showed a variation in response with energy of 0.8% over the energy range 4-15 MeV. Prior to introducing the diode into clinical use, an assessment of beam perturbation directly behind the diode was made. The maximum reduction in local dose directly behind the diode at a depth of 1.0 cm below the surface was approximately 13% at 4 and 15 MeV.

  3. Hydrothermal growth of n-ZnO films on a patterned p-GaN epilayer and its application in heterojunction light-emitting diodes

    NASA Astrophysics Data System (ADS)

    Ko, Rong-Ming; Wang, Shui-Jinn; Chen, Ching-Yi; Wu, Cheng-Han; Lin, Yan-Ru; Lo, Hsin-Ming

    2017-04-01

    The hydrothermal growth (HTG) of crystalline n-ZnO films on both the nonpatterned and patterned p-GaN epilayers with a honeycomb array of etched holes is demonstrated, and its application in n-ZnO/p-GaN heterojunction light-emitting diodes (HJ-LEDs) is reported. The results reveal that an HTG n-ZnO film on a patterned p-GaN layer exhibits a high-quality single crystal with FWHMs of 0.463 and 0.983° obtained from a ω-rocking curve and a ϕ-scan pattern, respectively, which are much better than those obtained on a nonpatterned p-GaN layer. In addition, the n-ZnO/patterned p-GaN HJ-LED exhibited a much better rectifying diode behavior owing to having a higher n-ZnO film crystallinity quality and an improved interface with the p-GaN layer. Strong violet and violet-blue lights emitted from the n-ZnO/patterned p-GaN HJ-LED at around 405, 412, and 430 nm were analyzed.

  4. On the effect of N-GaN/P-GaN/N-GaN/P-GaN/N-GaN built-in junctions in the n-GaN layer for InGaN/GaN light-emitting diodes.

    PubMed

    Kyaw, Zabu; Zhang, Zi-Hui; Liu, Wei; Tan, Swee Tiam; Ju, Zhen Gang; Zhang, Xue Liang; Ji, Yun; Hasanov, Namig; Zhu, Binbin; Lu, Shunpeng; Zhang, Yiping; Sun, Xiao Wei; Demir, Hilmi Volkan

    2014-01-13

    N-GaN/P-GaN/N-GaN/P-GaN/N-GaN (NPNPN-GaN) junctions embedded between the n-GaN region and multiple quantum wells (MQWs) are systematically studied both experimentally and theoretically to increase the performance of InGaN/GaN light emitting diodes (LEDs) in this work. In the proposed architecture, each thin P-GaN layer sandwiched in the NPNPN-GaN structure is completely depleted due to the built-in electric field in the NPNPN-GaN junctions, and the ionized acceptors in these P-GaN layers serve as the energy barriers for electrons from the n-GaN region, resulting in a reduced electron over flow and enhanced the current spreading horizontally in the n- GaN region. These lead to increased optical output power and external quantum efficiency (EQE) from the proposed device.

  5. Characterization of vertical GaN p-n diodes and junction field-effect transistors on bulk GaN down to cryogenic temperatures

    NASA Astrophysics Data System (ADS)

    Kizilyalli, I. C.; Aktas, O.

    2015-12-01

    There is great interest in wide-bandgap semiconductor devices and most recently in vertical GaN structures for power electronic applications such as power supplies, solar inverters and motor drives. In this paper the temperature-dependent electrical behavior of vertical GaN p-n diodes and vertical junction field-effect transistors fabricated on bulk GaN substrates of low defect density (104 to 106 cm-2) is described. Homoepitaxial MOCVD growth of GaN on its native substrate and the ability to control the doping in the drift layers in GaN have allowed the realization of vertical device architectures with drift layer thicknesses of 6 to 40 μm and net carrier electron concentrations as low as 1 × 1015 cm-3. This parameter range is suitable for applications requiring breakdown voltages of 1.2 kV to 5 kV. Mg, which is used as a p-type dopant in GaN, is a relatively deep acceptor (E A ≈ 0.18 eV) and susceptible to freeze-out at temperatures below 200 K. The loss of holes in p-GaN has a deleterious effect on p-n junction behavior, p-GaN contacts and channel control in junction field-effect transistors at temperatures below 200 K. Impact ionization-based avalanche breakdown (BV > 1200 V) in GaN p-n junctions is characterized between 77 K and 423 K for the first time. At higher temperatures the p-n junction breakdown voltage improves due to increased phonon scattering. A positive temperature coefficient in the breakdown voltage is demonstrated down to 77 K; however, the device breakdown characteristics are not as abrupt at temperatures below 200 K. On the other hand, contact resistance to p-GaN is reduced dramatically above room temperature, improving the overall device performance in GaN p-n diodes in all cases except where the n-type drift region resistance dominates the total forward resistance. In this case, the electron mobility can be deconvolved and is found to decrease with T -3/2, consistent with a phonon scattering model. Also, normally-on vertical junction

  6. SEM observation of p-n junction in semiconductors using fountain secondary electron detector

    NASA Astrophysics Data System (ADS)

    Sekiguchi, Takashi; Kimura, Takashi; Iwai, Hideo

    2016-11-01

    When we observe a p-n junction in a certain semiconductors using scanning electron microscope, it is known that the p-type region is brighter than n-type region in secondary electron (SE) image. To clarify this origin, the p-n junctions in 4H-SiC was observed using fountain secondary electron detector (FSED). The original FSED image shows brighter p-region than n-region, which is similar to the SE image taken by Everhart-Thonley detector, mainly due to the background component of SE signal. By subtracting the background, the line profiles of FSED signal across p-n junction have been recorded according to the SE energies. These profiles may include the detailed information of p-n junction.

  7. Correction of measured Gamma-Knife output factors for angular dependence of diode detectors and PinPoint ionization chamber.

    PubMed

    Hršak, Hrvoje; Majer, Marija; Grego, Timor; Bibić, Juraj; Heinrich, Zdravko

    2014-12-01

    Dosimetry for Gamma-Knife requires detectors with high spatial resolution and minimal angular dependence of response. Angular dependence and end effect time for p-type silicon detectors (PTW Diode P and Diode E) and PTW PinPoint ionization chamber were measured with Gamma-Knife beams. Weighted angular dependence correction factors were calculated for each detector. The Gamma-Knife output factors were corrected for angular dependence and end effect time. For Gamma-Knife beams angle range of 84°-54°. Diode P shows considerable angular dependence of 9% and 8% for the 18 mm and 14, 8, 4 mm collimator, respectively. For Diode E this dependence is about 4% for all collimators. PinPoint ionization chamber shows angular dependence of less than 3% for 18, 14 and 8 mm helmet and 10% for 4 mm collimator due to volumetric averaging effect in a small photon beam. Corrected output factors for 14 mm helmet are in very good agreement (within ±0.3%) with published data and values recommended by vendor (Elekta AB, Stockholm, Sweden). For the 8 mm collimator diodes are still in good agreement with recommended values (within ±0.6%), while PinPoint gives 3% less value. For the 4 mm helmet Diodes P and E show over-response of 2.8% and 1.8%, respectively. For PinPoint chamber output factor of 4 mm collimator is 25% lower than Elekta value which is generally not consequence of angular dependence, but of volumetric averaging effect and lack of lateral electronic equilibrium. Diodes P and E represent good choice for Gamma-Knife dosimetry. Copyright © 2014 Associazione Italiana di Fisica Medica. Published by Elsevier Ltd. All rights reserved.

  8. Enhanced Output Power of Near-Ultraviolet Light-Emitting Diodes by p-GaN Micro-Rods

    NASA Astrophysics Data System (ADS)

    Wang, Dong-Sheng; Zhang, Ke-Xiong; Liang, Hong-Wei; Song, Shi-Wei; Yang, De-Chao; Shen, Ren-Sheng; Liu, Yang; Xia, Xiao-Chuan; Luo, Ying-Min; Du, Guo-Tong

    2014-02-01

    Near-ultraviolet (UV) InGaN/AlGaN light-emitting diodes (LEDs) are grown by low-pressure metal-organic chemical vapor deposition. The scanning electronic microscope image shows that the p-GaN micro-rods are formed above the interface of p-AlGaN/p-GaN due to the rapid growth rate of p-GaN in the vertical direction. The p-GaN micro-rods greatly increase the escape probability of photons inside the LED structure. Electroluminescence intensities of the 372 nm UV LED lamps with p-GaN micro rods are 88% higher than those of the flat surface LED samples.

  9. The electrical properties of n-ZnO/p-SnO heterojunction diodes

    NASA Astrophysics Data System (ADS)

    Javaid, K.; Xie, Y. F.; Luo, H.; Wang, M.; Zhang, H. L.; Gao, J. H.; Zhuge, F.; Liang, L. Y.; Cao, H. T.

    2016-09-01

    In the present work, n-type zinc oxide (ZnO) and p-type tin monoxide (SnO) based heterostructure diodes were fabricated on an indium-tin-oxide glass using the radio frequency magnetron sputtering technique. The prepared ZnO/SnO diodes exhibited a typical rectifying behavior, with a forward to reverse current ratio about 500 ± 5 at 2 V and turn on voltage around 1.6 V. The built-in voltage of the diode was extracted to be 0.5 V based on the capacitance-voltage (C-V) measurement. The valence and conduction band offsets were deliberated through the band energy diagram of ZnO/SnO heterojunction, as 1.08 eV and 0.41 eV, respectively. The potential barrier-dependent carrier transportation mechanism across the space charge region was also investigated.

  10. Evaluation of the dosimetric properties of a diode detector for small field proton radiosurgery

    PubMed Central

    Teran, Anthony V.; Slater, Jerry D.; Slater, James M.; Wroe, Andrew J.

    2015-01-01

    The small fields and sharp gradients typically encountered in proton radiosurgery require high spatial resolution dosimetric measurements, especially below 1–2 cm diameters. Radiochromic film provides high resolution, but requires postprocessing and special handling. Promising alternatives are diode detectors with small sensitive volumes (SV) that are capable of high resolution and real‐time dose acquisition. In this study we evaluated the PTW PR60020 proton dosimetry diode using radiation fields and beam energies relevant to radiosurgery applications. Energies of 127 and 157 MeV (9.7 to 15 cm range) and initial diameters of 8, 10, 12, and 20 mm were delivered using single‐stage scattering and four modulations (0, 15, 30, and 60 mm) to a water tank in our treatment room. Depth dose and beam profile data were compared with PTW Markus N23343 ionization chamber, EBT2 Gafchromic film, and Monte Carlo simulations. Transverse dose profiles were measured using the diode in "edge‐on" orientation or EBT2 film. Diode response was linear with respect to dose, uniform with dose rate, and showed an orientation‐dependent (i.e., beam parallel to, or perpendicular to, detector axis) response of less than 1%. Diode vs. Markus depth‐dose profiles, as well as Markus relative dose ratio vs. simulated dose‐weighted average lineal energy plots, suggest that any LET‐dependent diode response is negligible from particle entrance up to the very distal portion of the SOBP for the energies tested. Finally, while not possible with the ionization chamber due to partial volume effects, accurate diode depth‐dose measurements of 8, 10, and 12 mm diameter beams were obtained compared to Monte Carlo simulations. Because of the small SV that allows measurements without partial volume effects and the capability of submillimeter resolution (in edge‐on orientation) that is crucial for small fields and high‐dose gradients (e.g., penumbra, distal edge), as well as negligible LET

  11. Gettering of Residual Impurities by Ion Implantation Damage in Poly-AlN UV Diode Detectors

    NASA Astrophysics Data System (ADS)

    Khan, A. H.; Stacy, T.; Meese, J. M.

    1996-03-01

    UV diode detectors have been fabricated from oriented polycrystalline AlN grown on (111) n-type 3-15Ω-cm Si substrates by CVD using AlCl3 and ammonia with a hydrogen carrier gas at 760-800C, 40-45 torr and gas flow rates of 350, 120, and 120 sccm for hydrogen, ammonia and hydrogen over heated AlCl_3. Half of the AlN film of thickness 1.5-2.0 microns was masked off prior to ion implantation. Samples were ion-implanted at 5 kV with methane, nitrogen and argon to a dose of 5-6 x 10^18 ions/cm^2. The AlN was contacted with sputtered Au while the Si was contacted with evaporated Al. No annealing was performed. Rectification was obtained as a result of radiation damage in the AlN. SIMs analysis showed a reduction of oxygen, hydrogen, chlorine and carbon by several orders of magnitude and to a depth of several microns in the ion implanted samples compared to the masked samples. The quantum efficiency was 16nm uncorrected for reflection from the AlN and thin metal contact.

  12. ZnS-Based ZnSTe:N/n-ZnS Light-Emitting Diodes

    NASA Astrophysics Data System (ADS)

    Ichino, Kunio; Kojima, Takahiro; Obata, Shunsuke; Kuroyanagi, Takuma; Nakazawa, Shoichi; Kashiyama, Shota

    2013-11-01

    ZnS1-xTex:N/n-ZnS diodes have been fabricated in an attempt to convert ZnS into p-type by Te incorporation and the resulting upward shift of the valence band maximum. The diodes exhibit clear rectification in the current-voltage characteristic and a peak of the electron-beam-induced current at the ZnS1-xTex:N/n-ZnS interface. Furthermore, a ZnS0.85Te0.15:N/n-ZnS diode exhibits blue-green electroluminescence due to self-activated emission in n-ZnS at 290 K under a forward current. These results suggest p-type conduction in ZnS1-xTex:N, and thus the LED operation of a ZnS-based pn-junction.

  13. Development of a silicon diode detector for skin dosimetry in radiotherapy.

    PubMed

    Vicoroski, Nikolina; Espinoza, Anthony; Duncan, Mitchell; Oborn, Bradley M; Carolan, Martin; Metcalfe, Peter; Menichelli, David; Perevertaylo, Vladimir L; Lerch, Michael L F; Rosenfeld, Anatoly B; Petasecca, Marco

    2017-10-01

    The aim of in vivo skin dosimetry was to measure the absorbed dose to the skin during radiotherapy, when treatment planning calculations cannot be relied on. It is of particularly importance in hypo-fractionated stereotactic modalities, where excessive dose can lead to severe skin toxicity. Currently, commercial diodes for such applications are with water equivalent depths ranging from 0.5 to 0.8 mm. In this study, we investigate a new detector for skin dosimetry based on a silicon epitaxial diode, referred to as the skin diode. The skin diode is manufactured on a thin epitaxial layer and packaged using the "drop-in" technology. It was characterized in terms of percentage depth dose, dose linearity, and dose rate dependence, and benchmarked against the Attix ionization chamber. The response of the skin diode in the build-up region of the percentage depth dose (PDD) curve of a 6 MV clinical photon beam was investigated. Geant4 radiation transport simulations were used to model the PDD in order to estimate the water equivalent measurement depth (WED) of the skin diode. Measured output factors using the skin diode were compared with the MOSkin detector and EBT3 film at 10 cm depth and at surface at isocenter of a water equivalent phantom. The intrinsic angular response of the skin diode was also quantified in charge particle equilibrium conditions (CPE) and at the surface of a solid water phantom. Finally, the radiation hardness of the skin diode up to an accumulated dose of 80 kGy using photons from a Co-60 gamma source was evaluated. The PDD curve measured with the skin diode was within 0.5% agreement of the equivalent Geant4 simulated curve. When placed at the phantom surface, the WED of the skin diode was estimated to be 0.075 ± 0.005 mm from Geant4 simulations and was confirmed using the response of a corrected Attix ionization chamber placed at water equivalent depth of 0.075 mm, with the measurement agreement to within 0.3%. The output factor measurements at

  14. Fabrication and characterization of GaN-based light-emitting diodes without pre-activation of p-type GaN.

    PubMed

    Hu, Xiao-Long; Wang, Hong; Zhang, Xi-Chun

    2015-01-01

    We fabricated GaN-based light-emitting diodes (LEDs) without pre-activation of p-type GaN. During the fabrication process, a 100-nm-thick indium tin oxide film was served as the p-type contact layer and annealed at 500°C in N2 ambient for 20 min to increase its transparency as well as to activate the p-type GaN. The electrical measurements showed that the LEDs were featured by a lower forward voltage and higher wall-plug efficiency in comparison with LEDs using pre-activation of p-type GaN. We discussed the mechanism of activation of p-type GaN at 500°C in N2 ambient. Furthermore, x-ray photoemission spectroscopy examinations were carried out to study the improved electrical performances of the LEDs without pre-activation of p-type GaN.

  15. Entrance dose measurements for in‐vivo diode dosimetry: Comparison of correction factors for two types of commercial silicon diode detectors

    PubMed Central

    Zhu, X. R.

    2000-01-01

    Silicon diode dosimeters have been used routinely for in‐vivo dosimetry. Despite their popularity, an appropriate implementation of an in‐vivo dosimetry program using diode detectors remains a challenge for clinical physicists. One common approach is to relate the diode readout to the entrance dose, that is, dose to the reference depth of maximum dose such as dmax for the 10×10 cm2 field. Various correction factors are needed in order to properly infer the entrance dose from the diode readout, depending on field sizes, target‐to‐surface distances (TSD), and accessories (such as wedges and compensate filters). In some clinical practices, however, no correction factor is used. In this case, a diode‐dosimeter‐based in‐vivo dosimetry program may not serve the purpose effectively; that is, to provide an overall check of the dosimetry procedure. In this paper, we provide a formula to relate the diode readout to the entrance dose. Correction factors for TSD, field size, and wedges used in this formula are also clearly defined. Two types of commercial diode detectors, ISORAD (n‐type) and the newly available QED (p‐type) (Sun Nuclear Corporation), are studied. We compared correction factors for TSDs, field sizes, and wedges. Our results are consistent with the theory of radiation damage of silicon diodes. Radiation damage has been shown to be more serious for n‐type than for p‐type detectors. In general, both types of diode dosimeters require correction factors depending on beam energy, TSD, field size, and wedge. The magnitudes of corrections for QED (p‐type) diodes are smaller than ISORAD detectors. PACS number(s): 87.66.–a, 87.52.–g PMID:11674824

  16. Facile fabrication and electrical investigations of nanostructured p-Si/n-TiO2 hetero-junction diode

    NASA Astrophysics Data System (ADS)

    Kumar, Arvind; Mondal, Sandip; Rao, K. S. R. Koteswara

    2018-05-01

    In this work, we have fabricated the nanostructured p-Si/n-TiO2 hetero-junction diode by using a facile spin-coating method. The XRD analysis suggests the presence of well crystalline anatase TiO2 film on Si with small grain size (˜16 nm). We have drawn the band alignment using Anderson model to understand the electrical transport across the junction. The current-voltage (J-V) characteristics analysis reveals the good rectification ratio (103 at ± 3 V) and slightly higher ideality factor (4.7) of our device. The interface states are responsible for the large ideality factor as Si/TiO2 form a dissimilar interface and possess a large number of dangling bonds. The study reveals the promises to be used Si/TiO2 diode as an alternative to the traditional p-n homo-junction diode, which typically require high budget.

  17. Black Phosphorus-Zinc Oxide Nanomaterial Heterojunction for p-n Diode and Junction Field-Effect Transistor.

    PubMed

    Jeon, Pyo Jin; Lee, Young Tack; Lim, June Yeong; Kim, Jin Sung; Hwang, Do Kyung; Im, Seongil

    2016-02-10

    Black phosphorus (BP) nanosheet is two-dimensional (2D) semiconductor with distinct band gap and attracting recent attention from researches because it has some similarity to gapless 2D semiconductor graphene in the following two aspects: single element (P) for its composition and quite high mobilities depending on its fabrication conditions. Apart from several electronic applications reported with BP nanosheet, here we report for the first time BP nanosheet-ZnO nanowire 2D-1D heterojunction applications for p-n diodes and BP-gated junction field effect transistors (JFETs) with n-ZnO channel on glass. For these nanodevices, we take advantages of the mechanical flexibility of p-type conducting of BP and van der Waals junction interface between BP and ZnO. As a result, our BP-ZnO nanodimension p-n diode displays a high ON/OFF ratio of ∼10(4) in static rectification and shows kilohertz dynamic rectification as well while ZnO nanowire channel JFET operations are nicely demonstrated by BP gate switching in both electrostatics and kilohertz dynamics.

  18. Evaluation of the dosimetric properties of a diode detector for small field proton radiosurgery.

    PubMed

    McAuley, Grant A; Teran, Anthony V; Slater, Jerry D; Slater, James M; Wroe, Andrew J

    2015-11-08

    The small fields and sharp gradients typically encountered in proton radiosurgery require high spatial resolution dosimetric measurements, especially below 1-2 cm diameters. Radiochromic film provides high resolution, but requires postprocessing and special handling. Promising alternatives are diode detectors with small sensitive volumes (SV) that are capable of high resolution and real-time dose acquisition. In this study we evaluated the PTW PR60020 proton dosimetry diode using radiation fields and beam energies relevant to radiosurgery applications. Energies of 127 and 157 MeV (9.7 to 15 cm range) and initial diameters of 8, 10, 12, and 20mm were delivered using single-stage scattering and four modulations (0, 15, 30, and 60mm) to a water tank in our treatment room. Depth dose and beam profile data were compared with PTW Markus N23343 ionization chamber, EBT2 Gafchromic film, and Monte Carlo simulations. Transverse dose profiles were measured using the diode in "edge-on" orientation or EBT2 film. Diode response was linear with respect to dose, uniform with dose rate, and showed an orientation-dependent (i.e., beam parallel to, or perpendicular to, detector axis) response of less than 1%. Diodevs. Markus depth-dose profiles, as well as Markus relative dose ratio vs. simulated dose-weighted average lineal energy plots, suggest that any LET-dependent diode response is negligible from particle entrance up to the very distal portion of the SOBP for the energies tested. Finally, while not possible with the ionization chamber due to partial volume effects, accurate diode depth-dose measurements of 8, 10, and 12 mm diameter beams were obtained compared to Monte Carlo simulations. Because of the small SV that allows measurements without partial volume effects and the capability of submillimeter resolution (in edge-on orientation) that is crucial for small fields and high-dose gradients (e.g., penumbra, distal edge), as well as negligible LET dependence over nearly the

  19. Forward Current Transport Mechanisms of Ni/Au—InAlN/AlN/GaN Schottky Diodes

    NASA Astrophysics Data System (ADS)

    Wang, Xiao-Feng; Shao, Zhen-Guang; Chen, Dun-Jun; Lu, Hai; Zhang, Rong; Zheng, You-Dou

    2014-05-01

    We fabricate two Ni/Au-In0.17Al0.83N/AlN/GaN Schottky diodes on substrates of sapphire and Si, respectively, and investigate their forward-bias current transport mechanisms by temperature-dependent current-voltage measurements. In the temperature range of 300-485 K, the Schottky barrier heights (SBHs) calculated by using the conventional thermionic-emission (TE) model are strongly positively dependent on temperature, which is in contrast to the negative-temperature-dependent characteristic of traditional semiconductor Schottky diodes. By fitting the forward-bias I-V characteristics using different current transport models, we find that the tunneling current model can describe generally the I-V behaviors in the entire measured range of temperature. Under the high forward bias, the traditional TE mechanism also gives a good fit to the measured I-V data, and the actual barrier heights calculated according to the fitting TE curve are 1.434 and 1.413 eV at 300K for InAlN/AlN/GaN Schottky diodes on Si and the sapphire substrate, respectively, and the barrier height shows a slightly negative temperature coefficient. In addition, a formula is given to estimate SBHs of Ni/Au—InAlN/AlN/GaN Schottky diodes taking the Fermi-level pinning effect into account.

  20. High-Yield Growth and Characterization of ⟨100⟩ InP p-n Diode Nanowires.

    PubMed

    Cavalli, Alessandro; Wang, Jia; Esmaeil Zadeh, Iman; Reimer, Michael E; Verheijen, Marcel A; Soini, Martin; Plissard, Sebastien R; Zwiller, Val; Haverkort, Jos E M; Bakkers, Erik P A M

    2016-05-11

    Semiconductor nanowires are nanoscale structures holding promise in many fields such as optoelectronics, quantum computing, and thermoelectrics. Nanowires are usually grown vertically on (111)-oriented substrates, while (100) is the standard in semiconductor technology. The ability to grow and to control impurity doping of ⟨100⟩ nanowires is crucial for integration. Here, we discuss doping of single-crystalline ⟨100⟩ nanowires, and the structural and optoelectronic properties of p-n junctions based on ⟨100⟩ InP nanowires. We describe a novel approach to achieve low resistance electrical contacts to nanowires via a gradual interface based on p-doped InAsP. As a first demonstration in optoelectronic devices, we realize a single nanowire light emitting diode in a ⟨100⟩-oriented InP nanowire p-n junction. To obtain high vertical yield, which is necessary for future applications, we investigate the effect of the introduction of dopants on the nanowire growth.

  1. Solution epitaxy of gallium-doped ZnO on p-GaN for heterojunction light-emitting diodes

    NASA Astrophysics Data System (ADS)

    Le, H. Q.; Lim, S. K.; Goh, G. K. L.; Chua, S. J.; Ang, N. S. S.; Liu, W.

    2010-09-01

    We report white light emission from a Ga-doped ZnO/p-GaN heterojunction light-emitting diode which was fabricated by growing gallium-doped ZnO film on the p-GaN in water at 90°C. As determined from Ga-doped ZnO films grown on (111) oriented MgAl2O4 spinel single crystal substrates, thermal treatment at 600°C in nitrogen ambient leads to a carrier concentration of 3.1×1020 cm-3 (and carrier mobility of 28 cm2/Vs) which is two orders of magnitude higher than that of the undoped films. Electroluminescence emissions at wavelengths of 393 nm (3.155 eV) and 529.5 nm (2.4 eV) were observed under forward bias in the heterojunction diode and white light could be visibly observed. The high concentration of electrons supplied from the Ga-doped ZnO films helped to enhance the carrier recombination and increase the light-emitting efficiency of the heterojunction diode.

  2. Vertical GaN merged PiN Schottky diode with a breakdown voltage of 2 kV

    NASA Astrophysics Data System (ADS)

    Hayashida, Tetsuro; Nanjo, Takuma; Furukawa, Akihiko; Yamamuka, Mikio

    2017-06-01

    In this study, we successfully fabricated vertical GaN merged PiN Schottky (MPS) diodes and comparatively investigated the cyclic p-GaN width (W p) dependence of their electrical characteristics, including turn-on voltage and reverse leakage current. The MPS diodes with W p of more than 6 µm can turn on at around 3 V. Increasing W p can suppress the reverse leakage current. Moreover, the vertical GaN MPS diode with the breakdown voltage of 2 kV was realized for the first time.

  3. Detector with internal gain for short-wave infrared ranging applications

    NASA Astrophysics Data System (ADS)

    Fathipour, Vala; Mohseni, Hooman

    2017-09-01

    Abstarct.Highly sensitive photon <span class="hlt">detectors</span> are regarded as the key enabling elements in many applications. Due to the low photon energy at the short-wave infrared (SWIR), photon detection and imaging at this band are very challenging. As such, many efforts in photon <span class="hlt">detector</span> research are directed toward improving the performance of the photon <span class="hlt">detectors</span> operating in this wavelength range. To solve these problems, we have developed an electron-injection (EI) technique. The significance of this detection mechanism is that it can provide both high efficiency and high sensitivity at room temperature, a condition that is very difficult to achieve in conventional SWIR <span class="hlt">detectors</span>. An EI <span class="hlt">detector</span> offers an overall system-level sensitivity enhancement due to a feedback stabilized internal avalanche-free gain. Devices exhibit an excess noise of unity, operate in linear mode, require bias voltage of a few volts, and have a cutoff wavelength of 1700 nm. We review the material system, operating principle, and development of EI <span class="hlt">detectors</span>. The shortcomings of the first-generation devices were addressed in the second-generation <span class="hlt">detectors</span>. Measurement on second-generation devices showed a high-speed response of ˜6 ns rise time, low jitter of less than 20 ps, high amplification of more than 2000 (at optical power levels larger than a few <span class="hlt">n</span>W), unity excess noise factor, and low leakage current (amplified dark current ˜10 <span class="hlt">n</span>A at a bias voltage of -3 V and at room temperature. These characteristics make EI <span class="hlt">detectors</span> a good candidate for high-resolution flash light detection and ranging (LiDAR) applications with millimeter scale depth resolution at longer ranges compared with conventional <span class="hlt">p-i-n</span> <span class="hlt">diodes</span>. Based on our experimentally measured device characteristics, we compare the performance of the EI <span class="hlt">detector</span> with commercially available linear mode InGaAs avalanche photodiode (APD) as well as a <span class="hlt">p-i-n</span> <span class="hlt">diode</span> using a theoretical model. Flash LiDAR images obtained by our model show that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE10154E..0NW','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE10154E..0NW"><span>Simulation based comparative analysis of photoresponse in front- and back-illuminated Ga<span class="hlt">N</span> <span class="hlt">P-I-N</span> ultraviolet photodetectors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Jun; Guo, Jin; Xie, Feng; Wang, Guosheng; Wu, Haoran; Song, Man; Yi, Yuanyuan</p> <p>2016-10-01</p> <p>This paper presents the comparative analysis of influence of doping level and doping profile of the active region on zero bias photoresponse characteristics of Ga<span class="hlt">N</span>-based <span class="hlt">p-i-n</span> ultraviolet (UV) photodetectors operating at front- and back-illuminated. A two dimensional physically-based computer simulation of Ga<span class="hlt">N</span>-based <span class="hlt">p-i-n</span> UV photodetectors is presented. We implemented Ga<span class="hlt">N</span> material properties and physical models taken from the literature. It is shown that absorption layer doping profile has notable impacts on the photoresponse of the device. Especially, the effect of doping concentration and distribution of the absorption layer on photoresponse is discussed in detail. In the case of front illumination, comparative to uniform <span class="hlt">n</span>-type doping, the device with <span class="hlt">n</span>-type Gaussian doping profiles at absorption layer has higher responsivity. Comparative to front illumination, back illuminated <span class="hlt">detector</span> with <span class="hlt">p</span>-type doping profiles at absorption layer has higher maximum photoresponse, while the Gaussian doping profiles have a weaker ability to enhance the device responsivity. It is demonstrated that electric field distribution, mobility degradation, and recombinations are jointly responsible for the variance of photoresponse. Our work enriches the understanding and utilization of Ga<span class="hlt">N</span> based <span class="hlt">p-i-n</span> UV photodetectors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930018592','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930018592"><span>InGaAs/In<span class="hlt">P</span> heteroepitaxial Schottky barrier <span class="hlt">diodes</span> for terahertz applications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bhapkar, Udayan V.; Li, Yongjun; Mattauch, Robert J.</p> <p>1992-01-01</p> <p>This paper explores the feasibility of planar, sub-harmonically pumped, anti-parallel InGaAs/In<span class="hlt">P</span> heteroepitaxial Schottky <span class="hlt">diodes</span> for terahertz applications. We present calculations of the (<span class="hlt">I</span>-V) characteristics of such <span class="hlt">diodes</span> using a numerical model that considers tunneling. We also present noise and conversion loss predictions of <span class="hlt">diode</span> mixers operated at 500 GHz, and obtained from a multi-port mixer analysis, using the <span class="hlt">I</span>-V characteristics predicted by our model. Our calculations indicate that InGaAs/In<span class="hlt">P</span> heteroepitaxial Schottky barrier <span class="hlt">diodes</span> are expected to have an <span class="hlt">I</span>-V characteristic with an ideality factor comparable to that of GaAs Schottky <span class="hlt">diodes</span>. However, the reverse saturation current of InGaAs/In<span class="hlt">P</span> <span class="hlt">diodes</span> is expected to be much greater than that of GaAs <span class="hlt">diodes</span>. These predictions are confirmed by experiment. The mixer analyses predict that sub-harmonically pumped anti-parallel InGaAs/In<span class="hlt">P</span> <span class="hlt">diode</span> mixers are expected to offer a 2 dB greater conversion loss and a somewhat higher single sideband noise temperature than their GaAs counterparts. More importantly, the InGaAs/In<span class="hlt">P</span> devices are predicted to require only one-tenth of the local oscillator power required by similar GaAs <span class="hlt">diodes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.8987E..20L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.8987E..20L"><span>Plasma treatment of <span class="hlt">p-GaN/n</span>-ZnO nanorod light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Leung, Yu Hang; Ng, Alan M. C.; Djurišic, Aleksandra B.; Chan, Wai Kin; Fong, Patrick W. K.; Lui, Hsien Fai; Surya, Charles</p> <p>2014-03-01</p> <p>Zinc oxide (ZnO) is a material of great interest for short-wavelength optoelectronic applications due to its wide band gap (3.37 eV) and high exciton binding energy (60 meV). Due to the difficulty in stable <span class="hlt">p</span>-type doping of ZnO, other <span class="hlt">p</span>-type materials such as gallium nitride (Ga<span class="hlt">N</span>) have been used to form heterojunctions with ZnO. <span class="hlt">p-GaN/n</span>-ZnO heterojunction devices, in particular light-emitting <span class="hlt">diodes</span> (LED) have been extensively studied. There was a huge variety of electronic properties and emission colors on the reported devices. It is due to the different energy alignment at the interface caused by different properties of the Ga<span class="hlt">N</span> layer and ZnO counterpart in the junction. Attempts have been made on modifying the heterojunction by various methods, such as introducing a dielectric interlayer and post-growth surface treatment, and changing the growth methods of ZnO. In this study, heterojunction LED devices with <span class="hlt">p-GaN</span> and ZnO nanorods array are demonstrated. The ZnO nanorods were grown by a solution method. The ZnO nanorods were exposed to different kinds of plasma treatments (such as nitrogen and oxygen) after the growth. It was found that the treatment could cause significant change on the optical properties of the ZnO nanorods, as well as the electronic properties and light emissions of the resultant LED devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9254E..0ZN','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9254E..0ZN"><span>AlGaIn<span class="hlt">N</span> laser <span class="hlt">diode</span> technology for defence, security and sensing applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Najda, Stephen P.; Perlin, Piotr; Suski, Tadek; Marona, Lucja; Boćkowski, Mike; Leszczyński, Mike; Wisniewski, Przemek; Czernecki, Robert; Kucharski, Robert; Targowski, Grzegorz; Watson, Scott; Kelly, Antony E.</p> <p>2014-10-01</p> <p>The latest developments in AlGaIn<span class="hlt">N</span> laser <span class="hlt">diode</span> technology are reviewed for defence, security and sensing applications. The AlGaIn<span class="hlt">N</span> material system allows for laser <span class="hlt">diodes</span> to be fabricated over a very wide range of wavelengths from u.v., <span class="hlt">i</span>.e, 380nm, to the visible, <span class="hlt">i</span>.e., 530nm, by tuning the indium content of the laser GaIn<span class="hlt">N</span> quantum well. Advantages of using Plasma assisted MBE (PAMBE) compared to more conventional MOCVD epitaxy to grow AlGaIn<span class="hlt">N</span> laser structures are highlighted. Ridge waveguide laser <span class="hlt">diode</span> structures are fabricated to achieve single mode operation with optical powers of <100mW in the 400-420nm wavelength range that are suitable for telecom applications. Visible light communications at high frequency (up to 2.5 Gbit/s) using a directly modulated 422nm Gallium-nitride (Ga<span class="hlt">N</span>) blue laser <span class="hlt">diode</span> is reported. High power operation of AlGaIn<span class="hlt">N</span> laser <span class="hlt">diodes</span> is demonstrated with a single chip, AlGaIn<span class="hlt">N</span> laser <span class="hlt">diode</span> `mini-array' with a common <span class="hlt">p</span>-contact configuration at powers up to 2.5W cw at 410nm. Low defectivity and highly uniform Ga<span class="hlt">N</span> substrates allow arrays and bars of nitride lasers to be fabricated. Ga<span class="hlt">N</span> laser bars of up to 5mm with 20 emitters, mounted in a CS mount package, give optical powers up to 4W cw at ~410nm with a common contact configuration. An alternative package configuration for AlGaIn<span class="hlt">N</span> laser arrays allows for each individual laser to be individually addressable allowing complex free-space and/or fibre optic system integration within a very small form-factor.or.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ApPhL.102r3509F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ApPhL.102r3509F"><span>Saturation of the junction voltage in Ga<span class="hlt">N</span>-based laser <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Feng, M. X.; Liu, J. P.; Zhang, S. M.; Liu, Z. S.; Jiang, D. S.; Li, Z. C.; Wang, F.; Li, D. Y.; Zhang, L. Q.; Wang, H.; Yang, H.</p> <p>2013-05-01</p> <p>Saturation of the junction voltage in Ga<span class="hlt">N</span>-based laser <span class="hlt">diodes</span> (LDs) is studied. It is found that there is a bump above the lasing transition in the <span class="hlt">I(dV/dI)-I</span> curve, instead of a dip as that for GaAs-based LDs. The bump in <span class="hlt">I(dV/dI)-I</span> curve moves to higher currents along with the lasing threshold. A model considering ambipolar conduction and electron overflow into <span class="hlt">p-AlGaN</span> cladding layer due to poor carrier confinement in active region is used to explain the anomaly. The characteristic temperature of Ga<span class="hlt">N</span>-based LD is obtained by fitting threshold currents determined from <span class="hlt">I(dV/dI)-I</span> curves. Moreover, it is found that Ga<span class="hlt">N</span>-based LDs show characteristics with a nonlinear series resistance, which may be due to the electron overflow into <span class="hlt">p-AlGaN</span> cladding layer and the enhanced activation of Mg acceptors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22098691-calculation-sub-sub-sub-sub-sub-sub-sub-sub-sup-sub-sub-sub-sub-sub-sub-sub-several-small-detectors-two-linear-accelerators-using-monte-carlo-simulations','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22098691-calculation-sub-sub-sub-sub-sub-sub-sub-sub-sup-sub-sub-sub-sub-sub-sub-sub-several-small-detectors-two-linear-accelerators-using-monte-carlo-simulations"><span>Calculation of k{sub Q{sub c{sub l{sub <span class="hlt">i</span>{sub <span class="hlt">n</span>,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub <span class="hlt">i</span>}{sub <span class="hlt">n</span>},f{sub m}{sub s}{sub r}}}}}}}}} for several small <span class="hlt">detectors</span> and for two linear accelerators using Monte Carlo simulations</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Francescon, P.; Cora, S.; Satariano, N.</p> <p>2011-12-15</p> <p>Purpose: The scope of this study was to determine a complete set of correction factors for several <span class="hlt">detectors</span> in static small photon fields for two linear accelerators (linacs) and for several <span class="hlt">detectors</span>. Methods: Measurements for Monte Carlo (MC) commissioning were performed for two linacs, Siemens Primus and Elekta Synergy. After having determined the source parameters that best fit the measurements of field specific output factors, profiles, and tissue-phantom ratio, the generalized version of the classical beam quality correction factor for static small fields, k{sub Q{sub c{sub l{sub <span class="hlt">i</span>{sub <span class="hlt">n</span>,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub <span class="hlt">i</span>}{sub <span class="hlt">n</span>},f{sub m}{sub s}{sub r}}}}}}}}},more » were determined for several types of <span class="hlt">detectors</span> by using the egs{sub c}hamber Monte Carlo user code which can accurately reproduce the geometry and the material composition of the <span class="hlt">detector</span>. The influence of many parameters (energy and radial FWHM of the electron beam source, field dimensions, type of accelerator) on the value of k{sub Q{sub c{sub l{sub <span class="hlt">i</span>{sub <span class="hlt">n</span>,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub <span class="hlt">i</span>}{sub <span class="hlt">n</span>},f{sub m}{sub s}{sub r}}}}}}}}} was evaluated. Moreover, a MC analysis of the parameters that influence the change of k{sub Q{sub c{sub l{sub <span class="hlt">i</span>{sub <span class="hlt">n</span>,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub <span class="hlt">i</span>}{sub <span class="hlt">n</span>},f{sub m}{sub s}{sub r}}}}}}}}} as a function of field dimension was performed. A detailed analysis of uncertainties related to the measurements of the field specific output factor and to the Monte Carlo calculation of k{sub Q{sub c{sub l{sub <span class="hlt">i</span>{sub <span class="hlt">n</span>,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub <span class="hlt">i</span>}{sub <span class="hlt">n</span>},f{sub m}{sub s}{sub r}}}}}}}}} was done. Results: The simulations demonstrated that the correction factor k{sub Q{sub c{sub l{sub <span class="hlt">i</span>{sub <span class="hlt">n</span>,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub <span class="hlt">i</span>}{sub <span class="hlt">n</span>},f{sub m}{sub s}{sub r}}}}}}}}} can be considered independent from the quality beam factor Q in the range 0.68 {+-} 0.01 for all the <span class="hlt">detectors</span> analyzed. The k{sub Q{sub c{sub l{sub <span class="hlt">i</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22258586-reconfigurable-junction-diodes-photovoltaic-effect-exfoliated-mos-sub-films','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22258586-reconfigurable-junction-diodes-photovoltaic-effect-exfoliated-mos-sub-films"><span>Reconfigurable <span class="hlt">p-n</span> junction <span class="hlt">diodes</span> and the photovoltaic effect in exfoliated MoS{sub 2} films</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Sutar, Surajit; Agnihotri, Pratik; Comfort, Everett</p> <p>2014-03-24</p> <p>Realizing basic semiconductor devices such as <span class="hlt">p-n</span> junctions are necessary for developing thin-film and optoelectronic technologies in emerging planar materials such as MoS{sub 2}. In this work, electrostatic doping by buried gates is used to study the electronic and optoelectronic properties of <span class="hlt">p-n</span> junctions in exfoliated MoS{sub 2} flakes. Creating a controllable doping gradient across the device leads to the observation of the photovoltaic effect in monolayer and bilayer MoS{sub 2} flakes. For thicker flakes, strong ambipolar conduction enables realization of fully reconfigurable <span class="hlt">p-n</span> junction <span class="hlt">diodes</span> with rectifying current-voltage characteristics, and <span class="hlt">diode</span> ideality factors as low as 1.6. The spectralmore » response of the photovoltaic effect shows signatures of the predicted band gap transitions. For the first excitonic transition, a shift of >4{sub kB}T is observed between monolayer and bulk devices, indicating a thickness-dependence of the excitonic coulomb interaction.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5605292','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/5605292"><span>Bandpass x-ray <span class="hlt">diode</span> and x-ray multiplier <span class="hlt">detector</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Wang, C.L.</p> <p>1982-09-27</p> <p>An absorption-edge of an x-ray absorption filter and a quantum jump of a photocathode determine the bandpass characteristics of an x-ray <span class="hlt">diode</span> <span class="hlt">detector</span>. An anode, which collects the photoelectrons emitted by the photocathode, has enhanced amplification provided by photoelectron-multiplying means which include dynodes or a microchannel-plate electron-multiplier. Suppression of undesired high frequency response for a bandpass x-ray <span class="hlt">diode</span> is provided by subtracting a signal representative of energies above the passband from a signal representative of the overall response of the bandpass <span class="hlt">diode</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SuMi..111..302D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SuMi..111..302D"><span>Design of high breakdown voltage vertical Ga<span class="hlt">N</span> <span class="hlt">p-n</span> <span class="hlt">diodes</span> with high-K/low-K compound dielectric structure for power electronics applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Du, Jiangfeng; Li, Zhenchao; Liu, Dong; Bai, Zhiyuan; Liu, Yang; Yu, Qi</p> <p>2017-11-01</p> <p>In this work, a vertical Ga<span class="hlt">N</span> <span class="hlt">p-n</span> <span class="hlt">diode</span> with a high-K/low-K compound dielectric structure (Ga<span class="hlt">N</span> CD-VGD) is proposed and designed to achieve a record high breakdown voltage (BV) with a low specific on-resistance (Ron,sp). By introducing compound dielectric structure, the electric field near the <span class="hlt">p-n</span> junction interface is suppressed due to the effects of high-K passivation layer, and a new electric field peak is induced into the <span class="hlt">n</span>-type drift region, because of a discontinuity of electrical field at the interface of high-K and low-K layer. Therefore the distribution of electric field in Ga<span class="hlt">N</span> <span class="hlt">p-n</span> <span class="hlt">diode</span> becomes more uniform and an enhancement of breakdown voltage can be achieved. Numerical simulations demonstrate that Ga<span class="hlt">N</span> CD-VGD with a BV of 10650 V and a Ron,sp of 14.3 mΩ cm2, resulting in a record high figure-of-merit of 8 GW/cm2.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20653094-avalanche-diode-electron-detector-observing-neet','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20653094-avalanche-diode-electron-detector-observing-neet"><span>An Avalanche <span class="hlt">Diode</span> Electron <span class="hlt">Detector</span> for Observing NEET</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Kishimoto, Shunji</p> <p>2004-05-12</p> <p>Nuclear excitation by electron transition (NEET) occurs in atomic inner-shell ionization if the nuclear excitation and the electron transition have nearly the same energy and a common multipolarity. We successfully observed the NEET on 197Au and on 193Ir using a silicon avalanche <span class="hlt">diode</span> electron <span class="hlt">detector</span>. The <span class="hlt">detector</span> was used to find internal conversion electrons emitted from excited nuclei in time spectroscopy with a time gate method. Some nuclear resonant levels, including 8.410 keV on 169Tm and 80.577 keV on 166Er, were also observed with the <span class="hlt">detector</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JInst..13P2017K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JInst..13P2017K"><span>Characterization of a SiC MIS Schottky <span class="hlt">diode</span> as RBS particle <span class="hlt">detector</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kaufmann, I. R.; Pick, A. C.; Pereira, M. B.; Boudinov, H. I.</p> <p>2018-02-01</p> <p>A 4H-SiC Schottky <span class="hlt">diode</span> was investigated as a particle <span class="hlt">detector</span> for Rutherford Backscattering Spectroscopy (RBS) experiment. The device was fabricated on a commercial 4H-SiC epitaxial <span class="hlt">n</span>-type layer grown onto a 4H-SiC <span class="hlt">n</span>+ type substrate wafer doped with nitrogen. Hafnium oxide with thickness of 1 nm was deposited by Atomic Layer Deposition and 10 nm of Ni were deposited by sputtering to form the Ni/HfO2/4H-SiC MIS Schottky structure. Current-Voltage curves with variable temperature were measured to extract the real Schottky Barrier Height (0.32 V) and ideality factor values (1.15). Reverse current and Capacitance-Voltage measurements were performed on the 4H-SiC <span class="hlt">detector</span> and compared to a commercial Si barrier <span class="hlt">detector</span> acquired from ORTEC. RBS data for four alpha energies (1, 1.5, 2 and 2.5 MeV) were collected from an Au/Si sample using the fabricated SiC and the commercial Si <span class="hlt">detectors</span> simultaneously. The energy resolution for the fabricated <span class="hlt">detector</span> was estimated to be between 75 and 80 keV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApPhL.111n2104M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhL.111n2104M"><span>Effect of interface voids on electroluminescence colors for ZnO microdisk/<span class="hlt">p-GaN</span> heterojunction light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mo, Ran; Choi, Ji Eun; Kim, Hyeong Jin; Jeong, Junseok; Kim, Jong Chan; Kim, Yong-Jin; Jeong, Hu Young; Hong, Young Joon</p> <p>2017-10-01</p> <p>This study investigates the influence of voids on the electroluminescence (EL) emission color of ZnO microdisk/<span class="hlt">p-GaN</span> heterojunction light-emitting <span class="hlt">diodes</span> (LEDs). For this study, position-controlled microdisk arrays were fabricated on patterned <span class="hlt">p-GaN</span> via wet chemical epitaxy of ZnO, and specifically, the use of trisodium citrate dihydrate (TCD) yielded high-density voids at the bottom of the microdisk. Greenish yellow or whitish blue EL was emitted from the microdisk LEDs formed with or without TCD, respectively, at reverse-bias voltages. Such different EL colors were found to be responsible for the relative EL intensity ratio between indigo and yellow emission peaks, which were originated from radiative recombination at <span class="hlt">p-GaN</span> and ZnO, respectively. The relative EL intensity between dichromatic emissions is discussed in terms of (<span class="hlt">i</span>) junction edge effect provoked by interfacial voids and (ii) electron tunneling probability depending on the depletion layer geometry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016MRE.....3l6401J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016MRE.....3l6401J"><span>High transmittance hetero junctions based on <span class="hlt">n-ITO/p</span>-CuO bilayer thin films</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jaya, T. P.; Pradyumnan, P. P.</p> <p>2016-12-01</p> <p>Oxide based bilayered <span class="hlt">n-ITO/p</span>-CuO crystalline <span class="hlt">diodes</span> were fabricated by plasma vapor deposition using radio frequency magnetron sputtering. The <span class="hlt">p-n</span> hetero junction <span class="hlt">diodes</span> were highly transparent in the visible region and exhibits rectifying <span class="hlt">I</span>-V characteristics. The substrate temperature during fabrication of <span class="hlt">p</span>-layer CuO was found to have a profound influence on <span class="hlt">I</span>-V characteristics. The films deposited at substrate temperature of 150 °C and 230 °C exhibited <span class="hlt">diode</span> ideality factors of (η value) 1.731 and 1.862 respectively. This high ideality factor, combined with an optical transparency of above 70% suggests the potential use of these bi-layers in optoelectronic applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3758658','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3758658"><span>Photo-<span class="hlt">Detectors</span> Integrated with Resonant Tunneling <span class="hlt">Diodes</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Romeira, Bruno; Pessoa, Luis M.; Salgado, Henrique M.; Ironside, Charles N.; Figueiredo, José M. L.</p> <p>2013-01-01</p> <p>We report on photo-<span class="hlt">detectors</span> consisting of an optical waveguide that incorporates a resonant tunneling <span class="hlt">diode</span> (RTD). Operating at wavelengths around 1.55 μm in the optical communications C band we achieve maximum sensitivities of around 0.29 A/W which is dependent on the bias voltage. This is due to the nature of RTD nonlinear current-voltage characteristic that has a negative differential resistance (NDR) region. The resonant tunneling <span class="hlt">diode</span> photo-<span class="hlt">detector</span> (RTD-PD) can be operated in either non-oscillating or oscillating regimes depending on the bias voltage quiescent point. The oscillating regime is apparent when the RTD-PD is biased in the NDR region giving rise to electrical gain and microwave self-sustained oscillations Taking advantage of the RTD's NDR distinctive characteristics, we demonstrate efficient detection of gigahertz (GHz) modulated optical carriers and optical control of a RTD GHz oscillator. RTD-PD based devices can have applications in generation and optical control of GHz low-phase noise oscillators, clock recovery systems, and fiber optic enabled radio frequency communication systems. PMID:23881142</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23881142','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23881142"><span>Photo-<span class="hlt">detectors</span> integrated with resonant tunneling <span class="hlt">diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Romeira, Bruno; Pessoa, Luis M; Salgado, Henrique M; Ironside, Charles N; Figueiredo, José M L</p> <p>2013-07-22</p> <p>We report on photo-<span class="hlt">detectors</span> consisting of an optical waveguide that incorporates a resonant tunneling <span class="hlt">diode</span> (RTD). Operating at wavelengths around 1.55 μm in the optical communications C band we achieve maximum sensitivities of around 0.29 A/W which is dependent on the bias voltage. This is due to the nature of RTD nonlinear current-voltage characteristic that has a negative differential resistance (NDR) region. The resonant tunneling <span class="hlt">diode</span> photo-<span class="hlt">detector</span> (RTD-PD) can be operated in either non-oscillating or oscillating regimes depending on the bias voltage quiescent point. The oscillating regime is apparent when the RTD-PD is biased in the NDR region giving rise to electrical gain and microwave self-sustained oscillations Taking advantage of the RTD's NDR distinctive characteristics, we demonstrate efficient detection of gigahertz (GHz) modulated optical carriers and optical control of a RTD GHz oscillator. RTD-PD based devices can have applications in generation and optical control of GHz low-phase noise oscillators, clock recovery systems, and fiber optic enabled radio frequency communication systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29630291','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29630291"><span>Fabrication of Heterojunction <span class="hlt">Diode</span> Based on <span class="hlt">n</span>-ZnO Nanowires/<span class="hlt">p</span>-Si Substrate: Temperature Dependent Transport Characteristics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Badran, R I; Umar, Ahmad</p> <p>2017-01-01</p> <p>Herein, we report the growth and characterizations of well-crystalline <span class="hlt">n</span>-ZnO nanowires assembled in micro flower-shaped morphologies. The nanowires are grown on <span class="hlt">p</span>-Silicon substrate and characterized in terms of their structural, morphological and electrical properties. Temperature dependent transport characteristics of the fabricated <span class="hlt">n-ZnO/p</span>-Si heterojunction <span class="hlt">diode</span> were examined. The morphological studies revealed that the nanowires are grown in high-density and arrange in special micro flower shaped morphology. The structural characterizations confirmed that the nanowires are well-crystalline and possessing wurtzite hexagonal phase. The electrical properties were evaluated by examining the I–V characteristics of the fabricated <span class="hlt">n-ZnO/p</span>-Si heterojunction <span class="hlt">diode</span>. The I–V characteristics were studied at temperature <300 K and ≥300 K in the forward and reverse bias conditions. The detailed temperature dependent electrical properties revealed that the fabricated heterojunction assembly shows a <span class="hlt">diode</span>-like behavior with a turn-on voltage of 5 V at almost all temperatures and the delivered current changes between ˜1 to ˜5 μA when temperature changes from 77 K to 425 K. The rectifying behavior of the fabricated heterojunction <span class="hlt">diode</span>, at 5 V, was demonstrated by rectifying ratio of ˜4 at 77 K which decreases to ˜1.5 at 425 K. This analysis also showed that the mean potential barrier of the fabricated heterojunction (˜1.2 eV) is larger than the energy difference (0.72 eV) of the work functions between Si and ZnO.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22482022-zno-sic-diode-structural-electrical-photoresponse-characteristics','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22482022-zno-sic-diode-structural-electrical-photoresponse-characteristics"><span><span class="hlt">n-ZnO/p</span>-4H-SiC <span class="hlt">diode</span>: Structural, electrical, and photoresponse characteristics</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Guziewicz, M., E-mail: margu@ite.waw.pl; Jung, W.; Schifano, R.</p> <p></p> <p>Epitaxial <span class="hlt">n</span>-type ZnO film has been grown, on a commercial 5 μm thick <span class="hlt">p</span>-type 4H-SiC(00.1) Al doped epilayer, by atomic layer deposition. A full width at half maximum of the ZnO 00.2 diffraction peak rocking curve of 0.34°{sup  }± 0.02° has been measured. <span class="hlt">Diodes</span> formed on the <span class="hlt">n-ZnO/p</span>-4H-SiC heterostructure show rectifying behavior with a forward to reverse current ratio at the level of 10{sup 9} at ±4 V, a leakage current density of ∼6 × 10{sup −8} A/cm{sup 2}, and a low ideality factor equal to 1.17 ± 0.04. In addition, the <span class="hlt">diodes</span> exhibit selective photoresponse with a maximum at 367 nm, and with a current increasemore » of ∼10{sup 3} under illuminations with respect to the dark value, which makes such devices prospective candidates for ultraviolet light sensors.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_7 --> <div id="page_8" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="141"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20413842','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20413842"><span>Surface plasmon-enhanced light-emitting <span class="hlt">diodes</span> using silver nanoparticles embedded in <span class="hlt">p-GaN</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cho, Chu-Young; Kwon, Min-Ki; Lee, Sang-Jun; Han, Sang-Heon; Kang, Jang-Won; Kang, Se-Eun; Lee, Dong-Yul; Park, Seong-Ju</p> <p>2010-05-21</p> <p>We demonstrate the surface plasmon-enhanced blue light-emitting <span class="hlt">diodes</span> (LEDs) using Ag nanoparticles embedded in <span class="hlt">p-GaN</span>. A large increase in optical output power of 38% is achieved at an injection current of 20 mA due to an improved internal quantum efficiency of the LEDs. The enhancement of optical output power is dependent on the density of the Ag nanoparticles. This improvement can be attributed to an increase in the spontaneous emission rate through resonance coupling between the excitons in multiple quantum wells and localized surface plasmons in Ag nanoparticles embedded in <span class="hlt">p-GaN</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1990NIMPA.288...87H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1990NIMPA.288...87H"><span>The bipolar silicon microstrip <span class="hlt">detector</span>: A proposal for a novel precision tracking device</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Horisberger, R.</p> <p>1990-03-01</p> <p>It is proposed to combine the technology of fully depleted silicon microstrip <span class="hlt">detectors</span> fabricated on <span class="hlt">n</span> doped high resistivity silicon with the concept of the bipolar transistor. This is done by adding a <span class="hlt">n</span> ++ doped region inside the normal <span class="hlt">p</span> + implanted region of the reverse biased <span class="hlt">p</span> + <span class="hlt">n</span> <span class="hlt">diode</span>. Teh resulting structure has amplifying properties and is referred to as bipolar pixel transistor. The simplest readout scheme of a bipolar pixel array by an aluminium strip bus leads to the bipolar microstrip <span class="hlt">detector</span>. The bipolar pixel structure is expected to give a better signal-to-noise performance for the detection of minimum ionizing charged particle tracks than the normal silicon <span class="hlt">diode</span> strip <span class="hlt">detector</span> and therefore should allow in future the fabrication of thinner silicon <span class="hlt">detectors</span> for precision tracking.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19720047872&hterms=silicon+detector+electrons&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsilicon%2Bdetector%2Belectrons','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19720047872&hterms=silicon+detector+electrons&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsilicon%2Bdetector%2Belectrons"><span>Infrared response measurements on radiation-damaged Si/Li/ <span class="hlt">detectors</span>.</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sher, A. H.; Liu, Y. M.; Keery, W. J.</p> <p>1972-01-01</p> <p>The improved infrared response (IRR) technique has been used to qualitatively compare radiation effects on Si(Li) <span class="hlt">detectors</span> with energy levels reported for silicon in the literature. Measurements have been made on five commercial silicon <span class="hlt">detectors</span> and one fabricated in-house, both before and after irradiation with fast neutrons, 1.9-MeV protons, and 1.6-MeV electrons. Effects dependent upon the extent of radiation damage have been observed. It seems likely that the photo-EMF, or photo-voltage, effect is the basic mechanism for the observation of IRR in <span class="hlt">p-i-n</span> <span class="hlt">diodes</span> with a wide <span class="hlt">i</span>-region. Experimental characteristics of the IRR measurement are in agreement with those of the photovoltage effect.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JaJAP..56l5502J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JaJAP..56l5502J"><span>Plasma vapor deposited <span class="hlt">n</span>-indium tin oxide/<span class="hlt">p</span>-copper indium oxide heterojunctions for optoelectronic device applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jaya, T. P.; Pradyumnan, P. P.</p> <p>2017-12-01</p> <p>Transparent crystalline <span class="hlt">n</span>-indium tin oxide/<span class="hlt">p</span>-copper indium oxide <span class="hlt">diode</span> structures were fabricated on quartz substrates by plasma vapor deposition using radio frequency (RF) magnetron sputtering. The <span class="hlt">p-n</span> heterojunction <span class="hlt">diodes</span> were highly transparent in the visible region and exhibited rectifying current-voltage (<span class="hlt">I</span>-V) characteristics with a good ideality factor. The sputter power during fabrication of the <span class="hlt">p</span>-layer was found to have a profound effect on <span class="hlt">I</span>-V characteristics, and the <span class="hlt">diode</span> with the <span class="hlt">p</span>-type layer deposited at a maximum power of 200 W exhibited the highest value of the <span class="hlt">diode</span> ideality factor (η value) of 2.162, which suggests its potential use in optoelectronic applications. The ratio of forward current to reverse current exceeded 80 within the range of applied voltages of -1.5 to +1.5 V in all cases. The <span class="hlt">diode</span> structure possessed an optical transmission of 60-70% in the visible region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015NIMPA.778...40A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015NIMPA.778...40A"><span>Focal-plane <span class="hlt">detector</span> system for the KATRIN experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Amsbaugh, J. F.; Barrett, J.; Beglarian, A.; Bergmann, T.; Bichsel, H.; Bodine, L. I.; Bonn, J.; Boyd, N. M.; Burritt, T. H.; Chaoui, Z.; Chilingaryan, S.; Corona, T. J.; Doe, P. J.; Dunmore, J. A.; Enomoto, S.; Formaggio, J. A.; Fränkle, F. M.; Furse, D.; Gemmeke, H.; Glück, F.; Harms, F.; Harper, G. C.; Hartmann, J.; Howe, M. A.; Kaboth, A.; Kelsey, J.; Knauer, M.; Kopmann, A.; Leber, M. L.; Martin, E. L.; Middleman, K. J.; Myers, A. W.; Oblath, N. S.; Parno, D. S.; Peterson, D. A.; Petzold, L.; Phillips, D. G.; Renschler, P.; Robertson, R. G. H.; Schwarz, J.; Steidl, M.; Tcherniakhovski, D.; Thümmler, T.; Van Wechel, T. D.; VanDevender, B. A.; Vöcking, S.; Wall, B. L.; Wierman, K. L.; Wilkerson, J. F.; Wüstling, S.</p> <p>2015-04-01</p> <p>The focal-plane <span class="hlt">detector</span> system for the KArlsruhe TRItium Neutrino (KATRIN) experiment consists of a multi-pixel silicon <span class="hlt">p-i-n-diode</span> array, custom readout electronics, two superconducting solenoid magnets, an ultra high-vacuum system, a high-vacuum system, calibration and monitoring devices, a scintillating veto, and a custom data-acquisition system. It is designed to detect the low-energy electrons selected by the KATRIN main spectrometer. We describe the system and summarize its performance after its final installation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APExp..10l1005L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APExp..10l1005L"><span>Low-threshold voltage ultraviolet light-emitting <span class="hlt">diodes</span> based on (Al,Ga)<span class="hlt">N</span> metal-insulator-semiconductor structures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liang, Yu-Han; Towe, Elias</p> <p>2017-12-01</p> <p>Al-rich III-nitride-based deep-ultraviolet (UV) (275-320 nm) light-emitting <span class="hlt">diodes</span> are plagued with a low emission efficiency and high turn-on voltages. We report Al-rich (Al,Ga)<span class="hlt">N</span> metal-insulator-semiconductor UV light-emitting Schottky <span class="hlt">diodes</span> with low turn-on voltages of <3 V, which are about half those of typical (Al,Ga)<span class="hlt">N</span> <span class="hlt">p-i-n</span> <span class="hlt">diodes</span>. Our devices use a thin Al<span class="hlt">N</span> film as the insulator and an <span class="hlt">n</span>-type Al0.58Ga0.42<span class="hlt">N</span> film as the semiconductor. To improve the efficiency, we inserted a Ga<span class="hlt">N</span> quantum-well structure between the Al<span class="hlt">N</span> insulator and the <span class="hlt">n</span>-type Al x Ga1- x <span class="hlt">N</span> semiconductor. The benefits of the quantum-well structure include the potential to tune the emission wavelength and the capability to confine carriers for more efficient radiative recombination.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhD...50X5109A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhD...50X5109A"><span>Dc and ac electrical response of MOCVD grown Ga<span class="hlt">N</span> in <span class="hlt">p-i-n</span> structure, assessed through <span class="hlt">I</span>-V and admittance measurement</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ayarcı Kuruoğlu, Neslihan; Özdemir, Orhan; Bozkurt, Kutsal; Sundaram, Suresh; Salvestrini, Jean-Paul; Ougazzaden, Abdallah; Gaimard, Quentin; Belahsene, Sofiane; Merghem, Kamel; Ramdane, Abderrahim</p> <p>2017-12-01</p> <p>The electrical response of gallium nitride (Ga<span class="hlt">N</span>), produced through metal-organic chemical vapor deposition in a <span class="hlt">p-i-n</span> structure was investigated through temperature-dependent current-voltage (<span class="hlt">I</span>-V) and admittance measurement. The <span class="hlt">I</span>-V curves showed double <span class="hlt">diode</span> behavior together with several distinct regions in which trap-assisted tunnelling current has been identified at low and moderate forward/reverse direction and space charge limited current (SCLC) at large forward/reverse bias. The value of extracted energy (˜200 meV in forward and  ˜70 meV in reverse direction) marked the tunnelling entity as electron and heavy hole in the present structure. These values were also obtained in space charge limited regime and considered as minority carriers which might originate the experimentally observed negative capacitance issue at low frequencies over the junction under both forward and reverse bias directions. Analytically derived expression for the admittance in the revised versions of SCLC model was also applied to explain the inductance effect, yielding good fits to the experimentally measured admittance data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009JAP...106g3717C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009JAP...106g3717C"><span>Temperature dependence of current-voltage characteristics in highly doped Ag/<span class="hlt">p-GaN</span>/In Schottky <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ćınar, K.; Yıldırım, N.; Coşkun, C.; Turut, A.</p> <p>2009-10-01</p> <p>To obtain detailed information about the conduction process of the Ag/<span class="hlt">p-GaN</span> Schottky <span class="hlt">diodes</span> (SDs) fabricated by us, we measured the <span class="hlt">I</span>-V characteristics over the temperature range of 80-360 K by the steps of 20 K. The slope of the linear portion of the forward bias <span class="hlt">I</span>-V plot and nkT =E0 of the device remained almost unchanged as independent of temperature with an average of 25.71±0.90 V-1 and 41.44±1.38 meV, respectively. Therefore, it can be said that the experimental <span class="hlt">I</span>-V data quite well obey the field emission model rather than the thermionic emission or thermionic field emission model. The study is a very good experimental example for the FE model. Furthermore, the reverse bias saturation current ranges from 8.34×10-8 A at 80 K to 2.10×10-7 A at 360 K, indicating that the charge transport mechanism in the Ag/<span class="hlt">p-GaN</span> SD is tunneling due to the weak temperature dependence of the saturation current. The possible origin of high experimental characteristic tunneling energy of E00=39 meV, which is ten times larger than possible theoretical value of 3.89 meV, is attributed to the accumulation of a large amount of defect states near the Ga<span class="hlt">N</span> surface or to the deep level defect band induced by high doping or to any mechanism which enhances the electric field and the state density at the semiconductor surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApSS..428.1010A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApSS..428.1010A"><span>Experimental and computational investigation of graphene/SAMs/<span class="hlt">n</span>-Si Schottky <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aydin, H.; Bacaksiz, C.; Yagmurcukardes, N.; Karakaya, C.; Mermer, O.; Can, M.; Senger, R. T.; Sahin, H.; Selamet, Y.</p> <p>2018-01-01</p> <p>We have investigated the effect of two different self-assembled monolayers (SAMs) on electrical characteristics of bilayer graphene (BLG)/<span class="hlt">n</span>-Si Schottky <span class="hlt">diodes</span>. Novel 4″bis(diphenylamino)-1, 1‧:3″-terphenyl-5‧ carboxylic acids (TPA) and 4,4-di-9H-carbazol-9-yl-1,1‧:3‧1‧-terphenyl-5‧ carboxylic acid (CAR) aromatic SAMs have been used to modify <span class="hlt">n</span>-Si surfaces. Cyclic voltammetry (CV) and Kelvin probe force microscopy (KPFM) results have been evaluated to verify the modification of <span class="hlt">n</span>-Si surface. The current-voltage (<span class="hlt">I</span>-V) characteristics of bare and SAMs modified devices show rectification behaviour verifying a Schottky junction at the interface. The ideality factors (<span class="hlt">n</span>) from ln(<span class="hlt">I</span>)-V dependences were determined as 2.13, 1.96 and 2.07 for BLG/<span class="hlt">n</span>-Si, BLG/TPA/<span class="hlt">n</span>-Si and BLG/CAR/<span class="hlt">n</span>-Si Schottky <span class="hlt">diodes</span>, respectively. In addition, Schottky barrier height (SBH) and series resistance (Rs) of SAMs modified <span class="hlt">diodes</span> were decreased compared to bare <span class="hlt">diode</span> due to the formation of a compatible interface between graphene and Si as well as π-π interaction between aromatic SAMs and graphene. The CAR-based device exhibits better <span class="hlt">diode</span> characteristic compared to the TPA-based device. Computational simulations show that the BLG/CAR system exhibits smaller energy-level-differences than the BLG/TPA, which supports the experimental findings of a lower Schottky barrier and series resistance in BLG/CAR <span class="hlt">diode</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApPhL.110r1102N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhL.110r1102N"><span>Ultraviolet light-absorbing and emitting <span class="hlt">diodes</span> consisting of a <span class="hlt">p</span>-type transparent-semiconducting NiO film deposited on an <span class="hlt">n</span>-type Ga<span class="hlt">N</span> homoepitaxial layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nakai, Hiroshi; Sugiyama, Mutsumi; Chichibu, Shigefusa F.</p> <p>2017-05-01</p> <p>Gallium nitride (Ga<span class="hlt">N</span>) and related (Al,Ga,In)<span class="hlt">N</span> alloys provide practical benefits in the production of light-emitting <span class="hlt">diodes</span> (LEDs) and laser <span class="hlt">diodes</span> operating in ultraviolet (UV) to green wavelength regions. However, obtaining low resistivity <span class="hlt">p</span>-type Al<span class="hlt">N</span> or AlGa<span class="hlt">N</span> of large bandgap energies (Eg) is a critical issue in fabricating UV and deep UV-LEDs. NiO is a promising candidate for useful <span class="hlt">p</span>-type transparent-semiconducting films because its Eg is 4.0 eV and it can be doped into <span class="hlt">p</span>-type conductivity of sufficiently low resistivity. By using these technologies, heterogeneous junction <span class="hlt">diodes</span> consisting of a <span class="hlt">p</span>-type transparent-semiconducting polycrystalline NiO film on an <span class="hlt">n</span>-type single crystalline Ga<span class="hlt">N</span> epilayer on a low threading-dislocation density, free-standing Ga<span class="hlt">N</span> substrate were fabricated. The NiO film was deposited by using the conventional RF-sputtering method, and the Ga<span class="hlt">N</span> homoepitaxial layer was grown by metalorganic vapor phase epitaxy. They exhibited a significant photovoltaic effect under UV light and also exhibited an electroluminescence peak at 3.26 eV under forward-biased conditions. From the conduction and valence band (EV) discontinuities, the NiO/Ga<span class="hlt">N</span> heterointerface is assigned to form a staggered-type (TYPE-II) band alignment with the EV of NiO higher by 2.0 eV than that of Ga<span class="hlt">N</span>. A rectifying property that is consistent with the proposed band diagram was observed in the current-voltage characteristics. These results indicate that polycrystalline NiO functions as a hole-extracting and injecting layer of UV optoelectronic devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11128310','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11128310"><span>Comparative dosimetry of <span class="hlt">diode</span> and diamond <span class="hlt">detectors</span> in electron beams for intraoperative radiation therapy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Björk, P; Knöös, T; Nilsson, P</p> <p>2000-11-01</p> <p>The aim of the present study is to examine the validity of using silicon semiconductor <span class="hlt">detectors</span> in degraded electron beams with a broad energy spectrum and a wide angular distribution. A comparison is made with diamond <span class="hlt">detector</span> measurements, which is the dosimeter considered to give the best results provided that dose rate effects are corrected for. Two-dimensional relative absorbed dose distributions in electron beams (6-20 MeV) for intraoperative radiation therapy (IORT) are measured in a water phantom. To quantify deviations between the <span class="hlt">detectors</span>, a dose comparison tool that simultaneously examines the dose difference and distance to agreement (DTA) is used to evaluate the results in low- and high-dose gradient regions, respectively. Uncertainties of the experimental measurement setup (+/- 1% and +/- 0.5 mm) are taken into account by calculating a composite distribution that fails this dose-difference and DTA acceptance limit. Thus, the resulting area of disagreement should be related to differences in <span class="hlt">detector</span> performance. The dose distributions obtained with the <span class="hlt">diode</span> are generally in very good agreement with diamond <span class="hlt">detector</span> measurements. The buildup region and the dose falloff region show good agreement with increasing electron energy, while the region outside the radiation field close to the water surface shows an increased difference with energy. The small discrepancies in the composite distributions are due to several factors: (a) variation of the silicon-to-water collision stopping-power ratio with electron energy, (b) a more pronounced directional dependence for <span class="hlt">diodes</span> than for diamonds, and (c) variation of the electron fluence perturbation correction factor with depth. For all investigated treatment cones and energies, the deviation is within dose-difference and DTA acceptance criteria of +/- 3% and +/- 1 mm, respectively. Therefore, <span class="hlt">p</span>-type silicon <span class="hlt">diodes</span> are well suited, in the sense that they give results in close agreement with diamond <span class="hlt">detectors</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740007032','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740007032"><span>Short range laser obstacle <span class="hlt">detector</span>. [for surface vehicles using laser <span class="hlt">diode</span> array</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kuriger, W. L. (Inventor)</p> <p>1973-01-01</p> <p>A short range obstacle <span class="hlt">detector</span> for surface vehicles is described which utilizes an array of laser <span class="hlt">diodes</span>. The <span class="hlt">diodes</span> operate one at a time, with one <span class="hlt">diode</span> for each adjacent azimuth sector. A vibrating mirror a short distance above the surface provides continuous scanning in elevation for all azimuth sectors. A <span class="hlt">diode</span> laser is synchronized with the vibrating mirror to enable one <span class="hlt">diode</span> laser to be fired, by pulses from a clock pulse source, a number of times during each elevation scan cycle. The time for a given pulse of light to be reflected from an obstacle and received is detected as a measure of range to the obstacle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1338497','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1338497"><span>Focal-plane <span class="hlt">detector</span> system for the KATRIN experiment</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Amsbaugh, J. F.; Barrett, J.; Beglarian, A.</p> <p></p> <p>Here, the local plane <span class="hlt">detector</span> system for the KArlsiuhe TRItium Neutrino (KATRIN) experiment consists of a multi-pixel silicon <span class="hlt">p-i-n-diode</span> array, custom readout electronics, two superconducting solenoid magnets, an ultra high vacuum system, a high vacuum system, calibration and monitoring devices, a scintillating veto, and a custom data-acquisition system, It is designed to detect the low-energy electrons selected by the KATRIN main spectrometer. We describe the system and summarize its performance after its final installation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1338497-focal-plane-detector-system-katrin-experiment','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1338497-focal-plane-detector-system-katrin-experiment"><span>Focal-plane <span class="hlt">detector</span> system for the KATRIN experiment</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Amsbaugh, J. F.; Barrett, J.; Beglarian, A.; ...</p> <p>2015-01-09</p> <p>Here, the local plane <span class="hlt">detector</span> system for the KArlsiuhe TRItium Neutrino (KATRIN) experiment consists of a multi-pixel silicon <span class="hlt">p-i-n-diode</span> array, custom readout electronics, two superconducting solenoid magnets, an ultra high vacuum system, a high vacuum system, calibration and monitoring devices, a scintillating veto, and a custom data-acquisition system, It is designed to detect the low-energy electrons selected by the KATRIN main spectrometer. We describe the system and summarize its performance after its final installation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26827340','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26827340"><span>Performance evaluation of a lossy transmission lines based <span class="hlt">diode</span> <span class="hlt">detector</span> at cryogenic temperature.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Villa, E; Aja, B; de la Fuente, L; Artal, E</p> <p>2016-01-01</p> <p>This work is focused on the design, fabrication, and performance analysis of a square-law Schottky <span class="hlt">diode</span> <span class="hlt">detector</span> based on lossy transmission lines working under cryogenic temperature (15 K). The design analysis of a microwave <span class="hlt">detector</span>, based on a planar gallium-arsenide low effective Schottky barrier height <span class="hlt">diode</span>, is reported, which is aimed for achieving large input return loss as well as flat sensitivity versus frequency. The designed circuit demonstrates good sensitivity, as well as a good return loss in a wide bandwidth at Ka-band, at both room (300 K) and cryogenic (15 K) temperatures. A good sensitivity of 1000 mV/mW and input return loss better than 12 dB have been achieved when it works as a zero-bias Schottky <span class="hlt">diode</span> <span class="hlt">detector</span> at room temperature, increasing the sensitivity up to a minimum of 2200 mV/mW, with the need of a DC bias current, at cryogenic temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19198463','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19198463"><span>Improved light extraction efficiency in Ga<span class="hlt">N</span>-based light emitting <span class="hlt">diode</span> by nano-scale roughening of <span class="hlt">p-GaN</span> surface.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Park, Sang Jae; Sadasivam, Karthikeyan Giri; Chung, Tae Hoon; Hong, Gi Cheol; Kim, Jin Bong; Kim, Sang Mook; Park, Si-Hyun; Jeon, Seong-Ran; Lee, June Key</p> <p>2008-10-01</p> <p>Improvement in light extraction efficiency of Ultra Violet-Light Emitting <span class="hlt">Diode</span> (UV-LED) is achieved by nano-scale roughening of <span class="hlt">p</span>-type Gallium Nitride (<span class="hlt">p-GaN</span>) surface. The process of surface roughening is carried out by using self assembled gold (Au) nano-clusters with support of nano-size silicon-oxide (SiO2) pillars on <span class="hlt">p-GaN</span> surface as a dry etching mask and by <span class="hlt">p-GaN</span> regrowth in the regions not covered by the mask after dry etching. Au nano-clusters are formed by rapid thermal annealing (RTA) process carried out at 600 degrees C for 1 min using 15 nm thick Au layer on top of SiO2. The <span class="hlt">p-GaN</span> roughness is controlled by <span class="hlt">p-GaN</span> regrowth time. Four different time values of 15 sec, 30 sec, 60 sec and 120 sec are considered for <span class="hlt">p-GaN</span> regrowth. Among the four different <span class="hlt">p-GaN</span> regrowth time values 30 sec regrown <span class="hlt">p-GaN</span> sample has the optimum roughness to increase the electroluminescence (EL) intensity to a value approximately 60% higher than the EL intensity of a conventional LED.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26434582','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26434582"><span>Enhancement of the Si <span class="hlt">p-n</span> <span class="hlt">diode</span> NIR photoresponse by embedding β-FeSi2 nanocrystallites.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shevlyagin, A V; Goroshko, D L; Chusovitin, E A; Galkin, K N; Galkin, N G; Gutakovskii, A K</p> <p>2015-10-05</p> <p>By using solid phase epitaxy of thin Fe films and molecular beam epitaxy of Si, a <span class="hlt">p(+)-Si/p</span>-Si/β-FeSi2 nanocrystallites/<span class="hlt">n</span>-Si(111) <span class="hlt">diode</span> structure was fabricated. Transmission electron microscopy data confirmed a well-defined multilayered structure with embedded nanocrystallites of two typical sizes: 3-4 and 15-20 nm, and almost coherent epitaxy of the nanocrystallites with the Si matrix. The <span class="hlt">diode</span> at zero bias conditions exhibited a current responsivity of 1.7 mA/W, an external quantum efficiency of about 0.2%, and a specific detectivity of 1.2 × 10(9) cm × Hz(1/2)/W at a wavelength of 1300 nm at room temperature. In the avalanche mode, the responsivity reached up to 20 mA/W (2% in terms of efficiency) with a value of avalanche gain equal to 5. The data obtained indicate that embedding of β-FeSi2 nanocrystallites into the depletion region of the Si <span class="hlt">p-n</span> junction results in expansion of the spectral sensitivity up to 1600 nm and an increase of the photoresponse by more than two orders of magnitude in comparison with a conventional Si <span class="hlt">p-n</span> junction. Thereby, fabricated structure combines advantage of the silicon photodiode functionality and simplicity with near infrared light detection capability of β-FeSi2.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015NIMPB.365..163G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015NIMPB.365..163G"><span>Modeling of radiation damage recovery in particle <span class="hlt">detectors</span> based on Ga<span class="hlt">N</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gaubas, E.; Ceponis, T.; Pavlov, J.</p> <p>2015-12-01</p> <p>The pulsed characteristics of the capacitor-type and PIN <span class="hlt">diode</span> type <span class="hlt">detectors</span> based on Ga<span class="hlt">N</span> have been simulated using the dynamic and drift-diffusion models. The drift-diffusion current simulations have been implemented by employing the commercial software package Synopsys TCAD Sentaurus. The bipolar drift regime has been analyzed. The possible internal gain in charge collection through carrier multiplication processes determined by impact ionization has been considered in order to compensate carrier lifetime reduction due to radiation defects introduced into Ga<span class="hlt">N</span> material of <span class="hlt">detector</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JaJAP..52hJK12K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JaJAP..52hJK12K"><span>Lateral Hydrogen Diffusion at <span class="hlt">p-GaN</span> Layers in Nitride-Based Light Emitting <span class="hlt">Diodes</span> with Tunnel Junctions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kuwano, Yuka; Kaga, Mitsuru; Morita, Takatoshi; Yamashita, Kouji; Yagi, Kouta; Iwaya, Motoaki; Takeuchi, Tetsuya; Kamiyama, Satoshi; Akasaki, Isamu</p> <p>2013-08-01</p> <p>We demonstrated lateral Mg activation along <span class="hlt">p-GaN</span> layers underneath <span class="hlt">n-GaN</span> surface layers in nitride-based light emitting <span class="hlt">diodes</span> (LEDs) with GaIn<span class="hlt">N</span> tunnel junctions. A high temperature thermal annealing was effective for the lateral Mg activation when the <span class="hlt">p-GaN</span> layers were partly exposed to an oxygen ambient as etched sidewalls. The activated regions gradually extended from the etched sidewalls to the centers with an increase of annealing time, observed as emission regions with current injection. These results suggest that hydrogen diffuses not vertically thorough the above <span class="hlt">n-GaN</span> but laterally through the exposed portions of the <span class="hlt">p-GaN</span>. The lowest voltage drop at the GaIn<span class="hlt">N</span> tunnel junction was estimated to be 0.9 V at 50 mA with the optimized annealing condition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ApPhL..97a3101L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ApPhL..97a3101L"><span>Color tunable light-emitting <span class="hlt">diodes</span> based on <span class="hlt">p+-Si/p</span>-CuAlO2/<span class="hlt">n</span>-ZnO nanorod array heterojunctions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ling, Bo; Zhao, Jun Liang; Sun, Xiao Wei; Tan, Swee Tiam; Kyaw, Aung Ko Ko; Divayana, Yoga; Dong, Zhi Li</p> <p>2010-07-01</p> <p>Wide-range color tuning from red to blue was achieved in phosphor-free <span class="hlt">p+-Si/p</span>-CuAlO2/<span class="hlt">n</span>-ZnO nanorod light-emitting <span class="hlt">diodes</span> at room temperature. CuAlO2 films were deposited on <span class="hlt">p</span>+-Si substrates by sputtering followed by annealing. ZnO nanorods were further grown on the annealed <span class="hlt">p+-Si/p</span>-CuAlO2 substrates by vapor phase transport. The color of the <span class="hlt">p</span>-CuAlO2/<span class="hlt">n</span>-ZnO nanorod array heterojunction electroluminescence depended on the annealing temperature of the CuAlO2 film. With the increase of the annealing temperature from 900 to 1050 °C, the emission showed a blueshift under the same forward bias. The origin of the blueshift is related to the amount of Cu concentration diffused into ZnO.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_8 --> <div id="page_9" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="161"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19870019008','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19870019008"><span>Development of a <span class="hlt">P-I-N</span> HgCdTe photomixer for laser heterodyne spectrometry</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bratt, Peter R.</p> <p>1987-01-01</p> <p>An improved HgCdTe photomixer technology was demonstrated employing a <span class="hlt">p-i-n</span> photodiode structure. The <span class="hlt">i</span>-region was near intrinsic <span class="hlt">n</span>-type HgCdTe; the <span class="hlt">n</span>-region was formed by B+ ion implantation; and the <span class="hlt">p</span>-region was formed either by a shallow Au diffusion or by a Pt Schottky barrier. Experimental devices in a back-side illuminated mesa <span class="hlt">diode</span> configuration were fabricated, tested, and delivered. The best photomixer was packaged in a 24-hour LN2 dewar along with a cooled GaAs FET preamplifier. Testing was performed by mixing black-body radiation with a CO2 laser beam and measuring the IF signal, noise, and signal-to-noise ratio in the GHz frequency range. Signal bandwidth for this photomixer was 1.3 GHz. The heterodyne NEP was 4.4 x 10 to the -20 W/Hz out to 1 GHz increasing to 8.6 x 10 to the -10 W/Hz at 2 GHz. Other photomixers delivered on this program had heterodyne NEPs at 1 GHz ranging from 8 x 10 to the -20 to 4.4 x 10 to the -19 W/Hz and NEP bandwidths from 2 to 4 GHz.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25350523','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25350523"><span><span class="hlt">p-i-n</span> heterojunctions with BiFeO3 perovskite nanoparticles and <span class="hlt">p</span>- and <span class="hlt">n</span>-type oxides: photovoltaic properties.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chatterjee, Soumyo; Bera, Abhijit; Pal, Amlan J</p> <p>2014-11-26</p> <p>We formed <span class="hlt">p-i-n</span> heterojunctions based on a thin film of BiFeO3 nanoparticles. The perovskite acting as an intrinsic semiconductor was sandwiched between a <span class="hlt">p</span>-type and an <span class="hlt">n</span>-type oxide semiconductor as hole- and electron-collecting layer, respectively, making the heterojunction act as an all-inorganic oxide <span class="hlt">p-i-n</span> device. We have characterized the perovskite and carrier collecting materials, such as NiO and MoO3 nanoparticles as <span class="hlt">p</span>-type materials and ZnO nanoparticles as the <span class="hlt">n</span>-type material, with scanning tunneling spectroscopy; from the spectrum of the density of states, we could locate the band edges to infer the nature of the active semiconductor materials. The energy level diagram of <span class="hlt">p-i-n</span> heterojunctions showed that type-II band alignment formed at the <span class="hlt">p-i</span> and <span class="hlt">i-n</span> interfaces, favoring carrier separation at both of them. We have compared the photovoltaic properties of the perovskite in <span class="hlt">p-i-n</span> heterojunctions and also in <span class="hlt">p-i</span> and <span class="hlt">i-n</span> junctions. From current-voltage characteristics and impedance spectroscopy, we have observed that two depletion regions were formed at the <span class="hlt">p-i</span> and <span class="hlt">i-n</span> interfaces of a <span class="hlt">p-i-n</span> heterojunction. The two depletion regions operative at <span class="hlt">p-i-n</span> heterojunctions have yielded better photovoltaic properties as compared to devices having one depletion region in the <span class="hlt">p-i</span> or the <span class="hlt">i-n</span> junction. The results evidenced photovoltaic devices based on all-inorganic oxide, nontoxic, and perovskite materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011APExp...4i2105F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011APExp...4i2105F"><span>AlGa<span class="hlt">N</span>-Cladding-Free m-Plane InGa<span class="hlt">N/GaN</span> Laser <span class="hlt">Diodes</span> with <span class="hlt">p</span>-Type AlGa<span class="hlt">N</span> Etch Stop Layers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Farrell, Robert M.; Haeger, Daniel A.; Hsu, Po Shan; Hardy, Matthew T.; Kelchner, Kathryn M.; Fujito, Kenji; Feezell, Daniel F.; Mishra, Umesh K.; DenBaars, Steven P.; Speck, James S.; Nakamura, Shuji</p> <p>2011-09-01</p> <p>We present a new method of improving the accuracy and reproducibility of dry etching processes for ridge waveguide InGa<span class="hlt">N/GaN</span> laser <span class="hlt">diodes</span> (LDs). A Ga<span class="hlt">N</span>:Al0.09Ga0.91<span class="hlt">N</span> etch rate selectivity of 11:1 was demonstrated for an m-plane LD with a 40 nm <span class="hlt">p</span>-Al0.09Ga0.91<span class="hlt">N</span> etch stop layer (ESL) surrounded by Al-free cladding layers, establishing the effectiveness of AlGa<span class="hlt">N</span>-based ESLs for controlling etch depth in ridge waveguide InGa<span class="hlt">N/GaN</span> LDs. These results demonstrate the potential for integrating AlGa<span class="hlt">N</span> ESLs into commercial device designs where accurate control of the etch depth of the ridge waveguide is necessary for stable, kink-free operation at high output powers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SPIE.7834E..0MR','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SPIE.7834E..0MR"><span>MCT (HgCdTe) IR <span class="hlt">detectors</span>: latest developments in France</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Reibel, Yann; Rubaldo, Laurent; Vaz, Cedric; Tribolet, Philippe; Baier, Nicolas; Destefanis, Gérard</p> <p>2010-10-01</p> <p>This paper presents an overview of the very recent developments of the MCT infrared <span class="hlt">detector</span> technology developed by CEA-LETI and Sofradir in France. New applications require high sensitivity, higher operating temperature and dual band <span class="hlt">detectors</span>. The standard <span class="hlt">n</span> on <span class="hlt">p</span> technology in production at Sofradir for 25 years is well mastered with an extremely robust and reliable process. Sofradir's interest in <span class="hlt">p</span> on <span class="hlt">n</span> technology opens the perspective of reducing dark current of <span class="hlt">diodes</span> so <span class="hlt">detectors</span> could operate in lower flux or higher operating temperature. In parallel, MCT Avalanche Photo <span class="hlt">Diodes</span> (APD) have demonstrated ideal performances for low flux and high speed application like laser gated imaging during the last few years. This technology also opens new prospects on next generation of imaging <span class="hlt">detectors</span> for compact, low flux and low power applications. Regarding 3rd Gen IR <span class="hlt">detectors</span>, the development of dual-band infrared <span class="hlt">detectors</span> has been the core of intense research and technological improvements for the last ten years. New TV (640 x 512 pixels) format MWIR/LWIR <span class="hlt">detectors</span> on 20μm pixel pitch, made from Molecular Beam Epitaxy, has been developed with dedicated Read-Out Integrated Circuit (ROIC) for real simultaneous detection and maximum SNR. Technological and products achievements, as well as latest results and performances are presented outlining the availability of <span class="hlt">p/n</span>, avalanche photodiodes and dual band technologies for new applications at system level.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApPhL.109j1103J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApPhL.109j1103J"><span>Reverse-bias-driven dichromatic electroluminescence of <span class="hlt">n</span>-ZnO wire arrays/<span class="hlt">p-GaN</span> film heterojunction light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jeong, Junseok; Choi, Ji Eun; Kim, Yong-Jin; Hwang, Sunyong; Kim, Sung Kyu; Kim, Jong Kyu; Jeong, Hu Young; Hong, Young Joon</p> <p>2016-09-01</p> <p>Position-controlled <span class="hlt">n</span>-ZnO microwire (MW) and nanowire-bundle (NW-B) arrays were fabricated using hydrothermal growth of ZnO on a patterned <span class="hlt">p-GaN</span> film. Both the wire/film <span class="hlt">p-n</span> heterojunctions showed electrical rectification features at reverse-bias (rb) voltages, analogous to backward <span class="hlt">diodes</span>. Dichromatic electroluminescence (EL) emissions with 445- and 560-nm-wavelength peaks displayed whitish-blue and greenish-yellow light from MW- and NW-B-based heterojunctions at rb voltages, respectively. The different dichromatic EL emission colors were studied based on photoluminescence spectra and the dichromatic EL peak intensity ratios as a function of the rb voltage. The different EL colors are discussed with respect to depletion thickness and electron tunneling probability determined by wire/film junction geometry and size.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22488786-simplified-gas-sensor-model-based-algan-gan-heterostructure-schottky-diode','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22488786-simplified-gas-sensor-model-based-algan-gan-heterostructure-schottky-diode"><span>Simplified gas sensor model based on AlGa<span class="hlt">N/GaN</span> heterostructure Schottky <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Das, Subhashis, E-mail: subhashis.ds@gmail.com; Majumdar, S.; Kumar, R.</p> <p>2015-08-28</p> <p>Physics based modeling of AlGa<span class="hlt">N/GaN</span> heterostructure Schottky <span class="hlt">diode</span> gas sensor has been investigated for high sensitivity and linearity of the device. Here the surface and heterointerface properties are greatly exploited. The dependence of two dimensional electron gas (2DEG) upon the surface charges is mainly utilized. The simulation of Schottky <span class="hlt">diode</span> has been done in Technology Computer Aided Design (TCAD) tool and <span class="hlt">I</span>-V curves are generated, from the <span class="hlt">I</span>-V curves 76% response has been recorded in presence of 500 ppm gas at a biasing voltage of 0.95 Volt.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5103186','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5103186"><span>Trap-mediated electronic transport properties of gate-tunable pentacene/MoS2 <span class="hlt">p-n</span> heterojunction <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kim, Jae-Keun; Cho, Kyungjune; Kim, Tae-Young; Pak, Jinsu; Jang, Jingon; Song, Younggul; Kim, Youngrok; Choi, Barbara Yuri; Chung, Seungjun; Hong, Woong-Ki; Lee, Takhee</p> <p>2016-01-01</p> <p>We investigated the trap-mediated electronic transport properties of pentacene/molybdenum disulphide (MoS2) <span class="hlt">p-n</span> heterojunction devices. We observed that the hybrid <span class="hlt">p-n</span> heterojunctions were gate-tunable and were strongly affected by trap-assisted tunnelling through the van der Waals gap at the heterojunction interfaces between MoS2 and pentacene. The pentacene/MoS2 <span class="hlt">p-n</span> heterojunction <span class="hlt">diodes</span> had gate-tunable high ideality factor, which resulted from trap-mediated conduction nature of devices. From the temperature-variable current-voltage measurement, a space-charge-limited conduction and a variable range hopping conduction at a low temperature were suggested as the gate-tunable charge transport characteristics of these hybrid <span class="hlt">p-n</span> heterojunctions. Our study provides a better understanding of the trap-mediated electronic transport properties in organic/2-dimensional material hybrid heterojunction devices. PMID:27829663</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NatSR...636775K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NatSR...636775K"><span>Trap-mediated electronic transport properties of gate-tunable pentacene/MoS2 <span class="hlt">p-n</span> heterojunction <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, Jae-Keun; Cho, Kyungjune; Kim, Tae-Young; Pak, Jinsu; Jang, Jingon; Song, Younggul; Kim, Youngrok; Choi, Barbara Yuri; Chung, Seungjun; Hong, Woong-Ki; Lee, Takhee</p> <p>2016-11-01</p> <p>We investigated the trap-mediated electronic transport properties of pentacene/molybdenum disulphide (MoS2) <span class="hlt">p-n</span> heterojunction devices. We observed that the hybrid <span class="hlt">p-n</span> heterojunctions were gate-tunable and were strongly affected by trap-assisted tunnelling through the van der Waals gap at the heterojunction interfaces between MoS2 and pentacene. The pentacene/MoS2 <span class="hlt">p-n</span> heterojunction <span class="hlt">diodes</span> had gate-tunable high ideality factor, which resulted from trap-mediated conduction nature of devices. From the temperature-variable current-voltage measurement, a space-charge-limited conduction and a variable range hopping conduction at a low temperature were suggested as the gate-tunable charge transport characteristics of these hybrid <span class="hlt">p-n</span> heterojunctions. Our study provides a better understanding of the trap-mediated electronic transport properties in organic/2-dimensional material hybrid heterojunction devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27829663','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27829663"><span>Trap-mediated electronic transport properties of gate-tunable pentacene/MoS2 <span class="hlt">p-n</span> heterojunction <span class="hlt">diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Jae-Keun; Cho, Kyungjune; Kim, Tae-Young; Pak, Jinsu; Jang, Jingon; Song, Younggul; Kim, Youngrok; Choi, Barbara Yuri; Chung, Seungjun; Hong, Woong-Ki; Lee, Takhee</p> <p>2016-11-10</p> <p>We investigated the trap-mediated electronic transport properties of pentacene/molybdenum disulphide (MoS 2 ) <span class="hlt">p-n</span> heterojunction devices. We observed that the hybrid <span class="hlt">p-n</span> heterojunctions were gate-tunable and were strongly affected by trap-assisted tunnelling through the van der Waals gap at the heterojunction interfaces between MoS 2 and pentacene. The pentacene/MoS 2 <span class="hlt">p-n</span> heterojunction <span class="hlt">diodes</span> had gate-tunable high ideality factor, which resulted from trap-mediated conduction nature of devices. From the temperature-variable current-voltage measurement, a space-charge-limited conduction and a variable range hopping conduction at a low temperature were suggested as the gate-tunable charge transport characteristics of these hybrid <span class="hlt">p-n</span> heterojunctions. Our study provides a better understanding of the trap-mediated electronic transport properties in organic/2-dimensional material hybrid heterojunction devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16563854','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16563854"><span>Natural gas pipeline leak <span class="hlt">detector</span> based on NIR <span class="hlt">diode</span> laser absorption spectroscopy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gao, Xiaoming; Fan, Hong; Huang, Teng; Wang, Xia; Bao, Jian; Li, Xiaoyun; Huang, Wei; Zhang, Weijun</p> <p>2006-09-01</p> <p>The paper reports on the development of an integrated natural gas pipeline leak <span class="hlt">detector</span> based on <span class="hlt">diode</span> laser absorption spectroscopy. The <span class="hlt">detector</span> transmits a 1.653 microm DFB <span class="hlt">diode</span> laser with 10 mW and detects a fraction of the backscatter reflected from the topographic targets. To eliminate the effect of topographic scatter targets, a ratio detection technique was used. Wavelength modulation and harmonic detection were used to improve the detection sensitivity. The experimental detection limit is 50 ppmm, remote detection for a distance up to 20 m away topographic scatter target is demonstrated. Using a known simulative leak pipe, minimum detectable pipe leak flux is less than 10 ml/min.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhCS.707a2013S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhCS.707a2013S"><span>Investigation of the Electrical Characteristics of Al/<span class="hlt">p</span>-Si/Al Schottky <span class="hlt">Diode</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Şenarslan, Elvan; Güzeldir, Betül; Sağlam, Mustafa</p> <p>2016-04-01</p> <p>In this study, <span class="hlt">p</span>-type Si semiconductor wafer with (100) orientation, 400 μm thickness and 1-10 Ω cm resistivity was used. The Si wafer before making contacts were chemically cleaned with the Si cleaning procedure which for remove organic contaminations were ultrasonically cleaned at acetone and methanol for 10 min respectively and then rinsed in deionized water of 18 MΩ and dried with high purity <span class="hlt">N</span>2. Then respectively RCA1(<span class="hlt">i</span>.e., boiling in NH3+H2O2+6H2O for 10 min at 60°C ), RCA2 (<span class="hlt">i</span>.e., boiling in HCl+H2O2+6H2O for 10 min at 60°C ) cleaning procedures were applied and rinsed in deionized water followed by drying with a stream of <span class="hlt">N</span>2. After the cleaning process, the wafer is immediately inserted in to the coating unit. Ohmic contact was made by evaporating of Al on the non-polished side of the <span class="hlt">p</span>-Si wafer pieces under ~ 4,2 10-6 Torr pressure. After process evaporation, <span class="hlt">p</span>-Si with omic contac thermally annealed 580°C for 3 min in a quartz tube furnace in <span class="hlt">N</span>2. Then, the rectifier contact is made by evaporation Al metal diameter of about 1.0 mm on the polished surface of <span class="hlt">p</span>-Si in turbo molecular pump at about ~ 1 10-6 Torr. Consequently, Al/<span class="hlt">p</span>-Si/Al Schottky <span class="hlt">diode</span> was obtained. The <span class="hlt">I</span>-V measurements of this <span class="hlt">diode</span> performed by the use of a KEITLEY 487 Picoammeter/Voltage Source and the C-V measurements were performed with HP 4192A (50-13 MHz) LF Impedance Analyzer at room temperature and in dark.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApPhL.110c3506Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhL.110c3506Z"><span>Investigation of <span class="hlt">p</span>-type depletion doping for InGa<span class="hlt">N/GaN</span>-based light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Yiping; Zhang, Zi-Hui; Tan, Swee Tiam; Hernandez-Martinez, Pedro Ludwig; Zhu, Binbin; Lu, Shunpeng; Kang, Xue Jun; Sun, Xiao Wei; Demir, Hilmi Volkan</p> <p>2017-01-01</p> <p>Due to the limitation of the hole injection, <span class="hlt">p</span>-type doping is essential to improve the performance of InGa<span class="hlt">N/GaN</span> multiple quantum well light-emitting <span class="hlt">diodes</span> (LEDs). In this work, we propose and show a depletion-region Mg-doping method. Here we systematically analyze the effectiveness of different Mg-doping profiles ranging from the electron blocking layer to the active region. Numerical computations show that the Mg-doping decreases the valence band barrier for holes and thus enhances the hole transportation. The proposed depletion-region Mg-doping approach also increases the barrier height for electrons, which leads to a reduced electron overflow, while increasing the hole concentration in the <span class="hlt">p-GaN</span> layer. Experimentally measured external quantum efficiency indicates that Mg-doping position is vitally important. The doping in or adjacent to the quantum well degrades the LED performance due to Mg diffusion, increasing the corresponding nonradiative recombination, which is well supported by the measured carrier lifetimes. The experimental results are well numerically reproduced by modifying the nonradiative recombination lifetimes, which further validate the effectiveness of our approach.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999SSEle..43.1929P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999SSEle..43.1929P"><span>Deep centers in AlGa<span class="hlt">N</span>-based light emitting <span class="hlt">diode</span> structures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Polyakov, A. Y.; Smirnov, N. B.; Govorkov, A. V.; Mil'vidskii, M. G.; Usikov, A. S.; Pushnyi, B. V.; Lundin, W. V.</p> <p>1999-10-01</p> <p>Deep traps were studied in Ga<span class="hlt">N</span> homojunction and AlGa<span class="hlt">N/GaN</span> heterojunction light emitting <span class="hlt">diode</span> (LED) <span class="hlt">p-i-n</span> structures by means of deep levels transient spectroscopy (DLTS), admittance and electroluminescence (EL) spectra measurements. It is shown that, in homojunction LED structures, the EL spectra comes from recombination involving Mg acceptors in-diffusing into the active <span class="hlt">i</span>-layer. This Mg in-diffusion is strongly suppressed in heterostructures with the upper <span class="hlt">p</span>-type layer containing about 5% of Al. As a result the main peak in the EL spectra of heterostructures is shifted toward higher energy compared to homojunctions. Joint doping of the <span class="hlt">i</span>-layer with Zn and Si allows to shift the main EL peak to longer wavelength. The dominant electron traps observed in the studied LED structures had ionization energies of 0.55 and 0.85 eV. The dominant hole traps had apparent ionization energies of 0.85 and 0.4 eV. The latter traps were shown to be metastable and it is argued that they could be at least in part responsible for the persistent photoconductivity observed in <span class="hlt">p-GaN</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JAP...122x4504B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JAP...122x4504B"><span>Fabrication of 4H-SiC Pi<span class="hlt">N</span> <span class="hlt">diodes</span> without bipolar degradation by improved device processes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bu, Yuan; Yoshimoto, Hiroyuki; Watanabe, Naoki; Shima, Akio</p> <p>2017-12-01</p> <p>We developed a simple technology for fabricating bipolar degradation-free 6.5 kV SiC Pi<span class="hlt">N</span> <span class="hlt">diodes</span> on the basal plane dislocation (BPD)-free areas of commercially available 4H-SiC wafers. In order to suppress process-induced basal plane dislocation, we first investigated the causes of BPD generation during fabrication and then improved the processes. We found that no BPD was induced on a flat Si-face, but a large number of BPDs were concentrated in the mesa edge after high-dose Al ions were implanted [<span class="hlt">p</span>++ ion implantation (<span class="hlt">I</span>. <span class="hlt">I</span>.)] at room temperature (RT) followed by activation annealing. Therefore, we examined new technologies in device processes including (<span class="hlt">I</span>) long-term high-temperature oxidation after the mesa process to remove etching damage in the mesa edge and (II) reducing the Al dose (<span class="hlt">p</span>+ <span class="hlt">I</span>. <span class="hlt">I</span>.) in the mesa edge to suppress BPD generation. We investigated the effect of the Al dose in the mesa edge on BPD generation and bipolar degradation. The results indicated that no BPD appeared when the dose was lower than 1 × 1015 atoms/cm2 and when long-term high-temperature oxidation was applied after the mesa process. As a result, we successfully fabricated 6.5 kV Pi<span class="hlt">N</span> <span class="hlt">diodes</span> without bipolar degradation on BPD-free areas. Moreover, the <span class="hlt">diodes</span> are very stable when applying 270 A/cm2 for over 100 h. Photoluminescence (PL) observation indicated that no BPD was generated during the improved fabrication processes. Besides, the Ir-Vr measurements showed that the breakdown voltage was over 8 kV at RT. The leakage currents are as low as 7.6 × 10-5 mA/cm2 (25 °C) and 6.3 × 10-4 mA/cm2 (150 °C) at 6.5 kV. Moreover, this result is applicable not only for Pi<span class="hlt">N</span> <span class="hlt">diodes</span> but also for MOSFETs (body <span class="hlt">diode</span>), IGBTs, thyristors, etc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22492405-investigation-significantly-high-barrier-height-cu-gan-schottky-diode','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22492405-investigation-significantly-high-barrier-height-cu-gan-schottky-diode"><span>Investigation of significantly high barrier height in Cu/Ga<span class="hlt">N</span> Schottky <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Garg, Manjari, E-mail: meghagarg142@gmail.com; Kumar, Ashutosh; Singh, R.</p> <p>2016-01-15</p> <p>Current-voltage (<span class="hlt">I</span>-V) measurements combined with analytical calculations have been used to explain mechanisms for forward-bias current flow in Copper (Cu) Schottky <span class="hlt">diodes</span> fabricated on Gallium Nitride (Ga<span class="hlt">N</span>) epitaxial films. An ideality factor of 1.7 was found at room temperature (RT), which indicated deviation from thermionic emission (TE) mechanism for current flow in the Schottky <span class="hlt">diode</span>. Instead the current transport was better explained using the thermionic field-emission (TFE) mechanism. A high barrier height of 1.19 eV was obtained at room temperature. X-ray photoelectron spectroscopy (XPS) was used to investigate the plausible reason for observing Schottky barrier height (SBH) that is significantlymore » higher than as predicted by the Schottky-Mott model for Cu/Ga<span class="hlt">N</span> <span class="hlt">diodes</span>. XPS measurements revealed the presence of an ultrathin cuprous oxide (Cu{sub 2}O) layer at the interface between Cu and Ga<span class="hlt">N</span>. With Cu{sub 2}O acting as a degenerate <span class="hlt">p</span>-type semiconductor with high work function of 5.36 eV, a high barrier height of 1.19 eV is obtained for the Cu/Cu{sub 2}O/Ga<span class="hlt">N</span> Schottky <span class="hlt">diode</span>. Moreover, the ideality factor and barrier height were found to be temperature dependent, implying spatial inhomogeneity of barrier height at the metal semiconductor interface.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17252808','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17252808"><span>Nanoparticle embedded <span class="hlt">p</span>-type electrodes for Ga<span class="hlt">N</span>-based flip-chip light emitting <span class="hlt">diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kwak, Joon Seop; Song, J O; Seong, T Y; Kim, B I; Cho, J; Sone, C; Park, Y</p> <p>2006-11-01</p> <p>We have investigated high-quality ohmic contacts for flip-chip light emitting <span class="hlt">diodes</span> using Zn-Ni nanoparticles/Ag schemes. The Zn-Ni nanoparticles/Ag contacts produce specific contact resistances of 10(-5)-10(-6) omegacm2 when annealed at temperatures of 330-530 degrees C for 1 min in air ambient, which are much better than those obtained from the Ag contacts. It is shown that blue InGa<span class="hlt">N/GaN</span> multi-quantum well light emitting <span class="hlt">diodes</span> fabricated with the annealed Zn-Ni nanoparticles/Ag contacts give much lower forward-bias voltages at 20 mA compared with those of the multi-quantum well light emitting <span class="hlt">diodes</span> made with the as-deposited Ag contacts. It is further presented that the multi-quantum well light emitting <span class="hlt">diodes</span> made with the Zn-Ni nanoparticles/Ag contacts show similar output power compared to those fabricated with the Ag contact layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APExp...8f1302Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APExp...8f1302Q"><span>Influence of external mechanical stress on electrical properties of single-crystal <span class="hlt">n</span>-3C-SiC/<span class="hlt">p</span>-Si heterojunction <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Qamar, Afzaal; Veit Dao, Dzung; Tanner, Philip; Phan, Hoang-Phuong; Dinh, Toan; Dimitrijev, Sima</p> <p>2015-06-01</p> <p>This article reports for the first time the electrical properties of fabricated <span class="hlt">n</span>-3C-SiC/<span class="hlt">p</span>-Si heterojunction <span class="hlt">diodes</span> under external mechanical stress in the [110] direction. An anisotype heterojunction <span class="hlt">diode</span> of <span class="hlt">n</span>-3C-SiC/<span class="hlt">p</span>-Si was fabricated by depositing 3C-SiC onto the Si substrate by low-pressure chemical vapor deposition. The mechanical stress significantly affected the scaling current density of the heterojunction. The scaling current density increases with stress and is explained in terms of a band offset reduction at the SiC/Si interface under applied stress. A reduction in the barrier height across the junction owing to applied stress is also explained quantitatively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4593177','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4593177"><span>Enhancement of the Si <span class="hlt">p-n</span> <span class="hlt">diode</span> NIR photoresponse by embedding β-FeSi2 nanocrystallites</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Shevlyagin, A. V.; Goroshko, D. L.; Chusovitin, E. A.; Galkin, K. N.; Galkin, N. G.; Gutakovskii, A. K.</p> <p>2015-01-01</p> <p>By using solid phase epitaxy of thin Fe films and molecular beam epitaxy of Si, a <span class="hlt">p+-Si/p</span>-Si/β-FeSi2 nanocrystallites/<span class="hlt">n</span>-Si(111) <span class="hlt">diode</span> structure was fabricated. Transmission electron microscopy data confirmed a well-defined multilayered structure with embedded nanocrystallites of two typical sizes: 3–4 and 15–20 nm, and almost coherent epitaxy of the nanocrystallites with the Si matrix. The <span class="hlt">diode</span> at zero bias conditions exhibited a current responsivity of 1.7 mA/W, an external quantum efficiency of about 0.2%, and a specific detectivity of 1.2 × 109 cm × Hz1/2/W at a wavelength of 1300 nm at room temperature. In the avalanche mode, the responsivity reached up to 20 mA/W (2% in terms of efficiency) with a value of avalanche gain equal to 5. The data obtained indicate that embedding of β-FeSi2 nanocrystallites into the depletion region of the Si <span class="hlt">p-n</span> junction results in expansion of the spectral sensitivity up to 1600 nm and an increase of the photoresponse by more than two orders of magnitude in comparison with a conventional Si <span class="hlt">p-n</span> junction. Thereby, fabricated structure combines advantage of the silicon photodiode functionality and simplicity with near infrared light detection capability of β-FeSi2. PMID:26434582</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SPIE10532E..19S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SPIE10532E..19S"><span>Distributed feedback InGa<span class="hlt">N/GaN</span> laser <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Slight, Thomas J.; Watson, Scott; Yadav, Amit; Grzanka, Szymon; Stanczyk, Szymon; Docherty, Kevin E.; Rafailov, Edik; Perlin, Piotr; Najda, Steve; Leszczyński, Mike; Kelly, Anthony E.</p> <p>2018-02-01</p> <p>We have realised InGa<span class="hlt">N/GaN</span> distributed feedback laser <span class="hlt">diodes</span> emitting at a single wavelength in the 42X nm wavelength range. Laser <span class="hlt">diodes</span> based on Gallium Nitride (Ga<span class="hlt">N</span>) are useful devices in a wide range of applications including atomic spectroscopy, data storage and optical communications. To fully exploit some of these application areas there is a need for a Ga<span class="hlt">N</span> laser <span class="hlt">diode</span> with high spectral purity, e.g. in atomic clocks, where a narrow line width blue laser source can be used to target the atomic cooling transition. Previously, Ga<span class="hlt">N</span> DFB lasers have been realised using buried or surface gratings. Buried gratings require complex overgrowth steps which can introduce epi-defects. Surface gratings designs, can compromise the quality of the <span class="hlt">p</span>-type contact due to dry etch damage and are prone to increased optical losses in the grating regions. In our approach the grating is etched into the sidewall of the ridge. Advantages include a simpler fabrication route and design freedom over the grating coupling strength.Our intended application for these devices is cooling of the Sr+ ion and for this objective the laser characteristics of SMSR, linewidth, and power are critical. We investigate how these characteristics are affected by adjusting laser design parameters such as grating coupling coefficient and cavity length.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006SeScT..21.1699B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006SeScT..21.1699B"><span>Design, fabrication and characterization of an a-Si:H-based UV <span class="hlt">detector</span> for sunburn applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bayat, Khadijeh; Vygranenko, Yuriy; Sazonov, Andrei; Farrokh-Baroughi, Mahdi</p> <p>2006-12-01</p> <p>A thin-film a-Si:H pin <span class="hlt">detector</span> was developed for selective detection of UVA (320-400 nm) radiation. In order for the fabrication technology to be transferable onto flexible substrates, all of the processing steps were conducted at temperatures less than 125 °C. The measured saturation current as low as 2 <span class="hlt">p</span>A cm-2 and the ideality factor of 1.47 show that the pin <span class="hlt">diodes</span> have a good quality <span class="hlt">i</span>-layer as well as <span class="hlt">p-i</span> and <span class="hlt">n-i</span> interfaces. The film thicknesses were optimized to suppress the <span class="hlt">detector</span> sensitivity in the visible spectral range, and the peak of spectral response was observed at 410 nm. The selectivity estimated from the ratio of the photocurrent generated by UVA absorption to the total photocurrent is 21%.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_9 --> <div id="page_10" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="181"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26434984','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26434984"><span>Semiconductor-Insulator-Semiconductor <span class="hlt">Diode</span> Consisting of Monolayer MoS2, h-BN, and Ga<span class="hlt">N</span> Heterostructure.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jeong, Hyun; Bang, Seungho; Oh, Hye Min; Jeong, Hyeon Jun; An, Sung-Jin; Han, Gang Hee; Kim, Hyun; Kim, Ki Kang; Park, Jin Cheol; Lee, Young Hee; Lerondel, Gilles; Jeong, Mun Seok</p> <p>2015-10-27</p> <p>We propose a semiconductor-insulator-semiconductor (SIS) heterojunction <span class="hlt">diode</span> consisting of monolayer (1-L) MoS2, hexagonal boron nitride (h-BN), and epitaxial <span class="hlt">p-GaN</span> that can be applied to high-performance nanoscale optoelectronics. The layered materials of 1-L MoS2 and h-BN, grown by chemical vapor deposition, were vertically stacked by a wet-transfer method on a <span class="hlt">p-GaN</span> layer. The final structure was verified by confocal photoluminescence and Raman spectroscopy. Current-voltage (<span class="hlt">I</span>-V) measurements were conducted to compare the device performance with that of a more classical <span class="hlt">p-n</span> structure. In both structures (the <span class="hlt">p-n</span> and SIS heterojunction <span class="hlt">diode</span>), clear current-rectifying characteristics were observed. In particular, a current and threshold voltage were obtained for the SIS structure that was higher compared to that of the <span class="hlt">p-n</span> structure. This indicated that tunneling is the predominant carrier transport mechanism. In addition, the photoresponse of the SIS structure induced by the illumination of visible light was observed by photocurrent measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25968802','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25968802"><span>Ga<span class="hlt">N</span>-based photon-recycling green light-emitting <span class="hlt">diodes</span> with vertical-conduction structure.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sheu, Jinn-Kong; Chen, Fu-Bang; Yen, Wei-Yu; Wang, Yen-Chin; Liu, Chun-Nan; Yeh, Yu-Hsiang; Lee, Ming-Lun</p> <p>2015-04-06</p> <p>A <span class="hlt">p-i-n</span> structure with near-UV(<span class="hlt">n</span>-UV) emitting InGa<span class="hlt">N/GaN</span> multiple quantum well(MQW) structure stacked on a green unipolar InGa<span class="hlt">N/GaN</span> MQW was epitaxially grown at the same sapphire substrate. Photon recycling green light-emitting <span class="hlt">diodes</span>(LEDs) with vertical-conduction feature on silicon substrates were then fabricated by wafer bonding and laser lift-off techniques. The green InGa<span class="hlt">N/GaN</span> QWs were pumped with <span class="hlt">n</span>-UV light to reemit low-energy photons when the LEDs were electrically driven with a forward current. Efficiency droop is potentially insignificant compared with the direct green LEDs due to the increase of effective volume of active layer in the optically pumped green LEDs, <span class="hlt">i</span>.e., light emitting no longer limited in the QWs nearest to the <span class="hlt">p</span>-type region to cause severe Auger recombination and carrier overflow losses.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18585292','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18585292"><span>A lamp light-emitting <span class="hlt">diode</span>-induced fluorescence <span class="hlt">detector</span> for capillary electrophoresis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Xu, Jing; Xiong, Yan; Chen, Shiheng; Guan, Yafeng</p> <p>2008-07-15</p> <p>A light-emitting <span class="hlt">diode</span>-induced fluorescence <span class="hlt">detector</span> (LED-FD) for capillary electrophoresis was constructed and evaluated. A lamp LED with an enhanced emission spectrum and a band pass filter was used as the excitation light source. Refractive index matching fluid (RIMF) was used in the detection cell to reduce scattering light and the noise level. The limit of detection (LOD) for fluorescein was 1.5 <span class="hlt">n</span>M (SNR=3). The system exhibited linear responses in the range of 1 x 10(-8) to 5 x 10(-6)M (R=0.999). Application of the lamp LED-FD for the analysis of FITC-labeled ephedra herb extract by capillary electrophoresis was demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SeScT..33f5013M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SeScT..33f5013M"><span>Observation and discussion of avalanche electroluminescence in Ga<span class="hlt">N</span> <span class="hlt">p-n</span> <span class="hlt">diodes</span> offering a breakdown electric field of 3 MV cm‑1</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mandal, S.; Kanathila, M. B.; Pynn, C. D.; Li, W.; Gao, J.; Margalith, T.; Laurent, M. A.; Chowdhury, S.</p> <p>2018-06-01</p> <p>We report on the first observation of avalanche electroluminescence resulting from band-to-band recombination (BTBR) of electron hole pairs at the breakdown limit of Gallium Nitride <span class="hlt">p-n</span> <span class="hlt">diodes</span> grown homo-epitaxially on single crystalline Ga<span class="hlt">N</span> substrates. The <span class="hlt">diodes</span> demonstrated a near ideal breakdown electric field of 3 MV cm‑1 with electroluminescence (EL) demonstrating sharp peaks of emission energies near and at the band gap of Ga<span class="hlt">N</span>. The high critical electric field, near the material limit of Ga<span class="hlt">N</span>, was achieved by generating a smooth curved mesa edge with low plasma damage, using etch engineering without any use of field termination. The superior material quality was critical for such a near-ideal performance. An electric field of 3 MV cm‑1 recorded at the breakdown resulted in impact ionization, confirmed by a positive temperature dependence of the breakdown voltage. The spectral data provided evidence of BTBR of electron hole pairs that were generated by avalanche carrier multiplication in the depletion region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26577391','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26577391"><span>Substrate-Free InGa<span class="hlt">N/GaN</span> Nanowire Light-Emitting <span class="hlt">Diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Neplokh, Vladimir; Messanvi, Agnes; Zhang, Hezhi; Julien, Francois H; Babichev, Andrey; Eymery, Joel; Durand, Christophe; Tchernycheva, Maria</p> <p>2015-12-01</p> <p>We report on the demonstration of substrate-free nanowire/polydimethylsiloxane (PDMS) membrane light-emitting <span class="hlt">diodes</span> (LEDs). Metal-organic vapour-phase epitaxy (MOVPE)-grown InGa<span class="hlt">N/GaN</span> core-shell nanowires were encapsulated into PDMS layer. After metal deposition to <span class="hlt">p-GaN</span>, a thick PDMS cap layer was spin-coated and the membrane was manually peeled from the sapphire substrate, flipped upside down onto a steel holder, and transparent indium tin oxide (ITO) contact to <span class="hlt">n-GaN</span> was deposited. The fabricated LEDs demonstrate rectifying <span class="hlt">diode</span> characteristics. For the electroluminescence (EL) measurements, the samples were manually bonded using silver paint. The EL spectra measured at different applied voltages demonstrate a blue shift with the current increase. This shift is explained by the current injection into the InGa<span class="hlt">N</span> areas of the active region with different average indium content.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SuMi...82..269K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SuMi...82..269K"><span>Electrical parameters of Au/<span class="hlt">n-GaN</span> and Pt/<span class="hlt">n-GaN</span> Schottky <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kadaoui, Mustapha Amine; Bouiadjra, Wadi Bachir; Saidane, Abdelkader; Belahsene, Sofiane; Ramdane, Abderrahim</p> <p>2015-06-01</p> <p>Electrical properties of Si-doped Ga<span class="hlt">N</span> epitaxial layers, grown on a c-plane sapphire substrate by MOCVD to form Schottky <span class="hlt">diodes</span> with Gold (Au) and platinum (Pt) and using Ti/Al/Au as Ohmic contact, are investigated. Characterization was performed through <span class="hlt">I</span>-V and C-V-f measurements at room temperature. Schottky barrier height (Φb), ideality factor (<span class="hlt">n</span>), and series resistance (Rs) were extracted from forward <span class="hlt">I</span>-V characteriztics using Cheung and Lien methods. Φb, doping concentration (Nd) and Rs frequency dependence were extracted from C-V-f characteriztics. Pt/<span class="hlt">n-GaN</span> shows a non-linear behavior with a barrier height of 0.63 eV, an ideality factor of 2.3, and series resistance of 63 Ω. Au/<span class="hlt">n-GaN</span> behaves like two <span class="hlt">diodes</span> in parallel with two barrier heights of (0.83 and 0.9 eV), two ideality factors of (5.8 and 3.18) and two series resistance of (10.6 and 68 Ω). Interface state properties in both samples have been investigated taking into account the bias dependence of the effective barrier height. The amount of stimulated traps along the energy-gap at the interface increases with voltage bias, which increases NSS exponentially from 4.24 ṡ 1013 to 3.67 ṡ 1014 eV-1 cm-2 in the range (Ec - 0.17) to (Ec - 0.61) eV for Pt/<span class="hlt">n-GaN</span>, and from 2.3 ṡ 1013 to 1.14 ṡ 1014 eV-1 cm-2, in the range (Ec - 0.31) to (Ec - 0.82) eV for Au/<span class="hlt">n-GaN</span>. The values of interface states density and series resistance for both samples are found to decrease with increasing frequency. Peak intensity was a measure of active interface states. C-V-f results confirm the model of the Schottky <span class="hlt">diode</span> with a native interfacial insulator layer along the space charge region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApPhL.110k3501T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhL.110k3501T"><span>Radial tunnel <span class="hlt">diodes</span> based on In<span class="hlt">P</span>/InGaAs core-shell nanowires</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tizno, Ofogh; Ganjipour, Bahram; Heurlin, Magnus; Thelander, Claes; Borgström, Magnus T.; Samuelson, Lars</p> <p>2017-03-01</p> <p>We report on the fabrication and characterization of radial tunnel <span class="hlt">diodes</span> based on In<span class="hlt">P(n+)/InGaAs(p</span>+) core-shell nanowires, where the effect of Zn-dopant precursor flow on the electrical properties of the devices is evaluated. Selective and local etching of the InGaAs shell is employed to access the nanowire core in the contact process. Devices with an <span class="hlt">n+-p</span> doping profile show normal <span class="hlt">diode</span> rectification, whereas <span class="hlt">n+-p</span>+ junctions exhibit typical tunnel <span class="hlt">diode</span> characteristics with peak-to-valley current ratios up to 14 at room temperature and 100 at 4.2 K. A maximum peak current density of 28 A/cm2 and a reverse current density of 7.3 kA/cm2 at VSD = -0.5 V are extracted at room temperature after normalization with the effective junction area.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999PhRvB..5911257W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999PhRvB..5911257W"><span>Electrical transport through Pb(Zr,Ti)O3 <span class="hlt">p-n</span> and <span class="hlt">p-p</span> heterostructures modulated by bound charges at a ferroelectric surface: Ferroelectric <span class="hlt">p-n</span> <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Watanabe, Yukio</p> <p>1999-05-01</p> <p>Current through (Pb,La)(Zr,Ti)O3 ferroelectrics on perovskite semiconductors is found to exhibit <span class="hlt">diode</span> characteristics of which polarity is universally determined by the carrier conduction-type semiconductors. A persisting highly reproducible resistance modulation by a dc voltage, which has a short retention, is observed and is ascribed to a band bending of the ferroelectric by the formation of charged traps. This interpretation is consistent with a large relaxation current observed at a low voltage. On the other hand, a reproducible resistance modulation by a pulse voltage, which has a long retention, is observed in metal/(Pb,La)(Zr,Ti)O3/SrTiO3:Nb but not in metal/(Pb,La)(Zr,Ti)O3/(La,Sr)2CuO4 and is attributed to a possible band bending due to the spontaneous polarization (<span class="hlt">P</span>) switching. The observed current voltage (IV) characteristics, the polarity dependence, the relaxation, and the modulation are explicable, if we assume a <span class="hlt">p-n</span> or a <span class="hlt">p-p</span> junction at the ferroelectric semiconductor interface (<span class="hlt">p</span>: hole conduction type, <span class="hlt">n</span>: electron conduction type). The analysis suggests that an intrinsically inhomogeneous <span class="hlt">P</span> (∇<span class="hlt">P</span>) near the ferroelectric/metal interface is likely very weak or existing in a very thin layer, when a reaction of the metal with the ferroelectric is eliminated. Additionally, the various aspects of transport through ferroelectrics are explained as a transport in the carrier depleted region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JaJAP..57dFR07H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JaJAP..57dFR07H"><span>Influence of basal-plane dislocation structures on expansion of single Shockley-type stacking faults in forward-current degradation of 4H-SiC <span class="hlt">p-i-n</span> <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hayashi, Shohei; Yamashita, Tamotsu; Senzaki, Junji; Miyazato, Masaki; Ryo, Mina; Miyajima, Masaaki; Kato, Tomohisa; Yonezawa, Yoshiyuki; Kojima, Kazutoshi; Okumura, Hajime</p> <p>2018-04-01</p> <p>The origin of expanded single Shockley-type stacking faults in forward-current degradation of 4H-SiC <span class="hlt">p-i-n</span> <span class="hlt">diodes</span> was investigated by the stress-current test. At a stress-current density lower than 25 A cm-2, triangular stacking faults were formed from basal-plane dislocations in the epitaxial layer. At a stress-current density higher than 350 A cm-2, both triangular and long-zone-shaped stacking faults were formed from basal-plane dislocations that converted into threading edge dislocations near the interface between the epitaxial layer and the substrate. In addition, the conversion depth of basal-plane dislocations that expanded into the stacking fault was inside the substrate deeper than the interface. These results indicate that the conversion depth of basal-plane dislocations strongly affects the threshold stress-current density at which the expansion of stacking faults occurs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9620E..0UW','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9620E..0UW"><span>Effect of <span class="hlt">p-GaN</span> layer doping on the photoresponse of Ga<span class="hlt">N</span>-based <span class="hlt">p-i-n</span> ultraviolet photodetectors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Jun; Guo, Jin; Xie, Feng; Wang, Wanjun; Wang, Guosheng; Wu, Haoran; Wang, Tanglin; Song, Man</p> <p>2015-08-01</p> <p>We report on two-dimensional (2D) numerical simulations of photoresponse characteristics for Ga<span class="hlt">N</span> based <span class="hlt">p-i-n</span> ultraviolet (UV) photodetectors. Effects of doping density of <span class="hlt">p-GaN</span> layer on the photoresponse have been investigated. In order to accurately simulate the device performance, the theoretical calculation includes doping-dependent mobility degradation by Arora model and high field saturation model. Theoretical modeling shows that the doping density of <span class="hlt">p</span>- Ga<span class="hlt">N</span> layer can significantly affect the photoresponse of Ga<span class="hlt">N</span> based <span class="hlt">p-i-n</span> UV photodetectors, especially at schottky contact. We have to make a suitable choice of the doping in the device design according to the simulation results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhD...51o5103G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhD...51o5103G"><span>Optical characterization of magnesium incorporation in <span class="hlt">p-GaN</span> layers for core–shell nanorod light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gîrgel, I.; Šatka, A.; Priesol, J.; Coulon, P.-M.; Le Boulbar, E. D.; Batten, T.; Allsopp, D. W. E.; Shields, P. A.</p> <p>2018-04-01</p> <p>III-nitride nanostructures are of interest for a new generation of light-emitting <span class="hlt">diodes</span> (LEDs). However, the characterization of doping incorporation in nanorod (NR) structures, which is essential for creating the <span class="hlt">p-n</span> junction <span class="hlt">diodes</span>, is extremely challenging. This is because the established electrical measurement techniques (such as capacitance–voltage or Hall-effect methods) require a simple sample geometry and reliable ohmic contacts, both of which are difficult to achieve in nanoscale devices. The need for homogenous, conformal <span class="hlt">n</span>-type or <span class="hlt">p</span>-type layers in core–shell nanostructures magnifies these challenges. Consequently, we demonstrate how a combination of non-contact methods (micro-photoluminescence, micro-Raman and cathodoluminescence), as well as electron-beam-induced-current, can be used to analyze the uniformity of magnesium incorporation in core–shell NRs and make a first estimate of doping levels by the evolution of band transitions, strain and current mapping. These techniques have been used to optimize the growth of core–shell nanostructures for electrical carrier injection, a significant milestone for their use in LEDs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ApPhL.102r1115R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ApPhL.102r1115R"><span>Effects of two-step Mg doping in <span class="hlt">p-GaN</span> on efficiency characteristics of InGa<span class="hlt">N</span> blue light-emitting <span class="hlt">diodes</span> without AlGa<span class="hlt">N</span> electron-blocking layers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ryu, Han-Youl; Lee, Jong-Moo</p> <p>2013-05-01</p> <p>A light-emitting <span class="hlt">diode</span> (LED) structure containing <span class="hlt">p</span>-type Ga<span class="hlt">N</span> layers with two-step Mg doping profiles is proposed to achieve high-efficiency performance in InGa<span class="hlt">N</span>-based blue LEDs without any AlGa<span class="hlt">N</span> electron-blocking-layer structures. Photoluminescence and electroluminescence (EL) measurement results show that, as the hole concentration in the <span class="hlt">p-GaN</span> interlayer between active region and the <span class="hlt">p-GaN</span> layer increases, defect-related nonradiative recombination increases, while the electron current leakage decreases. Under a certain hole-concentration condition in the <span class="hlt">p-GaN</span> interlayer, the electron leakage and active region degradation are optimized so that high EL efficiency can be achieved. The measured efficiency characteristics are analyzed and interpreted using numerical simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JaJAP..57e0310K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JaJAP..57e0310K"><span>Spectroscopic evidence of photogenerated carrier separation by built-in electric field in Sb-doped <span class="hlt">n</span>-BaSi2/B-doped <span class="hlt">p</span>-BaSi2 homojunction <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kodama, Komomo; Takabe, Ryota; Deng, Tianguo; Toko, Kaoru; Suemasu, Takashi</p> <p>2018-05-01</p> <p>The operation of a BaSi2 homojunction solar cell is first demonstrated. In <span class="hlt">n</span>+-BaSi2 (20 nm)/<span class="hlt">p</span>-BaSi2 (500 nm)/<span class="hlt">p</span>+-BaSi2 (50 nm) homojunction <span class="hlt">diodes</span> on <span class="hlt">p</span>+-Si(111) (resistivity ρ < 0.01 Ω cm), the internal quantum efficiency (IQE) under AM1.5 illumination becomes pronounced at wavelengths λ < 800 nm and exceeded 30% at λ = 500 nm. In contrast, the IQE values are small at λ < 600 nm in <span class="hlt">n</span>+-BaSi2 (300 nm)/<span class="hlt">p</span>-Si (ρ > 0.1 Ω cm) heterojunction <span class="hlt">diodes</span>, but are high in the range between 600 and 1200 nm. The difference in spectral response demonstrates the photogenerated carrier separation by the built-in electric field in the homojunction <span class="hlt">diode</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SeScT..25i5008F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SeScT..25i5008F"><span>Interface state density of free-standing Ga<span class="hlt">N</span> Schottky <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Faraz, S. M.; Ashraf, H.; Imran Arshad, M.; Hageman, P. R.; Asghar, M.; Wahab, Q.</p> <p>2010-09-01</p> <p>Schottky <span class="hlt">diodes</span> were fabricated on the HVPE-grown, free-standing gallium nitride (Ga<span class="hlt">N</span>) layers of <span class="hlt">n</span>- and <span class="hlt">p</span>-types. Both contacts (ohmic and Schottky) were deposited on the top surface using Al/Ti and Pd/Ti/Au, respectively. The Schottky <span class="hlt">diode</span> fabricated on <span class="hlt">n-GaN</span> exhibited double barriers with values of 0.9 and 0.6 eV and better performance in the rectification factor together with reverse and forward currents with an ideality factor of 1.8. The barrier height for the <span class="hlt">p-GaN</span> Schottky <span class="hlt">diode</span> is 0.6 eV with an ideality factor of 4.16. From the capacitance-voltage (C-V) measurement, the net doping concentration of <span class="hlt">n-GaN</span> is 4 × 1017 cm-3, resulting in a lower reverse breakdown of around -12 V. The interface state density (NSS) as a function of EC-ESS is found to be in the range 4.23 × 1012-3.87 × 1011 eV-1 cm-2 (below the conduction band) from Ec-0.90 to EC-0.99. Possible reasons responsible for the low barrier height and high ideality factor have been addressed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NIMPA.828...46H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NIMPA.828...46H"><span>Processing of <span class="hlt">n+/p-/p</span>+ strip <span class="hlt">detectors</span> with atomic layer deposition (ALD) grown Al2O3 field insulator on magnetic Czochralski silicon (MCz-si) substrates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Härkönen, J.; Tuovinen, E.; Luukka, P.; Gädda, A.; Mäenpää, T.; Tuominen, E.; Arsenovich, T.; Junkes, A.; Wu, X.; Li, Z.</p> <p>2016-08-01</p> <p><span class="hlt">Detectors</span> manufactured on <span class="hlt">p</span>-type silicon material are known to have significant advantages in very harsh radiation environment over <span class="hlt">n</span>-type <span class="hlt">detectors</span>, traditionally used in High Energy Physics experiments for particle tracking. In <span class="hlt">p</span>-type (<span class="hlt">n</span>+ segmentation on <span class="hlt">p</span> substrate) position-sensitive strip <span class="hlt">detectors</span>, however, the fixed oxide charge in the silicon dioxide is positive and, thus, causes electron accumulation at the Si/SiO2 interface. As a result, unless appropriate interstrip isolation is applied, the <span class="hlt">n</span>-type strips are short-circuited. Widely adopted methods to terminate surface electron accumulation are segmented <span class="hlt">p</span>-stop or <span class="hlt">p</span>-spray field implantations. A different approach to overcome the near-surface electron accumulation at the interface of silicon dioxide and <span class="hlt">p</span>-type silicon is to deposit a thin film field insulator with negative oxide charge. We have processed silicon strip <span class="hlt">detectors</span> on <span class="hlt">p</span>-type Magnetic Czochralski silicon (MCz-Si) substrates with aluminum oxide (Al2O3) thin film insulator, grown with Atomic Layer Deposition (ALD) method. The electrical characterization by current-voltage and capacitance-voltage measurement shows reliable performance of the aluminum oxide. The final proof of concept was obtained at the test beam with 200 GeV/c muons. For the non-irradiated <span class="hlt">detector</span> the charge collection efficiency (CCE) was nearly 100% with a signal-to-noise ratio (S/<span class="hlt">N</span>) of about 40, whereas for the 2×1015 neq/cm2 proton irradiated <span class="hlt">detector</span> the CCE was 35%, when the sensor was biased at 500 V. These results are comparable with the results from <span class="hlt">p</span>-type <span class="hlt">detectors</span> with the <span class="hlt">p</span>-spray and <span class="hlt">p</span>-stop interstrip isolation techniques. In addition, interestingly, when the aluminum oxide was irradiated with Co-60 gamma-rays, an accumulation of negative fixed oxide charge in the oxide was observed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17723650','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17723650"><span>Low pressure ion chromatography with a low cost paired emitter-<span class="hlt">detector</span> <span class="hlt">diode</span> based <span class="hlt">detector</span> for the determination of alkaline earth metals in water samples.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barron, Leon; Nesterenko, Pavel N; Diamond, Dermot; O'Toole, Martina; Lau, King Tong; Paull, Brett</p> <p>2006-09-01</p> <p>The use of a low pressure ion chromatograph based upon short (25 mm x 4.6 mm) surfactant coated monolithic columns and a low cost paired emitter-<span class="hlt">detector</span> <span class="hlt">diode</span> (PEDD) based <span class="hlt">detector</span>, for the determination of alkaline earth metals in aqueous matrices is presented. The system was applied to the separation of magnesium, calcium, strontium and barium in less than 7min using a 0.15M KCl mobile phase at <span class="hlt">p</span>H 3, with post-column reaction detection at 570 nm using o-cresolphthalein complexone. A comparison of the performance of the PEDD <span class="hlt">detector</span> with a standard laboratory absorbance <span class="hlt">detector</span> is shown, with limits of detection for magnesium and calcium using the low cost PEDD <span class="hlt">detector</span> equal to 0.16 and 0.23 mg L(-1), respectively. Finally, the developed system was used for the determination of calcium and magnesium in a commercial spring water sample.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1340176-operando-spatial-imaging-edge-termination-electric-fields-gan-vertical-junction-diodes','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1340176-operando-spatial-imaging-edge-termination-electric-fields-gan-vertical-junction-diodes"><span>In-Operando Spatial Imaging of Edge Termination Electric Fields in Ga<span class="hlt">N</span> Vertical <span class="hlt">p-n</span> Junction <span class="hlt">Diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Leonard, Francois; Dickerson, J. R.; King, M. P.; ...</p> <p>2016-05-03</p> <p>Control of electric fields with edge terminations is critical to maximize the performance of high-power electronic devices. We proposed a variety of edge termination designs which makes the optimization of such designs challenging due to many parameters that impact their effectiveness. And while modeling has recently allowed new insight into the detailed workings of edge terminations, the experimental verification of the design effectiveness is usually done through indirect means, such as the impact on breakdown voltages. In this letter, we use scanning photocurrent microscopy to spatially map the electric fields in vertical Ga<span class="hlt">N</span> <span class="hlt">p-n</span> junction <span class="hlt">diodes</span> in operando. We alsomore » reveal the complex behavior of seemingly simple edge termination designs, and show how the device breakdown voltage correlates with the electric field behavior. Modeling suggests that an incomplete compensation of the <span class="hlt">p</span>-type layer in the edge termination creates a bilayer structure that leads to these effects, with variations that significantly impact the breakdown voltage.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19652937','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19652937"><span>Silicon <span class="hlt">diodes</span> as an alternative to diamond <span class="hlt">detectors</span> for depth dose curves and profile measurements of photon and electron radiation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Scherf, Christian; Peter, Christiane; Moog, Jussi; Licher, Jörg; Kara, Eugen; Zink, Klemens; Rödel, Claus; Ramm, Ulla</p> <p>2009-08-01</p> <p>Depth dose curves and lateral dose profiles should correspond to relative dose to water in any measured point, what can be more or less satisfied with different <span class="hlt">detectors</span>. Diamond as <span class="hlt">detector</span> material has similar dosimetric properties like water. Silicon <span class="hlt">diodes</span> and ionization chambers are also commonly used to acquire dose profiles. The authors compared dose profiles measured in an MP3 water phantom with a diamond <span class="hlt">detector</span> 60003, unshielded and shielded silicon <span class="hlt">diodes</span> 60008 and 60012 and a 0.125-cm(3) thimble chamber 233642 (PTW, Freiburg, Germany) for 6- and 25-MV photons. Electron beams of 6, 12 and 18 MeV were investigated with the diamond <span class="hlt">detector</span>, the unshielded <span class="hlt">diode</span> and a Markus chamber 23343. The unshielded <span class="hlt">diode</span> revealed relative dose differences at the water surface below +10% for 6-MV and +4% for 25-MV photons compared to the diamond data. These values decreased to less than 1% within the first millimeters of water depth. The shielded <span class="hlt">diode</span> was only required to obtain correct data of the fall-off zones for photon beams larger than 10 x 10 cm(2) because of important contributions of low-energy scattered photons. For electron radiation the largest relative dose difference of -2% was observed with the unshielded silicon <span class="hlt">diode</span> for 6 MeV within the build-up zone. Spatial resolutions were always best with the small voluminous silicon <span class="hlt">diodes</span>. Relative dose profiles obtained with the two silicon <span class="hlt">diodes</span> have the same degree of accuracy as with the diamond <span class="hlt">detector</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24058378','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24058378"><span>An ultra-thin Schottky <span class="hlt">diode</span> as a transmission particle <span class="hlt">detector</span> for biological microbeams.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Grad, Michael; Harken, Andrew; Randers-Pehrson, Gerhard; Attinger, Daniel; Brenner, David J</p> <p>2012-12-01</p> <p>We fabricated ultrathin metal-semiconductor Schottky <span class="hlt">diodes</span> for use as transmission particle <span class="hlt">detectors</span> in the biological microbeam at Columbia University's Radiological Research Accelerator Facility (RARAF). The RARAF microbeam can deliver a precise dose of ionizing radiation in cell nuclei with sub-micron precision. To ensure an accurate delivery of charged particles, the facility currently uses a commercial charged-particle <span class="hlt">detector</span> placed after the sample. We present here a transmission <span class="hlt">detector</span> that will be placed between the particle accelerator and the biological specimen, allowing the irradiation of samples that would otherwise block radiation from reaching a <span class="hlt">detector</span> behind the sample. Four <span class="hlt">detectors</span> were fabricated with co-planar gold and aluminum electrodes thermally evaporated onto etched <span class="hlt">n</span>-type crystalline silicon substrates, with device thicknesses ranging from 8.5 μm - 13.5 μm. We show coincident detections and pulse-height distributions of charged particles in both the transmission <span class="hlt">detector</span> and the commercial <span class="hlt">detector</span> above it. Detections are demonstrated at a range of operating conditions, including incoming particle type, count rate, and beam location on the <span class="hlt">detectors</span>. The 13.5 μm <span class="hlt">detector</span> is shown to work best to detect 2.7 MeV protons (H + ), and the 8.5 μm <span class="hlt">detector</span> is shown to work best to detect 5.4 MeV alpha particles ( 4 He ++ ). The development of a transmission <span class="hlt">detector</span> enables a range of new experiments to take place at RARAF on radiation-stopping samples such as thick tissues, targets that need immersion microscopy, and integrated microfluidic devices for handling larger quantities of cells and small organisms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3776448','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3776448"><span>An ultra-thin Schottky <span class="hlt">diode</span> as a transmission particle <span class="hlt">detector</span> for biological microbeams</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Harken, Andrew; Randers-Pehrson, Gerhard; Attinger, Daniel; Brenner, David J.</p> <p>2013-01-01</p> <p>We fabricated ultrathin metal-semiconductor Schottky <span class="hlt">diodes</span> for use as transmission particle <span class="hlt">detectors</span> in the biological microbeam at Columbia University’s Radiological Research Accelerator Facility (RARAF). The RARAF microbeam can deliver a precise dose of ionizing radiation in cell nuclei with sub-micron precision. To ensure an accurate delivery of charged particles, the facility currently uses a commercial charged-particle <span class="hlt">detector</span> placed after the sample. We present here a transmission <span class="hlt">detector</span> that will be placed between the particle accelerator and the biological specimen, allowing the irradiation of samples that would otherwise block radiation from reaching a <span class="hlt">detector</span> behind the sample. Four <span class="hlt">detectors</span> were fabricated with co-planar gold and aluminum electrodes thermally evaporated onto etched <span class="hlt">n</span>-type crystalline silicon substrates, with device thicknesses ranging from 8.5 μm – 13.5 μm. We show coincident detections and pulse-height distributions of charged particles in both the transmission <span class="hlt">detector</span> and the commercial <span class="hlt">detector</span> above it. Detections are demonstrated at a range of operating conditions, including incoming particle type, count rate, and beam location on the <span class="hlt">detectors</span>. The 13.5 μm <span class="hlt">detector</span> is shown to work best to detect 2.7 MeV protons (H+), and the 8.5 μm <span class="hlt">detector</span> is shown to work best to detect 5.4 MeV alpha particles (4He++). The development of a transmission <span class="hlt">detector</span> enables a range of new experiments to take place at RARAF on radiation-stopping samples such as thick tissues, targets that need immersion microscopy, and integrated microfluidic devices for handling larger quantities of cells and small organisms. PMID:24058378</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_10 --> <div id="page_11" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="201"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApPhL.110j2104N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhL.110j2104N"><span>All metalorganic chemical vapor phase epitaxy of <span class="hlt">p/n-GaN</span> tunnel junction for blue light emitting <span class="hlt">diode</span> applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Neugebauer, S.; Hoffmann, M. P.; Witte, H.; Bläsing, J.; Dadgar, A.; Strittmatter, A.; Niermann, T.; Narodovitch, M.; Lehmann, M.</p> <p>2017-03-01</p> <p>We report on III-Nitride blue light emitting <span class="hlt">diodes</span> (LEDs) comprising a Ga<span class="hlt">N</span>-based tunnel junction (TJ) all realized by metalorganic vapor phase epitaxy in a single growth process. The TJ grown atop the LED structures consists of a Mg-doped Ga<span class="hlt">N</span> layer and subsequently grown highly Ge-doped Ga<span class="hlt">N</span>. Long thermal annealing of 60 min at 800 °C is important to reduce the series resistance of the LEDs due to blockage of acceptor-passivating hydrogen diffusion through the <span class="hlt">n</span>-type doped top layer. Secondary ion mass spectroscopy measurements reveal Mg-incorporation into the topmost Ga<span class="hlt">N</span>:Ge layer, implying a non-abrupt <span class="hlt">p-n</span> tunnel junction and increased depletion width. Still, significantly improved lateral current spreading as compared to conventional semi-transparent Ni/Au <span class="hlt">p</span>-contact metallization and consequently a more homogeneous electroluminescence distribution across 1 × 1 mm2 LED structures is achieved. Direct estimation of the depletion width is obtained from electron holography experiments, which allows for a discussion of the possible tunneling mechanism.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22649602-currentvoltage-characteristics-high-voltage-sic-sup-sub-sup-diodes-avalanche-breakdown-mode','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22649602-currentvoltage-characteristics-high-voltage-sic-sup-sub-sup-diodes-avalanche-breakdown-mode"><span>Current–voltage characteristics of high-voltage 4H-SiC <span class="hlt">p</span>{sup +}–<span class="hlt">n</span>{sub 0}–<span class="hlt">n</span>{sup +} <span class="hlt">diodes</span> in the avalanche breakdown mode</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Ivanov, P. A., E-mail: Pavel.Ivanov@mail.ioffe.ru; Potapov, A. S.; Samsonova, T. P.</p> <p></p> <p><span class="hlt">p</span>{sup +}–<span class="hlt">n</span>{sub 0}–<span class="hlt">n</span>{sup +} 4H-SiC <span class="hlt">diodes</span> with homogeneous avalanche breakdown at 1860 V are fabricated. The pulse current–voltage characteristics are measured in the avalanche-breakdown mode up to a current density of 4000 A/cm{sup 2}. It is shown that the avalanche-breakdown voltage increases with increasing temperature. The following <span class="hlt">diode</span> parameters are determined: the avalanche resistance (8.6 × 10{sup –2} Ω cm{sup 2}), the electron drift velocity in the <span class="hlt">n</span>{sub 0} base at electric fields higher than 10{sup 6} V/cm (7.8 × 10{sup 6} cm/s), and the relative temperature coefficient of the breakdown voltage (2.1 × 10{sup –4} K{sup –1}).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000ApOpt..39.5609D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000ApOpt..39.5609D"><span>Shot-Noise-Limited Dual-Beam <span class="hlt">Detector</span> for Atmospheric Trace-Gas Monitoring with Near-Infrared <span class="hlt">Diode</span> Lasers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Durry, Georges; Pouchet, Ivan; Amarouche, Nadir; Danguy, Théodore; Megie, Gerard</p> <p>2000-10-01</p> <p>A dual-beam <span class="hlt">detector</span> is used to measure atmospheric trace species by differential absorption spectroscopy with commercial near-infrared InGaAs laser <span class="hlt">diodes</span>. It is implemented on the Spectrom tre <span class="hlt">Diodes</span> Laser Accordables, a balloonborne tunable <span class="hlt">diode</span> laser spectrometer devoted to the in situ monitoring of CH 4 and H 2 O. The dual-beam <span class="hlt">detector</span> is made of simple analogical subtractor circuits combined with InGaAs photodiodes. The detection strategy consists in taking the balanced analogical difference between the reference and the sample signals detected at the input and the output of an open optical multipass cell to apply the full dynamic range of the measurements (16 digits) to the weak molecular absorption information. The obtained sensitivity approaches the shot-noise limit. With a 56-m optical cell, the detection limit obtained when the spectra is recorded within 8 ms is 10 4 (expressed in absorbance units). The design and performances of both a simple substractor and an upgraded feedback substractor circuit are discussed with regard to atmospheric in situ CH 4 absorption spectra measured in the 1.653- m region. Mixing ratios are obtained from the absorption spectra by application of a nonlinear least-squares fit to the full molecular line shape in conjunction with in situ <span class="hlt">P</span> and T measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25298932','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25298932"><span>Study of a new design of <span class="hlt">p-N</span> semiconductor <span class="hlt">detector</span> array for nuclear medicine imaging by monte carlo simulation codes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hajizadeh-Safar, M; Ghorbani, M; Khoshkharam, S; Ashrafi, Z</p> <p>2014-07-01</p> <p>Gamma camera is an important apparatus in nuclear medicine imaging. Its detection part is consists of a scintillation <span class="hlt">detector</span> with a heavy collimator. Substitution of semiconductor <span class="hlt">detectors</span> instead of scintillator in these cameras has been effectively studied. In this study, it is aimed to introduce a new design of <span class="hlt">P-N</span> semiconductor <span class="hlt">detector</span> array for nuclear medicine imaging. A <span class="hlt">P-N</span> semiconductor <span class="hlt">detector</span> composed of <span class="hlt">N</span>-SnO2 :F, and <span class="hlt">P</span>-NiO:Li, has been introduced through simulating with MCNPX monte carlo codes. Its sensitivity with different factors such as thickness, dimension, and direction of emission photons were investigated. It is then used to configure a new design of an array in one-dimension and study its spatial resolution for nuclear medicine imaging. One-dimension array with 39 <span class="hlt">detectors</span> was simulated to measure a predefined linear distribution of Tc(99_m) activity and its spatial resolution. The activity distribution was calculated from <span class="hlt">detector</span> responses through mathematical linear optimization using LINPROG code on MATLAB software. Three different configurations of one-dimension <span class="hlt">detector</span> array, horizontal, vertical one sided, and vertical double-sided were simulated. In all of these configurations, the energy windows of the photopeak were ± 1%. The results show that the <span class="hlt">detector</span> response increases with an increase of dimension and thickness of the <span class="hlt">detector</span> with the highest sensitivity for emission photons 15-30° above the surface. Horizontal configuration array of <span class="hlt">detectors</span> is not suitable for imaging of line activity sources. The measured activity distribution with vertical configuration array, double-side <span class="hlt">detectors</span>, has no similarity with emission sources and hence is not suitable for imaging purposes. Measured activity distribution using vertical configuration array, single side <span class="hlt">detectors</span> has a good similarity with sources. Therefore, it could be introduced as a suitable configuration for nuclear medicine imaging. It has been shown that using</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015NIMPB.365..168O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015NIMPB.365..168O"><span>Formation of definite Ga<span class="hlt">N</span> <span class="hlt">p-n</span> junction by Mg-ion implantation to <span class="hlt">n--GaN</span> epitaxial layers grown on a high-quality free-standing Ga<span class="hlt">N</span> substrate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Oikawa, Takuya; Saijo, Yusuke; Kato, Shigeki; Mishima, Tomoyoshi; Nakamura, Tohru</p> <p>2015-12-01</p> <p><span class="hlt">P</span>-type conversion of <span class="hlt">n--GaN</span> by Mg-ion implantation was successfully performed using high quality Ga<span class="hlt">N</span> epitaxial layers grown on free-standing low-dislocation-density Ga<span class="hlt">N</span> substrates. These samples showed low-temperature PL spectra quite similar to those observed from Mg-doped MOVPE-grown <span class="hlt">p</span>-type Ga<span class="hlt">N</span>, consisting of Mg related donor-acceptor pair (DAP) and acceptor bound exciton (ABE) emission. <span class="hlt">P-n</span> <span class="hlt">diodes</span> fabricated by the Mg-ion implantation showed clear rectifying <span class="hlt">I</span>-V characteristics and UV and blue light emissions were observed at forward biased conditions for the first time.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150022222','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150022222"><span>Measurements of Breakdown Field and Forward Current Stability in 3C-SiC <span class="hlt">P-N</span> Junction <span class="hlt">Diodes</span> Grown on Step-Free 4H-SiC</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Neudeck, Philip G.; Spry, David J.; Trunek, Andrew J.</p> <p>2005-01-01</p> <p>This paper reports on initial fabrication and electrical characterization of 3C-SiC <span class="hlt">p-n</span> junction <span class="hlt">diodes</span> grown on step-free 4H-SiC mesas. <span class="hlt">Diodes</span> with <span class="hlt">n</span>-blocking-layer doping ranging from approx. 2 x 10(exp 16)/cu cm to approx.. 5 x 10(exp 17)/cu cm were fabricated and tested. No optimization of junction edge termination or ohmic contacts was employed. Room temperature reverse characteristics of the best devices show excellent low-leakage behavior, below previous 3C-SiC devices produced by other growth techniques, until the onset of a sharp breakdown knee. The resulting estimated breakdown field of 3C-SiC is at least twice the breakdown field of silicon, but is only around half the breakdown field of <0001> 4H-SiC for the doping range studied. Initial high current stressing of 3C <span class="hlt">diodes</span> at 100 A/sq cm for more than 20 hours resulted in less than 50 mV change in approx. 3 V forward voltage. 3C-SiC, pn junction, <span class="hlt">p+n</span> <span class="hlt">diode</span>, rectifier, reverse breakdown, breakdown field,heteroepitaxy, epitaxial growth, electroluminescence, mesa, bipolar <span class="hlt">diode</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996PhDT........25R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996PhDT........25R"><span>In-Situ Grown <span class="hlt">P-N</span> Junctions in MERCURY(1-X) Cadmium(x) Telluride for IR <span class="hlt">Detectors</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rao, Vithal Rajaram</p> <p></p> <p> necessary for high quantum efficiency devices. Photodiodes showed a cutoff wavelength of 7.5 mum, which correlates with the alloy composition of the base layer. Measured R_0 A of these <span class="hlt">diodes</span> varied between 1-100 ohm-cm ^2. In the lower R_0A <span class="hlt">diodes</span>, reverse bias was dominated by surface currents, possibly due to degradation of the passivating layer. <span class="hlt">Diodes</span> with higher R_0A showed under reverse bias that trap assisted tunneling current dominated their performance. The origin of these traps is process related and could correspond to the presence of inactivated arsenic close to the <span class="hlt">p-n</span> junction. Forward bias was dominated by diffusion and recombination currents, while the presence of additional leakage currents was evident.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JaJAP..57d0302H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JaJAP..57d0302H"><span>Leakage current reduction of vertical Ga<span class="hlt">N</span> junction barrier Schottky <span class="hlt">diodes</span> using dual-anode process</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hayashida, Tetsuro; Nanjo, Takuma; Furukawa, Akihiko; Watahiki, Tatsuro; Yamamuka, Mikio</p> <p>2018-04-01</p> <p>The origin of the leakage current of a trench-type vertical Ga<span class="hlt">N</span> <span class="hlt">diode</span> was discussed. We found that the edge of <span class="hlt">p-GaN</span> is the main leakage spot. To reduce the reverse leakage current at the edge of <span class="hlt">p-GaN</span>, a dual-anode process was proposed. As a result, the reverse blocking voltage defined at the leakage current density of 1 mA/cm2 of a vertical Ga<span class="hlt">N</span> junction barrier Schottky (JBS) <span class="hlt">diode</span> was improved from 780 to 1,190 V, which is the highest value ever reported for vertical Ga<span class="hlt">N</span> Schottky barrier <span class="hlt">diodes</span> (SBDs).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJWC.16201061L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJWC.16201061L"><span>Annealing dependence on flexible <span class="hlt">p</span>-CuGaO2/<span class="hlt">n</span>-ZnO heterojunction <span class="hlt">diode</span> deposited by RF sputtering method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li Lam, Mui; Hafiz Abu Bakar, Muhammad; Lam, Wai Yip; Alias, Afishah; Rahman, Abu Bakar Abd; Anuar Mohamad, Khairul; Uesugi, Katsuhiro</p> <p>2017-11-01</p> <p>In this work, <span class="hlt">p</span>-CuGaO2/<span class="hlt">n</span>-ZnO heterojunction <span class="hlt">diodes</span> were deposited by RF powered sputtering method on polyethylene terephthalate (PETP, PET) substrates. Structural, morphology, optical and electrical properties of CuGaO2/ZnO heterojunction was investigated as a function of annealing duration. The structural properties show the ZnO films (002) peak were stronger at the range of 34° while CuGaO2 (015) peak is not visible at 44°. The surface morphology revealed that RMS roughness become smoother as the annealing duration increase to 30 minutes and become rougher as the annealing duration is increased to 60 minutes. The optical properties of CuGaO2/ZnO heterojunction <span class="hlt">diode</span> at 30 minutes exhibit approximately 75% optical transmittance in the invisible region. The <span class="hlt">diodes</span> exhibited a rectifying characteristic and the maximum forward current was observed for the <span class="hlt">diode</span> annealed for 30 minutes. The <span class="hlt">diodes</span> show an ideality factor range from 43.69 to 71.29 and turn on voltage between 0.75 V and 1.05 V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NIMPA.879..101S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NIMPA.879..101S"><span>Low leakage current Ni/CdZnTe/In <span class="hlt">diodes</span> for X/ γ-ray <span class="hlt">detectors</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sklyarchuk, V. M.; Gnatyuk, V. A.; Pecharapa, W.</p> <p>2018-01-01</p> <p>The electrical characteristics of the Ni/Cd1-xZnxTe/In structures with a metal-semiconductor rectifying contact are investigated. The <span class="hlt">diodes</span>, fabricated on the base of In-doped <span class="hlt">n</span>-type Cd1-xZnxTe (CZT) crystals with resistivity of ∼1010 Ω ṡ cm, have low leakage current and can be used as X/ γ-ray <span class="hlt">detectors</span>. The rectifying contact was obtained by vacuum deposition of Ni on the semiconductor surface pretreated with argon plasma. The high barrier rectifying contact allowed us to increase applied reverse bias voltage up to 2500 V at the CZT crystal thickness of 1 mm. Dark (leakage) currents of the <span class="hlt">diodes</span> with the rectifying contact area of 4 mm2 did not exceed 3-5 <span class="hlt">n</span>A at bias voltage of 2000 V and room temperature. The charge transport mechanisms in the Ni/CZT/In structures have been interpreted as generation-recombination in the space charge region within the range of reverse bias of 5-100 V and as currents limited by space charge at both forward and reverse bias at V >100 V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SuMi..107..127S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SuMi..107..127S"><span>Polarization compensation at low <span class="hlt">p-GaN</span> doping density in InGa<span class="hlt">N/GaN</span> <span class="hlt">p-i-n</span> solar cells: Effect of InGa<span class="hlt">N</span> interlayers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saini, Basant; Adhikari, Sonachand; Pal, Suchandan; Kapoor, Avinsahi</p> <p>2017-07-01</p> <p>The effectiveness of polarization matching layer (PML) between <span class="hlt">i-InGaN/p-GaN</span> is studied numerically for Ga-face InGa<span class="hlt">N/GaN</span> <span class="hlt">p-i-n</span> solar cell at low <span class="hlt">p-GaN</span> doping (∼5e17 cm-3). The simulations are performed for four InxGa1-x<span class="hlt">N/GaN</span> heterostructures (x = 10%, 15%, 20% and 25%), thus investigating the impact of PML for low as well as high indium containing absorber regions. Use of PML presents a suitable alternative to counter the effects of polarization-induced electric fields arising at low <span class="hlt">p-GaN</span> doping density especially for absorber regions with high indium (>10%). It is seen that it not only mitigates the negative effects of polarization-induced electric fields but also reduces the high potential barriers existing at <span class="hlt">i-InGaN/p-GaN</span> heterojunction. The improvement in photovoltaic properties of the heterostructures even at low <span class="hlt">p-GaN</span> doping validates this claim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22649077-su-separating-effects-influencing-detector-response-small-mv-photon-fields','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22649077-su-separating-effects-influencing-detector-response-small-mv-photon-fields"><span>SU-F-T-490: Separating Effects Influencing <span class="hlt">Detector</span> Response in Small MV Photon Fields</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Wegener, S; Sauer, O</p> <p>2016-06-15</p> <p>Purpose: Different <span class="hlt">detector</span> properties influence their responses especially in field sizes below the lateral electron range. Due to the finite active volume, the <span class="hlt">detector</span> density and electron perturbation at other structural parts, the response factor is in general field size dependent. We aimed to visualize and separate the main effects contributing to <span class="hlt">detector</span> behavior for a variety of <span class="hlt">detector</span> types. This was achieved in an experimental setup, shielding the field center. Thus, effects caused by scattered radiation could be examined separately. Methods: Signal ratios for field sizes down to 8 mm (SSD 90 cm, water depth 10 cm) of amore » 6MV beam from a Siemens Primus LINAC were recorded with several <span class="hlt">detectors</span>: PTW microDiamond and PinPoint ionization chamber, shielded <span class="hlt">diodes</span> (PTW <span class="hlt">P</span>-60008, IBA PFD and SNC Edge) and unshielded <span class="hlt">diodes</span> (PTW E-60012 and IBA SFD). Measurements were carried out in open fields and with an aluminum pole of 4 mm diameter as a central block. The geometric volume effect was calculated from profiles obtained with Gafchromic EBT3 film, evaluated using FilmQA Pro software (Ashland, USA). Results: Volume corrections were 1.7% at maximum. After correction, in small open fields, unshielded <span class="hlt">diodes</span> showed a lower response than the diamond, <span class="hlt">i</span>.e. diamond <span class="hlt">detector</span> over-response seems to be higher than that for unshielded <span class="hlt">diodes</span>. Beneath the block, this behavior was amplified by a factor of 2. For the shielded <span class="hlt">diodes</span>, the overresponse for small open fields could be confirmed. However their lateral response behavior was strongly type dependent, e.g. the signal ratio dropped from 1.02 to 0.98 for the <span class="hlt">P</span>-60008 <span class="hlt">diode</span>. Conclusion: The lateral <span class="hlt">detector</span> response was experimentally examined. <span class="hlt">Detector</span> volume and density alone do not fully account for the field size dependence of <span class="hlt">detector</span> response. <span class="hlt">Detector</span> construction details play a major role, especially for shielded <span class="hlt">diodes</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950043872&hterms=electrical+characterization+diode&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Delectrical%2Bcharacterization%2Bdiode','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950043872&hterms=electrical+characterization+diode&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Delectrical%2Bcharacterization%2Bdiode"><span>Electrical properties of epitaxial 3C- and 6H-SiC <span class="hlt">p-n</span> junction <span class="hlt">diodes</span> produced side-by-side on 6H-SiC substrates</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Neudeck, Philip G.; Larkin, David J.; Starr, Jonathan E.; Powell, J. Anthony; Salupo, Carl S.; Matus, Lawrence G.</p> <p>1994-01-01</p> <p>3C-SiC (beta-SiC) and 6H-SiC <span class="hlt">p-n</span> junction <span class="hlt">diodes</span> have been fabricated in regions of both 3C-SiC and 6H-SiC epitaxial layers which were grown side-by-side on low-tilt-angle 6H-SiC substrates via a chemical vapor deposition (CVD) process. Several runs of <span class="hlt">diodes</span> exhibiting state-of-the-art electrical characteristics were produced, and performance characteristics were measured and compared as a function of doping, temperature, and polytype. The first 3C-SiC <span class="hlt">diodes</span> which rectify to reverse voltages in excess of 300 V were characterized, representing a six-fold blocking voltage improvement over experimental 3C-SiC <span class="hlt">diodes</span> produced by previous techniques. When placed under sufficient forward bias, the 3C-SiC <span class="hlt">diodes</span> emit significantly bright green-yellow light while the 6H-SiC <span class="hlt">diodes</span> emit in the blue-violet. The 6H-SiC <span class="hlt">p-n</span> junction <span class="hlt">diodes</span> represent the first reported high-quality 6H-SiC devices to be grown by CVD on very low-tilt-angle (less than 0.5 deg off the (0001) silicon face) 6H substrates. The reverse leakage current of a 200 micron diameter circular device at 1100 V reverse bias was less than 20 <span class="hlt">n</span>A at room temperature, and excellent rectification characteristics were demonstrated at the peak characterization temperature of 400 C.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29041450','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29041450"><span>Dependencies of surface plasmon coupling effects on the <span class="hlt">p-GaN</span> thickness of a thin-<span class="hlt">p</span>-type light-emitting <span class="hlt">diode</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Su, Chia-Ying; Lin, Chun-Han; Yao, Yu-Feng; Liu, Wei-Heng; Su, Ming-Yen; Chiang, Hsin-Chun; Tsai, Meng-Che; Tu, Charng-Gan; Chen, Hao-Tsung; Kiang, Yean-Woei; Yang, C C</p> <p>2017-09-04</p> <p>The high performance of a light-emitting <span class="hlt">diode</span> (LED) with the total <span class="hlt">p</span>-type thickness as small as 38 nm is demonstrated. By increasing the Mg doping concentration in the <span class="hlt">p-AlGaN</span> electron blocking layer through an Mg pre-flow process, the hole injection efficiency can be significantly enhanced. Based on this technique, the high LED performance can be maintained when the <span class="hlt">p</span>-type layer thickness is significantly reduced. Then, the surface plasmon coupling effects, including the enhancement of internal quantum efficiency, increase in output intensity, reduction of efficiency droop, and increase of modulation bandwidth, among the thin <span class="hlt">p</span>-type LED samples of different <span class="hlt">p</span>-type thicknesses that are compared. These advantageous effects are stronger as the <span class="hlt">p</span>-type layer becomes thinner. However, the dependencies of these effects on <span class="hlt">p</span>-type layer thickness are different. With a circular mesa size of 10 μm in radius, through surface plasmon coupling, we achieve the record-high modulation bandwidth of 625.6 MHz among c-plane Ga<span class="hlt">N</span>-based LEDs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5795930','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5795930"><span>A Low-Noise X-ray Astronomical Silicon-On-Insulator Pixel <span class="hlt">Detector</span> Using a Pinned Depleted <span class="hlt">Diode</span> Structure</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kamehama, Hiroki; Kawahito, Shoji; Shrestha, Sumeet; Nakanishi, Syunta; Yasutomi, Keita; Takeda, Ayaki; Tsuru, Takeshi Go</p> <p>2017-01-01</p> <p>This paper presents a novel full-depletion Si X-ray <span class="hlt">detector</span> based on silicon-on-insulator pixel (SOIPIX) technology using a pinned depleted <span class="hlt">diode</span> structure, named the SOIPIX-PDD. The SOIPIX-PDD greatly reduces stray capacitance at the charge sensing node, the dark current of the <span class="hlt">detector</span>, and capacitive coupling between the sensing node and SOI circuits. These features of the SOIPIX-PDD lead to low read noise, resulting high X-ray energy resolution and stable operation of the pixel. The back-gate surface pinning structure using neutralized <span class="hlt">p</span>-well at the back-gate surface and depleted <span class="hlt">n</span>-well underneath the <span class="hlt">p</span>-well for all the pixel area other than the charge sensing node is also essential for preventing hole injection from the <span class="hlt">p</span>-well by making the potential barrier to hole, reducing dark current from the Si-SiO2 interface and creating lateral drift field to gather signal electrons in the pixel area into the small charge sensing node. A prototype chip using 0.2 μm SOI technology shows very low readout noise of 11.0 e−rms, low dark current density of 56 <span class="hlt">p</span>A/cm2 at −35 °C and the energy resolution of 200 eV(FWHM) at 5.9 keV and 280 eV (FWHM) at 13.95 keV. PMID:29295523</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29295523','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29295523"><span>A Low-Noise X-ray Astronomical Silicon-On-Insulator Pixel <span class="hlt">Detector</span> Using a Pinned Depleted <span class="hlt">Diode</span> Structure.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kamehama, Hiroki; Kawahito, Shoji; Shrestha, Sumeet; Nakanishi, Syunta; Yasutomi, Keita; Takeda, Ayaki; Tsuru, Takeshi Go; Arai, Yasuo</p> <p>2017-12-23</p> <p>This paper presents a novel full-depletion Si X-ray <span class="hlt">detector</span> based on silicon-on-insulator pixel (SOIPIX) technology using a pinned depleted <span class="hlt">diode</span> structure, named the SOIPIX-PDD. The SOIPIX-PDD greatly reduces stray capacitance at the charge sensing node, the dark current of the <span class="hlt">detector</span>, and capacitive coupling between the sensing node and SOI circuits. These features of the SOIPIX-PDD lead to low read noise, resulting high X-ray energy resolution and stable operation of the pixel. The back-gate surface pinning structure using neutralized <span class="hlt">p</span>-well at the back-gate surface and depleted <span class="hlt">n</span>-well underneath the <span class="hlt">p</span>-well for all the pixel area other than the charge sensing node is also essential for preventing hole injection from the <span class="hlt">p</span>-well by making the potential barrier to hole, reducing dark current from the Si-SiO₂ interface and creating lateral drift field to gather signal electrons in the pixel area into the small charge sensing node. A prototype chip using 0.2 μm SOI technology shows very low readout noise of 11.0 e - rms , low dark current density of 56 <span class="hlt">p</span>A/cm² at -35 °C and the energy resolution of 200 eV(FWHM) at 5.9 keV and 280 eV (FWHM) at 13.95 keV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JAP...122a3104L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JAP...122a3104L"><span>Design and characterization of free-running InGaAs<span class="hlt">P</span> single-photon <span class="hlt">detector</span> with active-quenching technique</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Junliang; Zhang, Tingfa; Li, Yongfu; Ding, Lei; Tao, Junchao; Wang, Ying; Wang, Qingpu; Fang, Jiaxiong</p> <p>2017-07-01</p> <p>A free-running single-photon <span class="hlt">detector</span> for 1.06 μm wavelength based on an InGaAs<span class="hlt">P/InP</span> single-photon avalanche <span class="hlt">diode</span> is presented. The <span class="hlt">detector</span> incorporates an ultra-fast active-quenching technique to greatly lessen the afterpulsing effects. An improved method for avalanche characterization using electroluminescence is proposed, and the performance of the <span class="hlt">detector</span> is evaluated. The number of avalanche carriers is as low as 1.68 ×106 , resulting in a low total afterpulse probability of 4% at 233 K, 10% detection efficiency, and 1 μs hold-off time.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JKPS...71..349N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JKPS...71..349N"><span>Effects of <span class="hlt">P</span>3HT concentration on the electrical properties of the Au/PEDOT:PSS/<span class="hlt">P</span>3HT/<span class="hlt">n-GaN</span> hybrid junction structure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Noh, Ji-yeon; Lee, Ha Young; Lim, Kyung-won; Ahn, Hyung Soo; Yi, Sam Nyung; Jeon, Hunsoo; Shin, Min Jeong; Yu, Young Moon; Ha, Dong Han</p> <p>2017-09-01</p> <p>An inorganic-organic hybrid junction has been fabricated by spin coating the <span class="hlt">p</span>-type poly(3- hexylthiophene-2,5-diyl)(<span class="hlt">P</span>3HT) and poly(3,4-ethylenedioxythiophene)-poly(styrenesulfonate) (PEDOT: PSS) on an <span class="hlt">n</span>-type Ga<span class="hlt">N</span> layer. The Ga<span class="hlt">N</span> layer was formed on Al2O3 by metal organic chemical vapor deposition(MOCVD) method. To investigate the effects of <span class="hlt">P</span>3HT concentration on the electrical properties, we changed <span class="hlt">P</span>3HT solution concentration and speed of spin coater. The currentvoltage (<span class="hlt">I</span>-V ) characteristic of Au/PEDOT:PSS/<span class="hlt">P</span>3HT/<span class="hlt">n-GaN</span> shows rectifying behavior. The <span class="hlt">I</span>-V characteristic was examined in the frame work of the thermionic emission model. The most proper rectifying behavior was obtained for 0.6 wt% and thickness below 65 nm of <span class="hlt">P</span>3HT used <span class="hlt">diode</span>. We expect that such hybrid structures, suitably developed, might be enable the fabrication of highquality electronic and optoelectronic devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1175165','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1175165"><span>Process for direct integration of a thin-film silicon <span class="hlt">p-n</span> junction <span class="hlt">diode</span> with a magnetic tunnel junction</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Toet, Daniel; Sigmon, Thomas W.</p> <p>2004-12-07</p> <p>A process for direct integration of a thin-film silicon <span class="hlt">p-n</span> junction <span class="hlt">diode</span> with a magnetic tunnel junction for use in advanced magnetic random access memory (MRAM) cells for high performance, non-volatile memory arrays. The process is based on pulsed laser processing for the fabrication of vertical polycrystalline silicon electronic device structures, in particular <span class="hlt">p-n</span> junction <span class="hlt">diodes</span>, on films of metals deposited onto low temperature-substrates such as ceramics, dielectrics, glass, or polymers. The process preserves underlayers and structures onto which the devices are typically deposited, such as silicon integrated circuits. The process involves the low temperature deposition of at least one layer of silicon, either in an amorphous or a polycrystalline phase on a metal layer. Dopants may be introduced in the silicon film during or after deposition. The film is then irradiated with short pulse laser energy that is efficiently absorbed in the silicon, which results in the crystallization of the film and simultaneously in the activation of the dopants via ultrafast melting and solidification. The silicon film can be patterned either before or after crystallization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/880619','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/880619"><span>Process For Direct Integration Of A Thin-Film Silicon <span class="hlt">P-N</span> Junction <span class="hlt">Diode</span> With A Magnetic Tunnel Junction</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Toet, Daniel; Sigmon, Thomas W.</p> <p>2005-08-23</p> <p>A process for direct integration of a thin-film silicon <span class="hlt">p-n</span> junction <span class="hlt">diode</span> with a magnetic tunnel junction for use in advanced magnetic random access memory (MRAM) cells for high performance, non-volatile memory arrays. The process is based on pulsed laser processing for the fabrication of vertical polycrystalline silicon electronic device structures, in particular <span class="hlt">p-n</span> junction <span class="hlt">diodes</span>, on films of metals deposited onto low temperature-substrates such as ceramics, dielectrics, glass, or polymers. The process preserves underlayers and structures onto which the devices are typically deposited, such as silicon integrated circuits. The process involves the low temperature deposition of at least one layer of silicon, either in an amorphous or a polycrystalline phase on a metal layer. Dopants may be introduced in the silicon film during or after deposition. The film is then irradiated with short pulse laser energy that is efficiently absorbed in the silicon, which results in the crystallization of the film and simultaneously in the activation of the dopants via ultrafast melting and solidification. The silicon film can be patterned either before or after crystallization.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_11 --> <div id="page_12" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="221"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/875136','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/875136"><span>Process for direct integration of a thin-film silicon <span class="hlt">p-n</span> junction <span class="hlt">diode</span> with a magnetic tunnel junction</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Toet, Daniel; Sigmon, Thomas W.</p> <p>2003-01-01</p> <p>A process for direct integration of a thin-film silicon <span class="hlt">p-n</span> junction <span class="hlt">diode</span> with a magnetic tunnel junction for use in advanced magnetic random access memory (MRAM) cells for high performance, non-volatile memory arrays. The process is based on pulsed laser processing for the fabrication of vertical polycrystalline silicon electronic device structures, in particular <span class="hlt">p-n</span> junction <span class="hlt">diodes</span>, on films of metals deposited onto low temperature-substrates such as ceramics, dielectrics, glass, or polymers. The process preserves underlayers and structures onto which the devices are typically deposited, such as silicon integrated circuits. The process involves the low temperature deposition of at least one layer of silicon, either in an amorphous or a polycrystalline phase on a metal layer. Dopants may be introduced in the silicon film during or after deposition. The film is then irradiated with short pulse laser energy that is efficiently absorbed in the silicon, which results in the crystallization of the film and simultaneously in the activation of the dopants via ultrafast melting and solidification. The silicon film can be patterned either before or after crystallization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23683053','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23683053"><span>Fabricate heterojunction <span class="hlt">diode</span> by using the modified spray pyrolysis method to deposit nickel-lithium oxide on indium tin oxide substrate.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wu, Chia-Ching; Yang, Cheng-Fu</p> <p>2013-06-12</p> <p><span class="hlt">P</span>-type lithium-doped nickel oxide (<span class="hlt">p</span>-LNiO) thin films were deposited on an <span class="hlt">n</span>-type indium tin oxide (ITO) glass substrate using the modified spray pyrolysis method (SPM), to fabricate a transparent <span class="hlt">p-n</span> heterojunction <span class="hlt">diode</span>. The structural, optical, and electrical properties of the <span class="hlt">p</span>-LNiO and ITO thin films and the <span class="hlt">p-LNiO/n</span>-ITO heterojunction <span class="hlt">diode</span> were characterized by field emission scanning electron microscopy (FE-SEM), X-ray diffraction (XRD), UV-visible spectroscopy, Hall effect measurement, and current-voltage (<span class="hlt">I</span>-V) measurements. The nonlinear and rectifying <span class="hlt">I</span>-V properties confirmed that a heterojunction <span class="hlt">diode</span> characteristic was successfully formed in the <span class="hlt">p-LNiO/n</span>-ITO (<span class="hlt">p-n</span>) structure. The <span class="hlt">I</span>-V characteristic was dominated by space-charge-limited current (SCLC), and the Anderson model demonstrated that band alignment existed in the <span class="hlt">p-LNiO/n</span>-ITO heterojunction <span class="hlt">diode</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/2285140','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/2285140"><span>Construction of a fast, inexpensive rapid-scanning <span class="hlt">diode</span>-array <span class="hlt">detector</span> and spectrometer.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Carter, T P; Baek, H K; Bonninghausen, L; Morris, R J; van Wart, H E</p> <p>1990-10-01</p> <p>A 512-element <span class="hlt">diode</span>-array spectroscopic detection system capable of acquiring multiple spectra at a rate of 5 ms per spectrum with an effective scan rate of 102.9 kHz has been constructed. Spectra with fewer <span class="hlt">diode</span> elements can also be acquired at scan rates up to 128 kHz. The <span class="hlt">detector</span> utilizes a Hamamatsu silicon photodiode-array sensor that is interfaced to Hamamatsu driver/amplifier and clock generator boards and a DRA laboratories 12-bit 160-kHz analog-to-digital converter. These are standard, commercially available devices which cost approximately $3500. The system is interfaced to and controlled by an IBM XT microcomputer. Detailed descriptions of the home-built <span class="hlt">detector</span> housing and control/interface circuitry are presented and its application to the study of the reaction of horseradish peroxidase with hydrogen peroxide is demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23683526','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23683526"><span>Enhancement of light output power of Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> with photonic quasi-crystal patterned on <span class="hlt">p-GaN</span> surface and <span class="hlt">n</span>-side sidewall roughing.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lai, Fang-I; Yang, Jui-Fu</p> <p>2013-05-17</p> <p>In this paper, Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> (LEDs) with photonic quasi-crystal (PQC) structure on <span class="hlt">p-GaN</span> surface and <span class="hlt">n</span>-side roughing by nano-imprint lithography are fabricated and investigated. At an injection current of 20 mA, the LED with PQC structure on <span class="hlt">p-GaN</span> surface and <span class="hlt">n</span>-side roughing increased the light output power of the InGa<span class="hlt">N/GaN</span> multiple quantum well LEDs by a factor of 1.42, and the wall-plug efficiency is 26% higher than the conventional Ga<span class="hlt">N</span>-based LED type. After 500-h life test (55°C/50 mA), it was found that the normalized output power of Ga<span class="hlt">N</span>-based LED with PQC structure on <span class="hlt">p-GaN</span> surface and <span class="hlt">n</span>-side roughing only decreased by 6%. These results offer promising potential to enhance the light output powers of commercial light-emitting devices using the technique of nano-imprint lithography.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3671165','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3671165"><span>Enhancement of light output power of Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> with photonic quasi-crystal patterned on <span class="hlt">p-GaN</span> surface and <span class="hlt">n</span>-side sidewall roughing</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2013-01-01</p> <p>In this paper, Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> (LEDs) with photonic quasi-crystal (PQC) structure on <span class="hlt">p-GaN</span> surface and <span class="hlt">n</span>-side roughing by nano-imprint lithography are fabricated and investigated. At an injection current of 20 mA, the LED with PQC structure on <span class="hlt">p-GaN</span> surface and <span class="hlt">n</span>-side roughing increased the light output power of the InGa<span class="hlt">N/GaN</span> multiple quantum well LEDs by a factor of 1.42, and the wall-plug efficiency is 26% higher than the conventional Ga<span class="hlt">N</span>-based LED type. After 500-h life test (55°C/50 mA), it was found that the normalized output power of Ga<span class="hlt">N</span>-based LED with PQC structure on <span class="hlt">p-GaN</span> surface and <span class="hlt">n</span>-side roughing only decreased by 6%. These results offer promising potential to enhance the light output powers of commercial light-emitting devices using the technique of nano-imprint lithography. PMID:23683526</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22310885-high-performance-zero-bias-ultraviolet-photodetector-based-gan-zno-heterojunction','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22310885-high-performance-zero-bias-ultraviolet-photodetector-based-gan-zno-heterojunction"><span>High-performance zero-bias ultraviolet photodetector based on <span class="hlt">p-GaN/n</span>-ZnO heterojunction</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Su, Longxing; Zhang, Quanlin; Chen, Mingming</p> <p>2014-08-18</p> <p>Lattice-match <span class="hlt">p-GaN</span> and <span class="hlt">n</span>-ZnO bilayers were heteroepitaxially grown on the c-sapphire substrate by metal organic chemical vapor deposition and molecular beam epitaxy technique, respectively. X-ray diffraction and photoluminescence investigations revealed the high crystal quality of the bilayer films. Subsequently, a <span class="hlt">p-GaN/n</span>-ZnO heterojunction photodetector was fabricated. The <span class="hlt">p-n</span> junction exhibited a clear rectifying <span class="hlt">I</span>-V characteristic with a turn-on voltage of 3.7 V. At zero-bias voltage, the peak responsivity was 0.68 mA/W at 358 nm, which is one of the best performances reported for <span class="hlt">p-GaN/n</span>-ZnO heterojunction <span class="hlt">detectors</span> due to the excellent crystal quality of the bilayer films. These show that the high-performance <span class="hlt">p-GaN/n</span>-ZnO heterojunction diodemore » is potential for applications of portable UV <span class="hlt">detectors</span> without driving power.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JAP...117d5710G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JAP...117d5710G"><span>Comprehensive study of the electronic and optical behavior of highly degenerate <span class="hlt">p</span>-type Mg-doped Ga<span class="hlt">N</span> and AlGa<span class="hlt">N</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gunning, Brendan P.; Fabien, Chloe A. M.; Merola, Joseph J.; Clinton, Evan A.; Doolittle, W. Alan; Wang, Shuo; Fischer, Alec M.; Ponce, Fernando A.</p> <p>2015-01-01</p> <p>The bulk and 2-dimensional (2D) electrical transport properties of heavily Mg-doped <span class="hlt">p</span>-type Ga<span class="hlt">N</span> films grown on Al<span class="hlt">N</span> buffer layers by Metal Modulated Epitaxy are explored. Distinctions are made between three primary <span class="hlt">p</span>-type conduction mechanisms: traditional valence band conduction, impurity band conduction, and 2D conduction within a 2D hole gas at a hetero-interface. The bulk and 2D contributions to the overall carrier transport are identified and the relative contributions are found to vary strongly with growth conditions. Films grown with III/V ratio less than 1.5 exhibit high hole concentrations exceeding 2 × 1019 cm-3 with effective acceptor activation energies of 51 meV. Films with III/V ratios greater than 1.5 exhibit lower overall hole concentrations and significant contributions from 2D transport at the hetero-interface. Films grown with III/V ratio of 1.2 and Mg concentrations exceeding 2 × 1020 cm-3 show no detectable inversion domains or Mg precipitation. Highly Mg-doped <span class="hlt">p-GaN</span> and <span class="hlt">p-AlGaN</span> with Al fractions up to 27% similarly exhibit hole concentrations exceeding 2 × 1019 cm-3. The <span class="hlt">p-GaN</span> and <span class="hlt">p</span>-Al0.11Ga0.89<span class="hlt">N</span> films show broad ultraviolet (UV) photoluminescence peaks, which intercept the valence band, supporting the presence of a Mg acceptor band. Finally, a multi-quantum-well light-emitting <span class="hlt">diode</span> (LED) and <span class="hlt">p-i-n</span> <span class="hlt">diode</span> are grown, both of which demonstrate rectifying behavior with turn-on voltages of 3-3.5 V and series resistances of 6-10 Ω without the need for any post-metallization annealing. The LED exhibits violet-blue luminescence at 425 nm, while the <span class="hlt">p-i-n</span> <span class="hlt">diode</span> shows UV luminescence at 381 nm, and both devices still show substantial light emission even when submerged in liquid nitrogen at 77 K.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900027878&hterms=ito&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dito','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900027878&hterms=ito&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dito"><span>Radiation resistance and comparative performance of ITO/In<span class="hlt">P</span> and <span class="hlt">n/p</span> In<span class="hlt">P</span> homojunction solar cells</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Weinberg, I.; Swartz, C. K.; Hart, R. E., Jr.; Coutts, T. J.</p> <p>1988-01-01</p> <p>The radiation resistance of ITO/In<span class="hlt">P</span> cells processed by dc magnetron sputtering is compared to that of standard <span class="hlt">n/p</span> In<span class="hlt">P</span> and GaAs homojunction cells. After 20 MeV proton irradiations, it is found that the radiation resistance of the present ITO/In<span class="hlt">P</span> cell is comparable to that of the <span class="hlt">n/p</span> homojunction In<span class="hlt">P</span> cell and that both In<span class="hlt">P</span> cell types have radiation resistances significantly greater than GaAs. The relatively lower radiation resistance, observed at higher fluence, for the In<span class="hlt">P</span> cell with the deepest junction depth, is attributed to losses in the cells emitter region. <span class="hlt">Diode</span> parameters obtained from <span class="hlt">I</span> sub sc - V sub oc plots, data from surface Raman spectrosocpy, and determinations of surface conductivity type are used to investigate the configuration of the ITO/In<span class="hlt">P</span> cells. It is concluded that these latter cells are <span class="hlt">n/p</span> homojunctions, the <span class="hlt">n</span>-region consisting of a disordered layer at the oxide semiconductor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890003448','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890003448"><span>Radiation resistance and comparative performance of ITO/In<span class="hlt">P</span> and <span class="hlt">n/p</span> In<span class="hlt">P</span> homojunction solar cells</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Weinberg, I.; Swartz, C. K.; Hart, R. E., Jr.; Coutts, T. J.</p> <p>1988-01-01</p> <p>The radiation resistance of ITO/In<span class="hlt">P</span> cells processed by DC magnetron sputtering is compared to that of standard <span class="hlt">n/p</span> In<span class="hlt">P</span> and GaAs homojunction cells. After 20 MeV proton irradiations, it is found that the radiation resistance of the present ITO/In<span class="hlt">P</span> cell is comparable to that of the <span class="hlt">n/p</span> homojunction In<span class="hlt">P</span> cell and that both In<span class="hlt">P</span> cell types have radiation resistance significantly greater than GaAs. The relatively lower radiation resistance, observed at higher fluence, for the In<span class="hlt">P</span> cell with the deepest junction depth, is attributed to losses in the cells emitter region. <span class="hlt">Diode</span> parameters obtained from <span class="hlt">I</span> sub sc - V sub oc plots, data from surface Raman spectroscopy, and determinations of surface conductivity types are used to investigate the configuration of the ITO/In<span class="hlt">P</span> cells. It is concluded that thesee latter cells are <span class="hlt">n/p</span> homojunctions, the <span class="hlt">n</span>-region consisting of a disordered layer at the oxide semiconductor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26745934','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26745934"><span>Small field <span class="hlt">detector</span> correction factors kQclin,Qmsr (fclin,fmsr) for silicon-<span class="hlt">diode</span> and diamond <span class="hlt">detectors</span> with circular 6 MV fields derived using both empirical and numerical methods.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>O'Brien, D J; León-Vintró, L; McClean, B</p> <p>2016-01-01</p> <p>The use of radiotherapy fields smaller than 3 cm in diameter has resulted in the need for accurate <span class="hlt">detector</span> correction factors for small field dosimetry. However, published factors do not always agree and errors introduced by biased reference <span class="hlt">detectors</span>, inaccurate Monte Carlo models, or experimental errors can be difficult to distinguish. The aim of this study was to provide a robust set of <span class="hlt">detector</span>-correction factors for a range of <span class="hlt">detectors</span> using numerical, empirical, and semiempirical techniques under the same conditions and to examine the consistency of these factors between techniques. Empirical <span class="hlt">detector</span> correction factors were derived based on small field output factor measurements for circular field sizes from 3.1 to 0.3 cm in diameter performed with a 6 MV beam. A PTW 60019 microDiamond <span class="hlt">detector</span> was used as the reference dosimeter. Numerical <span class="hlt">detector</span> correction factors for the same fields were derived based on calculations from a geant4 Monte Carlo model of the <span class="hlt">detectors</span> and the Linac treatment head. Semiempirical <span class="hlt">detector</span> correction factors were derived from the empirical output factors and the numerical dose-to-water calculations. The PTW 60019 microDiamond was found to over-respond at small field sizes resulting in a bias in the empirical <span class="hlt">detector</span> correction factors. The over-response was similar in magnitude to that of the unshielded <span class="hlt">diode</span>. Good agreement was generally found between semiempirical and numerical <span class="hlt">detector</span> correction factors except for the PTW 60016 <span class="hlt">Diode</span> <span class="hlt">P</span>, where the numerical values showed a greater over-response than the semiempirical values by a factor of 3.7% for a 1.1 cm diameter field and higher for smaller fields. <span class="hlt">Detector</span> correction factors based solely on empirical measurement or numerical calculation are subject to potential bias. A semiempirical approach, combining both empirical and numerical data, provided the most reliable results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22594286-reverse-bias-driven-dichromatic-electroluminescence-zno-wire-arrays-gan-film-heterojunction-light-emitting-diodes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22594286-reverse-bias-driven-dichromatic-electroluminescence-zno-wire-arrays-gan-film-heterojunction-light-emitting-diodes"><span>Reverse-bias-driven dichromatic electroluminescence of <span class="hlt">n</span>-ZnO wire arrays/<span class="hlt">p-GaN</span> film heterojunction light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Jeong, Junseok; Choi, Ji Eun; Hong, Young Joon, E-mail: yjhong@sejong.ac.kr</p> <p></p> <p>Position-controlled <span class="hlt">n</span>-ZnO microwire (MW) and nanowire-bundle (NW-B) arrays were fabricated using hydrothermal growth of ZnO on a patterned <span class="hlt">p-GaN</span> film. Both the wire/film p–<span class="hlt">n</span> heterojunctions showed electrical rectification features at reverse-bias (rb) voltages, analogous to backward <span class="hlt">diodes</span>. Dichromatic electroluminescence (EL) emissions with 445- and 560-nm-wavelength peaks displayed whitish-blue and greenish-yellow light from MW- and NW-B-based heterojunctions at rb voltages, respectively. The different dichromatic EL emission colors were studied based on photoluminescence spectra and the dichromatic EL peak intensity ratios as a function of the rb voltage. The different EL colors are discussed with respect to depletion thickness and electron tunnelingmore » probability determined by wire/film junction geometry and size.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20549226','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20549226"><span>COTS Silicon <span class="hlt">diodes</span> as radiation <span class="hlt">detectors</span> in proton and heavy charged particle radiotherapy 1.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kaiser, Franz-Joachim; Bassler, Niels; Jäkel, Oliver</p> <p>2010-08-01</p> <p>Modern radiotherapy facilities for cancer treatment such as the Heavy Ion Therapy Center (HIT) in Heidelberg, Germany, allow for sub-millimeter precision in dose deposition. For measurement of such dose distributions and characterization of the particle beams, <span class="hlt">detectors</span> with high spatial resolution are necessary. Here, a <span class="hlt">detector</span> based on the commercially available COTS photodiode (BPW-34) is presented. When applied in hadronic beams of protons and carbon ions, the <span class="hlt">detector</span> reproduces dose distribution well, but its response decreases rapidly by radiation damage. However, for MeV photon beams, the <span class="hlt">detector</span> exhibits a similar behavior as found in <span class="hlt">diode</span> <span class="hlt">detectors</span> usually applied in radiotherapy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810042693&hterms=Intrinsic+extrinsic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DIntrinsic%2Bextrinsic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810042693&hterms=Intrinsic+extrinsic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DIntrinsic%2Bextrinsic"><span>Thin <span class="hlt">n-i-p</span> silicon solar cell</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Meulenberg, A., Jr.; Allison, J. F.; Arndt, R. A.</p> <p>1980-01-01</p> <p>A space solar cell concept which combines high cell output with low diffusion length damage coefficients is presented for the purpose of reducing solar cell susceptibility to degradation from the radiation environment. High resistivity <span class="hlt">n-i-p</span> silicon solar cells ranging from upward of 83 micron-cm were exposed to AM0 ultraviolet illumination. It is shown that high resistivity cells act as extrinsic devices under dark conditions and as intrinsic devices under AM0 illumination. Resistive losses in thin <span class="hlt">n-i-p</span> cells are found to be comparable to those in low resistivity cells. Present voltage limitations appear to be due to generation and recombination in the diffused regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ApPhL.105x1103M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ApPhL.105x1103M"><span>Low temperature <span class="hlt">p</span>-type doping of (Al)Ga<span class="hlt">N</span> layers using ammonia molecular beam epitaxy for InGa<span class="hlt">N</span> laser <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Malinverni, M.; Lamy, J.-M.; Martin, D.; Feltin, E.; Dorsaz, J.; Castiglia, A.; Rossetti, M.; Duelk, M.; Vélez, C.; Grandjean, N.</p> <p>2014-12-01</p> <p>We demonstrate state-of-the-art <span class="hlt">p</span>-type (Al)Ga<span class="hlt">N</span> layers deposited at low temperature (740 °C) by ammonia molecular beam epitaxy (NH3-MBE) to be used as top cladding of laser <span class="hlt">diodes</span> (LDs) with the aim of further reducing the thermal budget on the InGa<span class="hlt">N</span> quantum well active region. Typical <span class="hlt">p</span>-type Ga<span class="hlt">N</span> resistivities and contact resistances are 0.4 Ω cm and 5 × 10-4 Ω cm2, respectively. As a test bed, we fabricated a hybrid laser structure emitting at 400 nm combining <span class="hlt">n</span>-type AlGa<span class="hlt">N</span> cladding and InGa<span class="hlt">N</span> active region grown by metal-organic vapor phase epitaxy, with the <span class="hlt">p</span>-doped waveguide and cladding layers grown by NH3-MBE. Single-mode ridge-waveguide LD exhibits a threshold voltage as low as 4.3 V for an 800 × 2 μm2 ridge dimension and a threshold current density of ˜5 kA cm-2 in continuous wave operation. The series resistance of the device is 6 Ω and the resistivity is 1.5 Ω cm, confirming thereby the excellent electrical properties of <span class="hlt">p</span>-type Al0.06Ga0.94<span class="hlt">N</span>:Mg despite the low growth temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810044880&hterms=Electronically+controlled+injection&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DElectronically%2Bcontrolled%2Binjection','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810044880&hterms=Electronically+controlled+injection&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DElectronically%2Bcontrolled%2Binjection"><span>Variable <span class="hlt">N</span>-type negative resistance in an injection-gated double-injection <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kapoor, A. K.; Henderson, H. T.</p> <p>1981-01-01</p> <p>Double-injection (DI) switching devices consist of <span class="hlt">p</span>+ and <span class="hlt">n</span>+ contacts (for hole and electron injection, respectively), separated by a near intrinsic semiconductor region containing deep traps. Under proper conditions, these devices exhibit S-type differential negative resistance (DNR) similar to silicon-controlled rectifiers. With the added influence of a <span class="hlt">p</span>+ gate appropriately placed between the anode (<span class="hlt">p</span>+) and cathode (<span class="hlt">n</span>+), the current-voltage characteristic of the device has been manipulated for the first time to exhibit a variable <span class="hlt">N</span>-type DNR. The anode current and the anode-to-cathode voltage levels at which this <span class="hlt">N</span>-type DNR is observed can be varied by changing the gate-to-cathode bias. In essence, the classical S-type DI <span class="hlt">diode</span> can be electronically transformed into an <span class="hlt">N</span>-type <span class="hlt">diode</span>. A first-order phenomenological model is proposed for the <span class="hlt">N</span>-type DNR.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ITNS...60.2888M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ITNS...60.2888M"><span>Low Energy X-Ray and γ-Ray <span class="hlt">Detectors</span> Fabricated on <span class="hlt">n</span>-Type 4H-SiC Epitaxial Layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mandal, Krishna C.; Muzykov, Peter G.; Chaudhuri, Sandeep K.; Terry, J. Russell</p> <p>2013-08-01</p> <p>Schottky barrier <span class="hlt">diode</span> (SBD) radiation <span class="hlt">detectors</span> have been fabricated on <span class="hlt">n</span>-type 4H-SiC epitaxial layers and evaluated for low energy x- and γ-rays detection. The <span class="hlt">detectors</span> were found to be highly sensitive to soft x-rays in the 50 eV to few keV range and showed 2.1 % energy resolution for 59.6 keV gamma rays. The response to soft x-rays for these <span class="hlt">detectors</span> was significantly higher than that of commercial off-the-shelf (COTS) SiC UV photodiodes. The devices have been characterized by current-voltage (<span class="hlt">I</span>-V) measurements in the 94-700 K range, thermally stimulated current (TSC) spectroscopy, x-ray diffraction (XRD) rocking curve measurements, and defect delineating chemical etching. <span class="hlt">I</span>-V characteristics of the <span class="hlt">detectors</span> at 500 K showed low leakage current ( <span class="hlt">n</span>A at 200 V) revealing a possibility of high temperature operation. The XRD rocking curve measurements revealed high quality of the epitaxial layer exhibiting a full width at half maximum (FWHM) of the rocking curve 3.6 arc sec. TSC studies in a wide range of temperature (94-550 K) revealed presence of relatively shallow levels ( 0.25 eV) in the epi bulk with a density 7×1013 cm-3 related to Al and B impurities and deeper levels located near the metal-semiconductor interface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA248645','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA248645"><span>Noncontact Characterization of PV <span class="hlt">Detector</span> Arrays</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1990-06-01</p> <p>11-7 3 III <span class="hlt">DIODE</span> ARRAY AS A SAW CONVOLVER/STORAGE CORRELATOR .... III-1 III.A NONLINEAR ( VARACTOR ) ACTION OF THE <span class="hlt">DIODES</span> .......................... <span class="hlt">I</span>...associated with the <span class="hlt">diodes</span> in the <span class="hlt">detector</span> array. The varactor action of the <span class="hlt">diodes</span> produces a voltage across the <span class="hlt">diodes</span> which is pro- portional to the...type of interactions desired herein. An alternative approach is to em- ploy thin dielectric overlays, such as zinc oxide or silicon nitride</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017RScI...88l3503L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017RScI...88l3503L"><span>A fast-neutron detection <span class="hlt">detector</span> based on fission material and large sensitive 4H silicon carbide Schottky <span class="hlt">diode</span> <span class="hlt">detector</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Linyue; Liu, Jinliang; Zhang, Jianfu; Chen, Liang; Zhang, Xianpeng; Zhang, Zhongbing; Ruan, Jinlu; Jin, Peng; Bai, Song; Ouyang, Xiaoping</p> <p>2017-12-01</p> <p>Silicon carbide radiation <span class="hlt">detectors</span> are attractive in the measurement of the total numbers of pulsed fast neutrons emitted from nuclear fusion and fission devices because of high neutron-gamma discrimination and good radiation resistance. A fast-neutron detection system was developed based on a large-area 4H-SiC Schottky <span class="hlt">diode</span> <span class="hlt">detector</span> and a 235U fission target. Excellent pulse-height spectra of fission fragments induced by mono-energy deuterium-tritium (D-T) fusion neutrons and continuous energy fission neutrons were obtained. The <span class="hlt">detector</span> is proven to be a good candidate for pulsed fast neutron detection in a complex radiation field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19198430','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19198430"><span>Insertion of two-dimensional photonic crystal pattern on <span class="hlt">p-GaN</span> layer of Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> using bi-layer nanoimprint lithography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Byeon, Kyeong-Jae; Hwang, Seon-Yong; Hong, Chang-Hee; Baek, Jong Hyeob; Lee, Heon</p> <p>2008-10-01</p> <p>Nanoimprint lithography (NIL) was adapted to fabricate two-dimensional (2-D) photonic crystal (PC) pattern on the <span class="hlt">p-GaN</span> layer of InGa<span class="hlt">N/GaN</span> multi quantum well light-emitting <span class="hlt">diodes</span> (LEDs) structure to improve the light extraction efficiency. For the uniform transfer of the PC pattern, a bi-layer imprinting method with liquid phase resin was used. The <span class="hlt">p-GaN</span> layer was patterned with a periodic array of holes by an inductively coupled plasma etching process, based on SiCl4/Ar plasmas. As a result, 2-D photonic crystal patterns with 144 nm, 200 nm and 347 nm diameter holes were uniformly formed on the <span class="hlt">p-GaN</span> layer and the photoluminescence (PL) intensity of each patterned LED samples was increased by more than 2.6 times, as compared to that of the un-patterned LED sample.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DNP.PJ006W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DNP.PJ006W"><span>Use of Ga<span class="hlt">N</span> as a Scintillating Ionizing Radiation <span class="hlt">Detector</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wensman, Johnathan; Guardala, Noel; Mathur, Veerendra; Alasagas, Leslie; Vanhoy, Jeffrey; Statham, John; Marron, Daniel; Millett, Marshall; Marsh, Jarrod; Currie, John; Price, Jack</p> <p>2017-09-01</p> <p>Gallium nitride (Ga<span class="hlt">N</span>) is a III/V direct bandgap semiconductor which has been used in light emitting <span class="hlt">diodes</span> (LEDs) since the 1990s. Currently, due to a potential for increased efficiency, Ga<span class="hlt">N</span> is being investigated as a replacement for silicon in power electronics finding potential uses ranging from data centers to electric vehicles. In addition to LEDs and power electronics though, doped Ga<span class="hlt">N</span> can be used as a gamma insensitive fast neutron <span class="hlt">detector</span> due to the direct band-gap, light propagation properties, and response to ionizing radiations. Investigation of Ga<span class="hlt">N</span> as a semiconductor scintillator for use in a radiation detection system involves mapping the response function of the <span class="hlt">detector</span> crystal over a range of photon and neutron energies, and measurements of light generation in the Ga<span class="hlt">N</span> crystal due to proton, alpha, and nitrogen projectiles. In this presentation we discuss the measurements made to date, and plausible interpretations of the response functions. This work funded in part by the Naval Surface Warfare Center, Carderock Division In-house Laboratory Independent Research program.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_12 --> <div id="page_13" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="241"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4257526','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4257526"><span>Electroluminescence of ordered ZnO nanorod array/<span class="hlt">p-GaN</span> light-emitting <span class="hlt">diodes</span> with graphene current spreading layer</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2014-01-01</p> <p>Ordered ZnO nanorod array/<span class="hlt">p-GaN</span> heterojunction light-emitting <span class="hlt">diodes</span> (LEDs) have been fabricated by introducing graphene as the current spreading layer, which exhibit improved electroluminescence performance by comparison to the LED using a conventional structure (indium-tin-oxide as the current spreading layer). In addition, by adjusting the diameter of ZnO nanorod array in use, the light emission of the ZnO nanorod array/<span class="hlt">p-GaN</span> heterojunction LEDs was enhanced further. This work has great potential applications in solid-state lighting, high performance optoelectronic devices, and so on. PACS 78.60.Fi; 85.60.Jb; 78.67.Lt; 81.10.Dn PMID:25489284</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25489284','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25489284"><span>Electroluminescence of ordered ZnO nanorod array/<span class="hlt">p-GaN</span> light-emitting <span class="hlt">diodes</span> with graphene current spreading layer.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dong, Jing-Jing; Hao, Hui-Ying; Xing, Jie; Fan, Zhen-Jun; Zhang, Zi-Li</p> <p>2014-01-01</p> <p>Ordered ZnO nanorod array/<span class="hlt">p-GaN</span> heterojunction light-emitting <span class="hlt">diodes</span> (LEDs) have been fabricated by introducing graphene as the current spreading layer, which exhibit improved electroluminescence performance by comparison to the LED using a conventional structure (indium-tin-oxide as the current spreading layer). In addition, by adjusting the diameter of ZnO nanorod array in use, the light emission of the ZnO nanorod array/<span class="hlt">p-GaN</span> heterojunction LEDs was enhanced further. This work has great potential applications in solid-state lighting, high performance optoelectronic devices, and so on. 78.60.Fi; 85.60.Jb; 78.67.Lt; 81.10.Dn.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApPhL.111u2102W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhL.111u2102W"><span>Asymmetrical quantum well degradation of InGa<span class="hlt">N/GaN</span> blue laser <span class="hlt">diodes</span> characterized by photoluminescence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wen, Pengyan; Liu, Jianping; Zhang, Shuming; Zhang, Liqun; Ikeda, Masao; Li, Deyao; Tian, Aiqin; Zhang, Feng; Cheng, Yang; Zhou, Wei; Yang, Hui</p> <p>2017-11-01</p> <p>The temperature, power, and voltage dependent photoluminescence spectra are studied in InGa<span class="hlt">N/GaN</span> double quantum well blue laser <span class="hlt">diodes</span>. Emissions from the two quantum wells can be distinguished at low temperature at low excitation power density due to the different built-in electric field in the two quantum wells. This finding is utilized to study the degradation of InGa<span class="hlt">N/GaN</span> blue laser <span class="hlt">diodes</span>. Two peaks are observed for the non-aged laser <span class="hlt">diode</span> (LD), while one peak for the aged LD which performed 3200 h until no laser output is detected. The disappearance of the high energy peak in the photoluminescence spectra indicates a heavier degradation of the quantum well on the <span class="hlt">p</span>-side, which agrees with our previous observation that both the linewidth and the potential fluctuation of InGa<span class="hlt">N</span> quantum wells (QWs) reduced for the aged LDs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010NIMPA.623..177A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010NIMPA.623..177A"><span>Collected charge of planar silicon <span class="hlt">detectors</span> after pion and proton irradiations up to 2.2 ×10 16 <span class="hlt">n</span> eq cm -2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Affolder, Anthony; Allport, Phil; Casse, Gianluigi</p> <p>2010-11-01</p> <p>The planned luminosity upgrade of the Large Hadron Collider at CERN (Super-LHC) will provide a challenging environment for the tracking and vertexing <span class="hlt">detector</span> systems. Planar, segmented silicon <span class="hlt">detectors</span> are one of the few radiation tolerant technologies under consideration for use for the Super-LHC tracking <span class="hlt">detectors</span> in either pixel or strip geometries. In this paper, charge collection measurements are made with planar silicon sensors with 2 different substrate materials (float zone and magnetic Czochralski) and 3 different <span class="hlt">diode</span> configurations (<span class="hlt">p</span>+ strip in <span class="hlt">n</span>-bulk, <span class="hlt">n</span>+ strip in <span class="hlt">n</span>-bulk, and <span class="hlt">n</span>+ strip in <span class="hlt">p</span>-bulk). For the first time, a comparison of the charge collection of these devices will be made after irradiation up to 6 ×1014 neq cm-2 with 280 MeV charged pions, and up to 2.2 ×1016 neq cm-2 with 26 MeV protons. This study covers the expected range of final fluences for the different layers of pixel and microstrip sensors of the ATLAS and CMS experiments at the Super-LHC. These measurements have been carried out using analogue, high-speed (40 MHz) electronics and a Strontium-90 beta source.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24150379','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24150379"><span>Size-controllable nanopyramids photonic crystal selectively grown on <span class="hlt">p-GaN</span> for enhanced light-extraction of light-emitting <span class="hlt">diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Du, Chengxiao; Wei, Tongbo; Zheng, Haiyang; Wang, Liancheng; Geng, Chong; Yan, Qingfeng; Wang, Junxi; Li, Jinmin</p> <p>2013-10-21</p> <p>Size-controllable <span class="hlt">p-GaN</span> hexagonal nanopyramids (HnPs)-photonic crystal (PhC) structures were selectively grown on flat <span class="hlt">p-GaN</span> layer for the elimination of total internal reflection of light-emitting <span class="hlt">diodes</span> (LEDs). The LEDs with HnPs-PhC of 46.3% bottom fill factor (PhC lattice constant is 730 nm) showed an improved light output power by 99.9% at forward current of 350 mA compared to the reference LEDs with flat <span class="hlt">p-GaN</span> layer. We confirmed the effect of HnPs-PhC with different bottom fill factors and the effect of nanopyramid-shaped and nanocolumn-shaped PhC on the light-extraction of LEDs was also investigated by using three-dimensional finite-difference time-domain simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NatSR...629535G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NatSR...629535G"><span>X-ray detection with zinc-blende (cubic) Ga<span class="hlt">N</span> Schottky <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gohil, T.; Whale, J.; Lioliou, G.; Novikov, S. V.; Foxon, C. T.; Kent, A. J.; Barnett, A. M.</p> <p>2016-07-01</p> <p>The room temperature X-ray responses as functions of time of two <span class="hlt">n</span> type cubic Ga<span class="hlt">N</span> Schottky <span class="hlt">diodes</span> (200 μm and 400 μm diameters) are reported. The current densities as functions of time for both <span class="hlt">diodes</span> showed fast turn-on transients and increases in current density when illuminated with X-ray photons of energy up to 35 keV. The <span class="hlt">diodes</span> were also electrically characterized: capacitance, implied depletion width and dark current measurements as functions of applied bias at room temperature are presented. At -5 V reverse bias, the capacitances of the <span class="hlt">diodes</span> were measured to be (84.05 ± 0.01) <span class="hlt">p</span>F and (121.67 ± 0.02) <span class="hlt">p</span>F, respectively. At -5 V reverse bias, the dark current densities of the <span class="hlt">diodes</span> were measured to be (347.2 ± 0.4) mA cm-2 and (189.0 ± 0.2) mA cm-2, respectively. The Schottky barrier heights of the devices (0.52 ± 0.07) eV and (0.63 ± 0.09) eV, respectively, were extracted from the forward dark current characteristics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23454962','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23454962"><span>Enhanced hole transport in InGa<span class="hlt">N/GaN</span> multiple quantum well light-emitting <span class="hlt">diodes</span> with a <span class="hlt">p</span>-type doped quantum barrier.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ji, Yun; Zhang, Zi-Hui; Tan, Swee Tiam; Ju, Zhen Gang; Kyaw, Zabu; Hasanov, Namig; Liu, Wei; Sun, Xiao Wei; Demir, Hilmi Volkan</p> <p>2013-01-15</p> <p>We study hole transport behavior of InGa<span class="hlt">N/GaN</span> light-emitting <span class="hlt">diodes</span> with the dual wavelength emission method. It is found that at low injection levels, light emission is mainly from quantum wells near <span class="hlt">p-GaN</span>, indicating that hole transport depth is limited in the active region. Emission from deeper wells only occurs under high current injection. However, with Mg-doped quantum barriers, holes penetrate deeper within the active region even under low injection, increasing the radiative recombination. Moreover, the improved hole transport leads to reduced forward voltage and enhanced light generation. This is also verified by numerical analysis of hole distribution and energy band structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JPhCS.606a2007P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JPhCS.606a2007P"><span>Experience from operating germanium <span class="hlt">detectors</span> in GERDA</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Palioselitis, Dimitrios; GERDA Collaboration</p> <p>2015-05-01</p> <p>Phase <span class="hlt">I</span> of the Germanium <span class="hlt">Detector</span> Array (GERDA) experiment, searching for the neutrinoless double beta (0νββ) decay of 76Ge, was completed in September 2013. The most competitive half-life lower limit for the 0νββ decay of 76Ge was set (T-0ν1/2 > 2.1 · 1025 yr at 90% C.L.). GERDA operates bare Ge <span class="hlt">diodes</span> immersed in liquid argon. During Phase <span class="hlt">I</span>, mainly refurbished semi-coaxial high purity Ge <span class="hlt">detectors</span> from previous experiments were used. The experience gained with handling and operating bare Ge <span class="hlt">diodes</span> in liquid argon, as well as the stability and performance of the <span class="hlt">detectors</span> during GERDA Phase <span class="hlt">I</span> are presented. Thirty additional new enriched BEGe-type <span class="hlt">detectors</span> were produced and will be used in Phase II. A subgroup of these <span class="hlt">detectors</span> has already been used successfully in GERDA Phase <span class="hlt">I</span>. The present paper gives an overview of the production chain of the new germanium <span class="hlt">detectors</span>, the steps taken to minimise the exposure to cosmic radiation during manufacturing, and the first results of characterisation measurements in vacuum cryostats.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AIPC..613.1620C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AIPC..613.1620C"><span>A new cryogenic <span class="hlt">diode</span> thermometer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Courts, S. S.; Swinehart, P. R.; Yeager, C. J.</p> <p>2002-05-01</p> <p>While the introduction of yet another cryogenic <span class="hlt">diode</span> thermometer is not earth shattering, a new <span class="hlt">diode</span> thermometer, the DT-600 series, recently introduced by Lake Shore Cryotronics, possesses three features that make it unique among commercial <span class="hlt">diode</span> thermometers. First, these <span class="hlt">diodes</span> have been probed at the chip level, allowing for the availability of a bare chip thermometer matching a standard curve-an important feature in situations where real estate is at a premium (IR <span class="hlt">detectors</span>), or where in-situ calibration is difficult. Second, the thermometry industry has assumed that interchangeability should be best at low temperatures. Thus, good interchangeability at room temperatures implies a very good interchangeability at cryogenic temperature, resulting in a premium priced sensor. The DT-600 series <span class="hlt">diode</span> thermometer is available in an interchangeability band comparable to platinum RTDs with the added advantage of interchangeability to 2 K. Third, and most important, the DT-600 series <span class="hlt">diode</span> does not exhibit an instability in the <span class="hlt">I</span>-V characteristic in the 8 K to 20 K temperature range that is observed in other commercial <span class="hlt">diode</span> thermometer devices [1]. This paper presents performance characteristics for the DT-600 series <span class="hlt">diode</span> thermometer along with a comparison of <span class="hlt">I</span>-V curves for this device and other commercial <span class="hlt">diode</span> thermometers exhibiting an <span class="hlt">I</span>-V instability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22267943-pn0-i+-breast-cancer-treatment-patterns-locoregional-recurrence-survival-outcomes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22267943-pn0-i+-breast-cancer-treatment-patterns-locoregional-recurrence-survival-outcomes"><span><span class="hlt">pN</span>0(<span class="hlt">i</span>+) Breast Cancer: Treatment Patterns, Locoregional Recurrence, and Survival Outcomes</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Karam, Irene; Breast Cancer Outcomes Unit, British Columbia Cancer Agency, Vancouver, BC; Lesperance, Maria F.</p> <p></p> <p>Purpose: To examine treatment patterns, recurrence, and survival outcomes in patients with <span class="hlt">pN</span>0(<span class="hlt">i</span>+) breast cancer. Methods and Materials: Subjects were 5999 women with AJCC (6th edition) <span class="hlt">p</span>T1-3, <span class="hlt">pN</span>0-<span class="hlt">N</span>1a, M0 breast cancer diagnosed between 2003 and 2006. Of these, 4342 (72%) had <span class="hlt">pN</span>0, 96 (2%) had <span class="hlt">pN</span>0(<span class="hlt">i</span>+), 349 (6%) had <span class="hlt">p</span>Nmic (micrometastases >0.2 mm to ≤2 mm), and 1212 (20%) had <span class="hlt">pN</span>1a (1-3 positive macroscopic nodes) disease. Treatment characteristics and 5-year Kaplan-Meier local recurrence, regional recurrence (RR), locoregional recurrence (LRR), and overall survival were compared between nodal subgroups. Multivariable analysis was performed using Cox regression modeling. A 1:3 case-match analysis examinedmore » outcomes in <span class="hlt">pN</span>0(<span class="hlt">i</span>+) cases compared with <span class="hlt">pN</span>0 controls matched for similar tumor and treatment characteristics. Results: Median follow-up was 4.8 years. Adjuvant systemic therapy use increased with nodal stage: 81%, 92%, 95%, and 94% in <span class="hlt">pN</span>0, <span class="hlt">pN</span>0(<span class="hlt">i</span>+), <span class="hlt">p</span>Nmic, and <span class="hlt">pN</span>1a disease, respectively (<span class="hlt">P</span><.001). Nodal radiation therapy (RT) use also increased with nodal stage: 1.7% in <span class="hlt">pN</span>0, 27% in <span class="hlt">pN</span>0(<span class="hlt">i</span>+), 33% in <span class="hlt">p</span>Nmic, and 63% in <span class="hlt">pN</span>1a cohorts (<span class="hlt">P</span><.001). Five-year Kaplan-Meier outcomes in <span class="hlt">pN</span>0 versus <span class="hlt">pN</span>0(<span class="hlt">i</span>+) cases were as follows: local recurrence 1.7% versus 3.7% (<span class="hlt">P</span>=.20), RR 0.5% versus 2.2% (<span class="hlt">P</span>=.02), and LRR 2.1% versus 5.8% (<span class="hlt">P</span>=.02). There were no RR events in 26 patients with <span class="hlt">pN</span>0(<span class="hlt">i</span>+) disease who received nodal RT and 2 RR events in 70 patients who did not receive nodal RT. On multivariable analysis, <span class="hlt">pN</span>0(<span class="hlt">i</span>+) was not associated with worse locoregional control or survival. On case-match analysis, LRR and overall survival were similar between <span class="hlt">pN</span>0(<span class="hlt">i</span>+) and matched <span class="hlt">pN</span>0 counterparts. Conclusions: Nodal involvement with isolated tumor cells is not a significant prognostic factor for LRR or survival in this study's multivariable and case-match analyses. These data do not support the routine use of nodal RT in the setting of <span class="hlt">pN</span>0(<span class="hlt">i</span>+) disease. Prospective studies are needed to define</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1289617-high-voltage-high-current-density-vertical-gan-power-diodes','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1289617-high-voltage-high-current-density-vertical-gan-power-diodes"><span>High voltage and high current density vertical Ga<span class="hlt">N</span> power <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Fischer, A. J.; Dickerson, J. R.; Armstrong, A. M.; ...</p> <p>2016-01-01</p> <p>We report on the realization of a Ga<span class="hlt">N</span> high voltage vertical <span class="hlt">p-n</span> <span class="hlt">diode</span> operating at > 3.9 kV breakdown with a specific on-resistance < 0.9 mΩ.cm 2. <span class="hlt">Diodes</span> achieved a forward current of 1 A for on-wafer, DC measurements, corresponding to a current density > 1.4 kA/cm 2. An effective critical electric field of 3.9 MV/cm was estimated for the devices from analysis of the forward and reverse current-voltage characteristics. Furthermore this suggests that the fundamental limit to the Ga<span class="hlt">N</span> critical electric field is significantly greater than previously believed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009PhyB..404.4889P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009PhyB..404.4889P"><span>Deep level transient spectroscopy signatures of majority traps in Ga<span class="hlt">N</span> <span class="hlt">p-n</span> <span class="hlt">diodes</span> grown by metal-organic vapor-phase epitaxy technique on Ga<span class="hlt">N</span> substrates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>PŁaczek-Popko, E.; Trzmiel, J.; Zielony, E.; Grzanka, S.; Czernecki, R.; Suski, T.</p> <p>2009-12-01</p> <p>In this study, we present the results of investigation on <span class="hlt">p-n</span> Ga<span class="hlt">N</span> <span class="hlt">diodes</span> by means of deep level transient spectroscopy (DLTS) within the temperature range of 77-350 K. Si-doped Ga<span class="hlt">N</span> layers were grown by metal-organic vapor-phase epitaxy technique (MOVPE) on the free-standing Ga<span class="hlt">N</span> substrates. Subsequently Mg-doped Ga<span class="hlt">N</span> layers were grown. To perform DLTS measurements Ni/Au contacts to <span class="hlt">p</span>-type material and Ti/Au contacts to <span class="hlt">n</span>-type material were processed. DLTS signal spectra revealed the presence of two majority traps of activation energies obtained from Arrhenius plots equal to E1=0.22 eV and E2=0.65 eV. In present work we show that the trap E1 is linked with the extended defects whereas the trap E2 is the point defect related. Its capture cross section is thermally activated with energy barrier for capture equal to 0.2 eV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2956611','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2956611"><span>A Planar, Chip-Based, Dual-Beam Refractometer Using an Integrated Organic Light Emitting <span class="hlt">Diode</span> (OLED) Light Source and Organic Photovoltaic (OPV) <span class="hlt">Detectors</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ratcliff, Erin L.; Veneman, P. Alex; Simmonds, Adam; Zacher, Brian; Huebner, Daniel</p> <p>2010-01-01</p> <p>We present a simple chip-based refractometer with a central organic light emitting <span class="hlt">diode</span> (OLED) light source and two opposed organic photovoltaic (OPV) <span class="hlt">detectors</span> on an internal reflection element (IRE) substrate, creating a true dual-beam sensor platform. For first-generation platforms, we demonstrate the use of a single heterojunction OLED based on electroluminescence emission from an Alq3/TPD heterojunction (tris-(8-hydroxyquinoline)aluminum/<span class="hlt">N</span>,N′-Bis(3-methylphenyl)-<span class="hlt">N</span>,N′-diphenylbenzidine) and light detection with planar heterojunction pentacene/C60 OPVs. The sensor utilizes the considerable fraction of emitted light from conventional thin film OLEDs that is coupled into guided modes in the IRE instead of into the forward (display) direction. A ray-optics description is used to describe light throughput and efficiency-limiting factors for light coupling from the OLED into the substrate modes, light traversing through the IRE substrate, and light coupling into the OPV <span class="hlt">detectors</span>. The arrangement of the OLED at the center of the chip provides for two sensing regions, a “sample” and “reference” channel, with detection of light by independent OPV <span class="hlt">detectors</span>. This configuration allows for normalization of the sensor response against fluctuations in OLED light output, stability, and local fluctuations (temperature) which might influence sensor response. The dual beam configuration permits significantly enhanced sensitivity to refractive index changes relative to single-beam protocols, and is easily integrated into a field-portable instrumentation package. Changes in refractive index (ΔR.<span class="hlt">I</span>.) between 10−2 and 10−3 R.<span class="hlt">I</span>. units could be detected for single channel operation, with sensitivity increased to ΔR.<span class="hlt">I</span>. ≈ 10−4 units when the dual beam configuration is employed. PMID:20218580</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..MAR.J5008T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..MAR.J5008T"><span>Electrical contact of wurtzite Ga<span class="hlt">N</span> mircrodisks on <span class="hlt">p</span>-type Ga<span class="hlt">N</span> template</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsai, Cheng-Da; Lo, Ikai; Wang, Ying-Chieh; Hsu, Yu-Chi; Shih, Cheng-Hung; Pang, Wen-Yuan; You, Shuo-Ting; Hu, Chia-Hsuan; Chou, Mitch M. C.; Yang, Chen-Chi; Lin, Yu-Chiao</p> <p>2015-03-01</p> <p>We developed a back processing to fabricate a secure electrical contact of wurtzite Ga<span class="hlt">N</span> microdisk on a transparent <span class="hlt">p</span>-type Ga<span class="hlt">N</span> template with the orientation, [10-10]disk // [10-10]template. Ga<span class="hlt">N</span> microdisks were grown on LiAlO2 substrate by using plasma-assisted molecular beam epitaxy. In the further study, we analyzed the TEM specimen of a sample with annealed Ga<span class="hlt">N</span> microdisk/<span class="hlt">p</span>-typed Ga<span class="hlt">N</span> template by selection area diffraction (SAD) to confirm the alignment of the microdisks with the template at the interface. From the <span class="hlt">I</span>-V measurements performed on the samples, we obtained a threshold voltage of ~ 5.9 V for the current passing through the Ga<span class="hlt">N</span> microdisks with a resistance of ~ 45 K Ω. The electrical contact can be applied to the nanometer-scaled Ga<span class="hlt">N</span> light-emitting <span class="hlt">diode</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22649259-su-verification-dose-distributions-from-high-dose-rate-brachytherapy-ir-source-using-multiple-array-diode-detector-mapcheck2','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22649259-su-verification-dose-distributions-from-high-dose-rate-brachytherapy-ir-source-using-multiple-array-diode-detector-mapcheck2"><span>SU-G-201-17: Verification of Dose Distributions From High-Dose-Rate Brachytherapy Ir-192 Source Using a Multiple-Array-<span class="hlt">Diode-Detector</span> (MapCheck2)</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Harpool, K; De La Fuente Herman, T; Ahmad, S</p> <p></p> <p>Purpose: To investigate quantitatively the accuracy of dose distributions for the Ir-192 high-dose-rate (HDR) brachytherapy source calculated by the Brachytherapy-Planning system (BPS) and measured using a multiple-array-<span class="hlt">diode-detector</span> in a heterogeneous medium. Methods: A two-dimensional <span class="hlt">diode-array-detector</span> system (MapCheck2) was scanned with a catheter and the CT-images were loaded into the Varian-Brachytherapy-Planning which uses TG-43-formalism for dose calculation. Treatment plans were calculated for different combinations of one dwell-position and varying irradiation times and different-dwell positions and fixed irradiation time with the source placed 12mm from the <span class="hlt">diode</span>-array plane. The calculated dose distributions were compared to the measured doses with MapCheck2 delivered bymore » an Ir-192-source from a Nucletron-Microselectron-V2-remote-after-loader. The linearity of MapCheck2 was tested for a range of dwell-times (2–600 seconds). The angular effect was tested with 30 seconds irradiation delivered to the central-<span class="hlt">diode</span> and then moving the source away in increments of 10mm. Results: Large differences were found between calculated and measured dose distributions. These differences are mainly due to absence of heterogeneity in the dose calculation and <span class="hlt">diode</span>-artifacts in the measurements. The dose differences between measured and calculated due to heterogeneity ranged from 5%–12% depending on the position of the source relative to the <span class="hlt">diodes</span> in MapCheck2 and different heterogeneities in the beam path. The linearity test of the <span class="hlt">diode-detector</span> showed 3.98%, 2.61%, and 2.27% over-response at short irradiation times of 2, 5, and 10 seconds, respectively, and within 2% for 20 to 600 seconds (<span class="hlt">p</span>-value=0.05) which depends strongly on MapCheck2 noise. The angular dependency was more pronounced at acute angles ranging up to 34% at 5.7 degrees. Conclusion: Large deviations between measured and calculated dose distributions for HDR-brachytherapy with Ir-192 may</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApPhL.106f3501Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApPhL.106f3501Z"><span>A hole modulator for InGa<span class="hlt">N/GaN</span> light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Zi-Hui; Kyaw, Zabu; Liu, Wei; Ji, Yun; Wang, Liancheng; Tan, Swee Tiam; Sun, Xiao Wei; Demir, Hilmi Volkan</p> <p>2015-02-01</p> <p>The low <span class="hlt">p</span>-type doping efficiency of the <span class="hlt">p-GaN</span> layer has severely limited the performance of InGa<span class="hlt">N/GaN</span> light-emitting <span class="hlt">diodes</span> (LEDs) due to the ineffective hole injection into the InGa<span class="hlt">N/GaN</span> multiple quantum well (MQW) active region. The essence of improving the hole injection efficiency is to increase the hole concentration in the <span class="hlt">p-GaN</span> layer. Therefore, in this work, we have proposed a hole modulator and studied it both theoretically and experimentally. In the hole modulator, the holes in a remote <span class="hlt">p</span>-type doped layer are depleted by the built-in electric field and stored in the <span class="hlt">p-GaN</span> layer. By this means, the overall hole concentration in the <span class="hlt">p-GaN</span> layer can be enhanced. Furthermore, the hole modulator is adopted in the InGa<span class="hlt">N/GaN</span> LEDs, which reduces the effective valance band barrier height for the <span class="hlt">p</span>-type electron blocking layer from ˜332 meV to ˜294 meV at 80 A/cm2 and demonstrates an improved optical performance, thanks to the increased hole concentration in the <span class="hlt">p-GaN</span> layer and thus the improved hole injection into the MQWs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1211345-comprehensive-study-electronic-optical-behavior-highly-degenerate-type-mg-doped-gan-algan','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1211345-comprehensive-study-electronic-optical-behavior-highly-degenerate-type-mg-doped-gan-algan"><span>Comprehensive study of the electronic and optical behavior of highly degenerate <span class="hlt">p</span>-type Mg-doped Ga<span class="hlt">N</span> and AlGa<span class="hlt">N</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Gunning, BP; Fabien, CAM; Merola, JJ</p> <p>2015-01-28</p> <p>The bulk and 2-dimensional (2D) electrical transport properties of heavily Mg-doped <span class="hlt">p</span>-type Ga<span class="hlt">N</span> films grown on Al<span class="hlt">N</span> buffer layers by Metal Modulated Epitaxy are explored. Distinctions are made between three primary <span class="hlt">p</span>-type conduction mechanisms: traditional valence band conduction, impurity band conduction, and 2D conduction within a 2D hole gas at a hetero-interface. The bulk and 2D contributions to the overall carrier transport are identified and the relative contributions are found to vary strongly with growth conditions. Films grown with III/V ratio less than 1.5 exhibit high hole concentrations exceeding 2 x 10(19) cm(-3) with effective acceptor activation energies of 51more » meV. Films with III/V ratios greater than 1.5 exhibit lower overall hole concentrations and significant contributions from 2D transport at the hetero-interface. Films grown with III/V ratio of 1.2 and Mg concentrations exceeding 2 x 10(20) cm(-3) show no detectable inversion domains or Mg precipitation. Highly Mg-doped <span class="hlt">p-GaN</span> and <span class="hlt">p-AlGaN</span> with Al fractions up to 27% similarly exhibit hole concentrations exceeding 2 x 10(19) cm(-3). The <span class="hlt">p-GaN</span> and <span class="hlt">p</span>-Al0.11Ga0.89<span class="hlt">N</span> films show broad ultraviolet (UV) photoluminescence peaks, which intercept the valence band, supporting the presence of a Mg acceptor band. Finally, a multi-quantum-well light-emitting <span class="hlt">diode</span> (LED) and <span class="hlt">p-i-n</span> <span class="hlt">diode</span> are grown, both of which demonstrate rectifying behavior with turn-on voltages of 3-3.5V and series resistances of 6-10 Omega without the need for any post-metallization annealing. The LED exhibits violet-blue luminescence at 425 nm, while the <span class="hlt">p-i-n</span> <span class="hlt">diode</span> shows UV luminescence at 381 nm, and both devices still show substantial light emission even when submerged in liquid nitrogen at 77 K. (C) 2015 AIP Publishing LLC.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApPhL.106h3502H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApPhL.106h3502H"><span>Current transient spectroscopy for trapping analysis on Au-free AlGa<span class="hlt">N/GaN</span> Schottky barrier <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hu, J.; Stoffels, S.; Lenci, S.; Bakeroot, B.; Venegas, R.; Groeseneken, G.; Decoutere, S.</p> <p>2015-02-01</p> <p>This paper presents a combined technique of high voltage off-state stress and current transient measurements to investigate the trapping/de-trapping characteristics of Au-free AlGa<span class="hlt">N/GaN</span> Schottky barrier <span class="hlt">diodes</span>. The device features a symmetric three-terminal structure with a central anode contact surrounded by two separate cathodes. Under the <span class="hlt">diode</span> off-state stress conditions, the two separate cathodes were electrically shorted. The de-trapping dynamics was studied by monitoring the recovery of the two-dimensional electron gas (2DEG) current at different temperatures by applying 0.5 V at cathode 2 while grounding cathode 1. During the recovery, the anode contact acts as a sensor of changes in <span class="hlt">diode</span> leakage current. This leakage variation was found to be mainly due to the barrier height variation. With this method, the energy level and capture cross section of different traps in the AlGa<span class="hlt">N/GaN</span> Schottky barrier <span class="hlt">diode</span> can be extracted. Furthermore, the physical location of different trapping phenomena is indicated by studying the variation of the <span class="hlt">diode</span> leakage current during the recovery. We have identified two distinct trapping mechanisms: (<span class="hlt">i</span>) electron trapping at the AlGa<span class="hlt">N</span> surface in the vicinity of the Schottky contact which results in the leakage reduction (barrier height ϕB increase) together with RON degradation; (ii) the electron trapping in the Ga<span class="hlt">N</span> channel layer which partially depletes the 2DEG. The physical origin of the two different traps is discussed in the text.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22253107-effects-mg-doped-aln-algan-superlattices-properties-gan-contact-layer-performance-deep-ultraviolet-light-emitting-diodes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22253107-effects-mg-doped-aln-algan-superlattices-properties-gan-contact-layer-performance-deep-ultraviolet-light-emitting-diodes"><span>Effects of Mg-doped Al<span class="hlt">N/AlGaN</span> superlattices on properties of <span class="hlt">p-GaN</span> contact layer and performance of deep ultraviolet light emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Al tahtamouni, T. M., E-mail: talal@yu.edu.jo; Lin, J. Y.; Jiang, H. X.</p> <p>2014-04-15</p> <p>Mg-doped Al<span class="hlt">N/AlGaN</span> superlattice (Mg-SL) and Mg-doped AlGa<span class="hlt">N</span> epilayers have been investigated in the 284 nm deep ultraviolet (DUV) light emitting <span class="hlt">diodes</span> (LEDs) as electron blocking layers. It was found that the use of Mg-SL improved the material quality of the <span class="hlt">p-GaN</span> contact layer, as evidenced in the decreased density of surface pits and improved surface morphology and crystalline quality. The performance of the DUV LEDs fabricated using Mg-SL was significantly improved, as manifested by enhanced light intensity and output power, and reduced turn-on voltage. The improved performance is attributed to the enhanced blocking of electron overflow, and enhanced hole injection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JKPS...70..765Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JKPS...70..765Z"><span>Improvement of luster consistency between the <span class="hlt">p</span>-Pad and the <span class="hlt">n</span>-Pad of Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> via the under-etching process</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zheng, Chenju; Lv, Jiajiang; Zhou, Shengjun; Liu, Sheng</p> <p>2017-04-01</p> <p>For improvement of the light extraction efficiency of Ga<span class="hlt">N</span>-based lateral light-emitting <span class="hlt">diodes</span> (LEDs), a <span class="hlt">p-GaN</span> surface was textured through a low-temperature (850 °C) <span class="hlt">p-GaN</span> growth process. However, the <span class="hlt">p-GaN</span> texturing process caused luster inconsistency between the <span class="hlt">n</span>-pad and the <span class="hlt">p</span>-pad due to the roughness difference between the indium-tin oxide (ITO) and the <span class="hlt">n-GaN</span> beneath the pads, which decreased the image recognition rate and accuracy during the wire bonding process for LED packaging. Therefore, an under-etching process was proposed to improve the luster consistency between the <span class="hlt">p</span>-pad and the <span class="hlt">n</span>-pad of Ga<span class="hlt">N</span>-based LEDs with a naturally textured <span class="hlt">p-GaN</span> surface. The under-etching process decreased the roughness of the exposed <span class="hlt">n-GaN</span> surface from 109 nm to 73.1 nm, which was similar to the roughness (74.8 nm) of the ITO surface. Optical microscopy showed that LEDs with a naturally textured <span class="hlt">p-GaN</span> surface exhibited excellent luster consistency between the <span class="hlt">n</span>-pad and the <span class="hlt">p</span>-pad after the proposed under-etching process had been applied. Further analysis indicated that the LEDs with a naturally textured <span class="hlt">p-GaN</span> surface showed no degradation of optical or the electrical performance after the proposed under-etching process had been applied. At a 20-mA injection current, the light output power of a LED with naturally a textured <span class="hlt">p-GaN</span> surface was 8.7% higher than that of a LED with a smooth <span class="hlt">p-GaN</span> surface.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_13 --> <div id="page_14" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="261"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25857885','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25857885"><span>Validated HPLC-<span class="hlt">Diode</span> Array <span class="hlt">Detector</span> Method for Simultaneous Evaluation of Six Quality Markers in Coffee.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gant, Anastasia; Leyva, Vanessa E; Gonzalez, Ana E; Maruenda, Helena</p> <p>2015-01-01</p> <p>Nicotinic acid, <span class="hlt">N</span>-methylpyridinium ion, and trigonelline are well studied nutritional biomarkers present in coffee, and they are indicators of thermal decomposition during roasting. However, no method is yet available for their simultaneous determination. This paper describes a rapid and validated HPLC-<span class="hlt">diode</span> array <span class="hlt">detector</span> method for the simultaneous quantitation of caffeine, trigonelline, nicotinic acid, <span class="hlt">N</span>-methylpyridinium ion, 5-caffeoylquinic acid, and 5-hydroxymethyl furfural that is applicable to three coffee matrixes: green, roasted, and instant. Baseline separation among all compounds was achieved in 30 min using a phenyl-hexyl RP column (250×4.6 mm, 5 μm particle size), 0.3% aqueous formic buffer (<span class="hlt">p</span>H 2.4)-methanol mobile phase at a flow rate of 1 mL/min, and a column temperature at 30°C. The method showed good linear correlation (r2>0.9985), precision (less than 3.9%), sensitivity (LOD=0.023-0.237 μg/mL; LOQ=0.069-0.711 μg/mL), and recovery (84-102%) for all compounds. This simplified method is amenable for a more complete routine evaluation of coffee in industry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740002321','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740002321"><span>Development of a (Hg, Cd)Te photodiode <span class="hlt">detector</span>, Phase 2. [for 10.6 micron spectral region</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1972-01-01</p> <p>High speed sensitive (Hg,Cd)Te photodiode <span class="hlt">detectors</span> operating in the 77 to 90 K temperature range have been developed for the 10.6 micron spectral region. <span class="hlt">P-N</span> junctions formed by impurity (gold) diffusion in <span class="hlt">p</span>-type (Hg, Cd) Te have been investigated. It is shown that the bandwidth and quantum efficiency of a <span class="hlt">diode</span> are a constant for a fixed ratio of mobility/lifetime ratio of minority carriers. The minority carrier mobility and lifetime uniquely determine the bandwidth and quantum efficiency and indicate the shallow <span class="hlt">n</span> on <span class="hlt">p</span> (Hg,Cd) Te <span class="hlt">diodes</span> are preferable as high performance, high frequency devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950014108','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950014108"><span>Annealing of irradiated <span class="hlt">n+p</span> In<span class="hlt">P</span> buried homojunctions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Walters, Robert J.; Summers, Geoffrey P.; Timmons, M. L.; Venkatasubramanian, R.; Hancock, J. A.; Hills, J. S.</p> <p>1994-01-01</p> <p>At the last SPRAT conference, the Naval Research Laboratory (NRL) presented results from two experiments. One studied <span class="hlt">n+p</span> diffused junction (DJ) In<span class="hlt">P</span> solar cells, and the other studied <span class="hlt">n+p</span> shallow homojunction (SHJ) In<span class="hlt">P</span> mesa <span class="hlt">diodes</span> grown by metalorganic chemical vapor deposition (MOCVD). The former work showed that a DJ solar cell in which the maximum power <span class="hlt">P</span>(sub max) had been degraded by nearly 80 percent under irradiation recovered completely under short circuit illumination at 450K. The recovery was accompanied by the removal of all but one of the radiation-induced defect levels. The latter work, on the other hand, showed that the radiation-induced defects in the SHJ <span class="hlt">diodes</span> did not anneal until the temperature reached 650K. These results suggest that an irradiated DJ solar cell, under illumination, will anneal at a temperature 200K lower than an irradiated SHJ cell. This is an unexpected result considering the similarity of the devices. The goal of the present research is to explain this different behavior. This paper investigates two points which arose from the previous studies. The first point is that the DJ cells were annealed under illumination while the SHJ <span class="hlt">diodes</span> were annealed without bias. The second point investigated here is that the emitters of the DJ and SHJ devices were significantly different.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014NIMPB.339...20G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014NIMPB.339...20G"><span>The effects of high-energy uranium ion irradiation on Au/<span class="hlt">n-GaN</span> Schottky <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gou, J.; Zhang, C. H.; Zhang, L. Q.; Song, Y.; Wang, L. X.; Li, J. J.; Meng, Y. C.; Li, H. X.; Yang, Y. T.; Lu, Z. W.</p> <p>2014-11-01</p> <p>The <span class="hlt">I</span>-V and C-V characteristics of Au/<span class="hlt">n-GaN</span> Schottky <span class="hlt">diodes</span> irradiated with 290-MeV 238U32+ ions are presented. The U ions can penetrate the <span class="hlt">n</span>-type Ga<span class="hlt">N</span> epi-layer with a thickness about 3 μm grown on the c-plane of a sapphire substrate using the MOCVD technique, leaving a purely electronic energy deposition. The Au/<span class="hlt">n-GaN</span> Schottky <span class="hlt">diodes</span> were irradiated to successively increasing fluences from 1 × 109 to 5 × 1011 ions cm-2. The measured <span class="hlt">I</span>-V curves show that the height of the Schottky barrier decreases after irradiation and that the Schottky barrier almost disappears when the ion fluence reaches 5 × 1010 ions cm-2. Meanwhile, the irradiation increases the series resistance. The C-V curves show that the capacitance drops sharply when the ion fluence reaches 5 × 1010 ions cm-2. The dielectric constant also decreases following the irradiation. The changes of the electrical properties are ascribed to the neutralization of the donor-like surface state and the acceptor-like surface state due to the migration of Au atoms at the interface of Au/<span class="hlt">n-GaN</span> under energetic U ions irradiations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27998148','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27998148"><span>Sb2S3/Spiro-OMeTAD Inorganic-Organic Hybrid <span class="hlt">p-n</span> Junction <span class="hlt">Diode</span> for High Performance Self-Powered Photodetector.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bera, Ashok; Das Mahapatra, Ayon; Mondal, Sulakshana; Basak, Durga</p> <p>2016-12-21</p> <p>Organic-inorganic hybrid <span class="hlt">diodes</span> are very promising for solution processing, low cost, high performance optoelectronic devices. Here, we report a high quality <span class="hlt">p-n</span> heterojunction <span class="hlt">diode</span> composed of <span class="hlt">n</span>-type inorganic Sb 2 S 3 and <span class="hlt">p</span>-type organic 2,2',7,7'-tetrakis-(<span class="hlt">N,N-di-p</span>-methoxyphenylamine)-9,9'-spirobifluorene (spiro-OMeTAD) with a rectification ratio of ∼10 2 at an applied bias of 1 V. On illumination with visible light (470 nm, 1.82 mW/cm 2 ), the current value in our device becomes 8 × 10 2 times that of its dark value even at a zero bias condition. The estimated responsivity value at zero bias is 0.087 A/W which is so far the highest reported for any organic-inorganic hybrid photodiode, to the best of our knowledge. It also exhibits a fast photoresponse time of <25 ms (instrumental limit). More importantly, our device can also detect visible light with power density as low as 8 μW/cm 2 with a photocurrent density of 1.2 μA/cm 2 and a photocurrent to dark current ratio of more than 8. We also demonstrate that the values of responsivity, short circuit current, and open circuit voltage of the photodetector can be improved significantly using a thin layer of TiO 2 hole-blocking layer. These findings suggest Sb 2 S 3 /spiro-OMeTAD heterojuncton as a promising candidate for efficient self-powered low visible light photodetector.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21517080','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21517080"><span><span class="hlt">p</span>-Type modulation doped InGa<span class="hlt">N/GaN</span> dot-in-a-wire white-light-emitting <span class="hlt">diodes</span> monolithically grown on Si(111).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nguyen, H P T; Zhang, S; Cui, K; Han, X; Fathololoumi, S; Couillard, M; Botton, G A; Mi, Z</p> <p>2011-05-11</p> <p>Full-color, catalyst-free InGa<span class="hlt">N/GaN</span> dot-in-a-wire light-emitting <span class="hlt">diodes</span> (LEDs) were monolithically grown on Si(111) by molecular beam epitaxy, with the emission characteristics controlled by the dot properties in a single epitaxial growth step. With the use of <span class="hlt">p</span>-type modulation doping in the dot-in-a-wire heterostructures, we have demonstrated the most efficient phosphor-free white LEDs ever reported, which exhibit an internal quantum efficiency of ∼56.8%, nearly unaltered CIE chromaticity coordinates with increasing injection current, and virtually zero efficiency droop at current densities up to ∼640 A/cm(2). The remarkable performance is attributed to the superior three-dimensional carrier confinement provided by the electronically coupled dot-in-a-wire heterostructures, the nearly defect- and strain-free Ga<span class="hlt">N</span> nanowires, and the significantly enhanced hole transport due to the <span class="hlt">p</span>-type modulation doping.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050232858&hterms=metal+detector&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dmetal%2Bdetector','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050232858&hterms=metal+detector&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dmetal%2Bdetector"><span>Characterization of Dual-Band Infrared <span class="hlt">Detectors</span> for Application to Remote Sensing</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Abedin, M. Nurul; Refaat, Tamer F.; Xiao, Yegao; Bhat, Ishwara</p> <p>2005-01-01</p> <p>NASA Langley Research Center (LaRC), in partnership with the Rensselaer Polytechnic Institute (RPI), developed photovoltaic infrared (IR) <span class="hlt">detectors</span> suitable at two different wavelengths using Sb-based material systems. Using lattice-matched InGaAsSb grown on GaSb substrates, dual wavelength <span class="hlt">detectors</span> operating at 1.7 and 2.5 micron wavelengths can be realized. <span class="hlt">P-N</span> junction <span class="hlt">diodes</span> are fabricated on both GaSb and InGaAsSb materials. The photodiode on GaSb detects wavelengths at 1.7 micron and the InGaAsSb <span class="hlt">detector</span> detects wavelengths at 2.2 micron or longer depending on the composition. The films for these devices are grown by metal-organic vapor phase epitaxy (MOVPE). The cross section of the independently accessed back-to-back photodiode dual band <span class="hlt">detector</span> consists of a <span class="hlt">p</span>-type substrate on which <span class="hlt">n-on-p</span> GaInAsSb junction is grown, followed by a <span class="hlt">p-on-n</span> GaSb junction. There are three ohmic contacts in this structure, one to the <span class="hlt">p</span>-GaSb top layer, one to the <span class="hlt">n-GaSb/n</span>-GaInAsSb layer and one to the <span class="hlt">p</span>-type GaSb substrate. The common terminal is the contact to the <span class="hlt">n-GaSb/n</span>-GaInAsSb layer. The contact to the <span class="hlt">n-GaSb/p</span>-GaInAsSb region of the photodiode in the dual band is electrically connected and is accessed at the edge of the photodiode. NASA LaRC acquired the fabricated dual band <span class="hlt">detector</span> from RPI and characterized the <span class="hlt">detector</span> at its <span class="hlt">Detector</span> Characterization Laboratory. Characterization results, such as responsivity, noise, quantum efficiency, and detectivity will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22395514-low-temperature-type-doping-al-gan-layers-using-ammonia-molecular-beam-epitaxy-ingan-laser-diodes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22395514-low-temperature-type-doping-al-gan-layers-using-ammonia-molecular-beam-epitaxy-ingan-laser-diodes"><span>Low temperature <span class="hlt">p</span>-type doping of (Al)Ga<span class="hlt">N</span> layers using ammonia molecular beam epitaxy for InGa<span class="hlt">N</span> laser <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Malinverni, M., E-mail: marco.malinverni@epfl.ch; Lamy, J.-M.; Martin, D.</p> <p>2014-12-15</p> <p>We demonstrate state-of-the-art <span class="hlt">p</span>-type (Al)Ga<span class="hlt">N</span> layers deposited at low temperature (740 °C) by ammonia molecular beam epitaxy (NH{sub 3}-MBE) to be used as top cladding of laser <span class="hlt">diodes</span> (LDs) with the aim of further reducing the thermal budget on the InGa<span class="hlt">N</span> quantum well active region. Typical <span class="hlt">p</span>-type Ga<span class="hlt">N</span> resistivities and contact resistances are 0.4 Ω cm and 5 × 10{sup −4} Ω cm{sup 2}, respectively. As a test bed, we fabricated a hybrid laser structure emitting at 400 nm combining <span class="hlt">n</span>-type AlGa<span class="hlt">N</span> cladding and InGa<span class="hlt">N</span> active region grown by metal-organic vapor phase epitaxy, with the <span class="hlt">p</span>-doped waveguide and cladding layers grown by NH{sub 3}-MBE. Single-mode ridge-waveguide LD exhibitsmore » a threshold voltage as low as 4.3 V for an 800 × 2 μm{sup 2} ridge dimension and a threshold current density of ∼5 kA cm{sup −2} in continuous wave operation. The series resistance of the device is 6 Ω and the resistivity is 1.5 Ω cm, confirming thereby the excellent electrical properties of <span class="hlt">p</span>-type Al{sub 0.06}Ga{sub 0.94}<span class="hlt">N</span>:Mg despite the low growth temperature.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ApSS..256.4972K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ApSS..256.4972K"><span>Heterojunction light emitting <span class="hlt">diodes</span> fabricated with different <span class="hlt">n</span>-layer oxide structures on <span class="hlt">p-GaN</span> layers by magnetron sputtering</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kong, Bo Hyun; Han, Won Suk; Kim, Young Yi; Cho, Hyung Koun; Kim, Jae Hyun</p> <p>2010-06-01</p> <p>We grew heterojunction light emitting <span class="hlt">diode</span> (LED) structures with various <span class="hlt">n</span>-type semiconducting layers by magnetron sputtering on <span class="hlt">p</span>-type Ga<span class="hlt">N</span> at high temperature. Because the undoped ZnO used as an active layer was grown under oxygen rich atmosphere, all LED devices showed the EL characteristics corresponding to orange-red wavelength due to high density of oxygen interstitial, which was coincident with the deep level photoluminescence emission of undoped ZnO. The use of the Ga doped layers as a top layer provided the sufficient electron carriers to active region and resulted in the intense EL emission. The LED sample with small quantity of Mg incorporated in MgZnO as an <span class="hlt">n</span>-type top layer showed more intense emission than the LED with ZnO, in spite of the deteriorated electrical and structural properties of the MgZnO film. This might be due to the improvement of output extraction efficiency induced by rough surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22591575-site-controlled-ingan-gan-single-photon-emitting-diode','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22591575-site-controlled-ingan-gan-single-photon-emitting-diode"><span>Site-controlled InGa<span class="hlt">N/GaN</span> single-photon-emitting <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Zhang, Lei; Deng, Hui, E-mail: dengh@umich.edu; Teng, Chu-Hsiang</p> <p>2016-04-11</p> <p>We report single-photon emission from electrically driven site-controlled InGa<span class="hlt">N/GaN</span> quantum dots. The device is fabricated from a planar light-emitting <span class="hlt">diode</span> structure containing a single InGa<span class="hlt">N</span> quantum well, using a top-down approach. The location, dimension, and height of each single-photon-emitting <span class="hlt">diode</span> are controlled lithographically, providing great flexibility for chip-scale integration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ApPhL.105o3503Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ApPhL.105o3503Z"><span>A hole accelerator for InGa<span class="hlt">N/GaN</span> light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Zi-Hui; Liu, Wei; Tan, Swee Tiam; Ji, Yun; Wang, Liancheng; Zhu, Binbin; Zhang, Yiping; Lu, Shunpeng; Zhang, Xueliang; Hasanov, Namig; Sun, Xiao Wei; Demir, Hilmi Volkan</p> <p>2014-10-01</p> <p>The quantum efficiency of InGa<span class="hlt">N/GaN</span> light-emitting <span class="hlt">diodes</span> (LEDs) has been significantly limited by the insufficient hole injection, and this is caused by the inefficient <span class="hlt">p</span>-type doping and the low hole mobility. The low hole mobility makes the holes less energetic, which hinders the hole injection into the multiple quantum wells (MQWs) especially when a <span class="hlt">p</span>-type AlGa<span class="hlt">N</span> electron blocking layer (EBL) is adopted. In this work, we report a hole accelerator to accelerate the holes so that the holes can obtain adequate kinetic energy, travel across the <span class="hlt">p</span>-type EBL, and then enter the MQWs more efficiently and smoothly. In addition to the numerical study, the effectiveness of the hole accelerator is experimentally shown through achieving improved optical output power and reduced efficiency droop for the proposed InGa<span class="hlt">N/GaN</span> LED.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhD...49w5101H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhD...49w5101H"><span>Enhanced wall-plug efficiency in AlGa<span class="hlt">N</span>-based deep-ultraviolet light-emitting <span class="hlt">diodes</span> with uniform current spreading <span class="hlt">p</span>-electrode structures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hao, Guo-Dong; Taniguchi, Manabu; Tamari, Naoki; Inoue, Shin-ichiro</p> <p>2016-06-01</p> <p>The current crowding is an especially severe issue in AlGa<span class="hlt">N</span>-based deep-ultraviolet (DUV) light-emitting <span class="hlt">diodes</span> (LEDs) because of the low conductivity of the <span class="hlt">n-AlGaN</span> cladding layer that has a high Al fraction. We theoretically investigated the improvement in internal quantum efficiency and total resistances in DUV-LEDs with an emission wavelength of 265 nm by a well-designed <span class="hlt">p</span>-electrode geometry to produce uniform current spreading. As a result, the wall-plug efficiency was enhanced by a factor of 60% at an injection current of 350 mA in the designed uniform-current-spreading <span class="hlt">p</span>-electrode LED when compared with an LED with a conventional cross-bar <span class="hlt">p</span>-electrode pattern.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22412627-hole-modulator-ingan-gan-light-emitting-diodes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22412627-hole-modulator-ingan-gan-light-emitting-diodes"><span>A hole modulator for InGa<span class="hlt">N/GaN</span> light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Zhang, Zi-Hui; Kyaw, Zabu; Liu, Wei</p> <p>2015-02-09</p> <p>The low <span class="hlt">p</span>-type doping efficiency of the <span class="hlt">p-GaN</span> layer has severely limited the performance of InGa<span class="hlt">N/GaN</span> light-emitting <span class="hlt">diodes</span> (LEDs) due to the ineffective hole injection into the InGa<span class="hlt">N/GaN</span> multiple quantum well (MQW) active region. The essence of improving the hole injection efficiency is to increase the hole concentration in the <span class="hlt">p-GaN</span> layer. Therefore, in this work, we have proposed a hole modulator and studied it both theoretically and experimentally. In the hole modulator, the holes in a remote <span class="hlt">p</span>-type doped layer are depleted by the built-in electric field and stored in the <span class="hlt">p-GaN</span> layer. By this means, the overall holemore » concentration in the <span class="hlt">p-GaN</span> layer can be enhanced. Furthermore, the hole modulator is adopted in the InGa<span class="hlt">N/GaN</span> LEDs, which reduces the effective valance band barrier height for the <span class="hlt">p</span>-type electron blocking layer from ∼332 meV to ∼294 meV at 80 A/cm{sup 2} and demonstrates an improved optical performance, thanks to the increased hole concentration in the <span class="hlt">p-GaN</span> layer and thus the improved hole injection into the MQWs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JEMat.tmp..122Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JEMat.tmp..122Y"><span>Temperature-Dependent Electrical Characteristics of Au/Si3<span class="hlt">N</span>4/4H <span class="hlt">n</span>-SiC MIS <span class="hlt">Diode</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yigiterol, F.; Güllü, H. H.; Bayraklı, Ö.; Yıldız, D. E.</p> <p>2018-03-01</p> <p>Electrical characteristics of the Au/Si3<span class="hlt">N</span>4/4H <span class="hlt">n</span>-SiC metal-insulator-semiconductor (MIS) <span class="hlt">diode</span> were investigated under the temperature, T , interval of 160-400 K using current-voltage (<span class="hlt">I</span>-V), capacitance-voltage ( C {-} V ) and conductance-voltage ( G/ω {-} V ) measurements. Firstly, the Schottky <span class="hlt">diode</span> parameters as zero-bias barrier height ( Φ_{B0} ) and ideality factor ( <span class="hlt">n</span> ) were calculated according to the thermionic emission (TE) from forward bias <span class="hlt">I</span>-V analysis in the whole working T . Experimental results showed that the values of Φ_{B0} were in increasing behavior with increasing T while <span class="hlt">n</span> values decreased with inverse proportionality in <span class="hlt">n</span> versus Φ_{{{{B}}0}} plot. Therefore, the non-ideal <span class="hlt">I</span>-V behavior with inhomogeneous barrier height (BH) formation has been discussed under the assumption of Gaussian distribution (GD). From the GD of BHs, the mean BH was found to be about 1.40 eV with 0.1697 standard deviation and the modified Richardson constant A^{*} of this <span class="hlt">diode</span> was obtained as 141.65 A/cm2 K2 in good agreement with the literature (the theoretical value of A^{*} is 137.21 A/cm2 K2). The relationship between Φ_{B0} and <span class="hlt">n</span> showed an abnormal <span class="hlt">I</span>-V behavior depending on T , and it was modeled by TE theory with GD of BH due to the effect in inhomogeneous BH at the interface. Secondly, according to Cheung's model, series resistance, R_{{S}} values were calculated in the T range of 160-400 K and these values were found to decrease with increasing T . Finally, the density of interface states, D_{{it}} was calculated and the T dependence of energy distribution of D_{{it}} profiles determined the forward <span class="hlt">I</span> {-} V measurements by taking into account the bias dependence of the effective BH, Φ_{{e}} and <span class="hlt">n</span> . D_{{it}} were also calculated according to the Hill-Coleman method from C {-} V and G/ω {-} V analysis. Furthermore, the variation of D_{{it}} as a function of frequency, f and T were determined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AIPC.1399..171R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AIPC.1399..171R"><span>Temperature Dependence Of Current-Voltage Characteristics Of Au/<span class="hlt">p-GaAsN</span> Schottky Barrier <span class="hlt">Diodes</span>, With Small <span class="hlt">N</span> Content</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rangel-Kuoppa, Victor-Tapio; Reentilä, Outi; Sopanen, Markku; Lipsanen, Harri</p> <p>2011-12-01</p> <p>The temperature dependent current-voltage (IVT) measurements on Au Schottky barrier <span class="hlt">diodes</span> made on intrinsically <span class="hlt">p</span>-type GaAs1-xNx were carried out. Three samples with small <span class="hlt">N</span> content (x = 0.5%, 0.7% and 1%) were studied. The temperature range was 10-320 K. All contacts were found to be of Schottky type. The ideality factor and the apparent barrier height calculated by using thermionic emission (TE) theory show a strong temperature dependence. The current voltage (IV) curves are fitted based on the TE theory, yielding a zero-bias carrier height (ΦB0) and a ideality factor (<span class="hlt">n</span>) that decrease and increase with decreasing temperature, respectively. The linear fitting of ΦB0 vs <span class="hlt">n</span> and its subsequent evaluation for <span class="hlt">n</span> = 1 give a zero-bias ΦB0 in the order of 0.35-0.4 eV. From the reverse-bias IV study, it is found that the experimental carrier density (NA) values increase with increasing temperature and are in agreement with the intrinsic carrier concentration for GaAs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApPhA.124...81O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApPhA.124...81O"><span>Comparative study of <span class="hlt">I</span>- V methods to extract Au/FePc/<span class="hlt">p</span>-Si Schottky barrier <span class="hlt">diode</span> parameters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Oruç, Çiğdem; Altındal, Ahmet</p> <p>2018-01-01</p> <p>So far, various methods have been proposed to extract the Schottky <span class="hlt">diode</span> parameters from measured current-voltage characteristics. In this work, Schottky barrier <span class="hlt">diode</span> with structure of Au/2(3),9(10),16(17),23(24)-tetra(4-(4-methoxyphenyl)-8-methylcoumarin-7 oxy) phthalocyaninatoiron(II) (FePc)/<span class="hlt">p</span>-Si was fabricated and current-voltage measurements were carried out on it. In addition, current-voltage measurements were also performed on Au/<span class="hlt">p</span>-Si structure, without FePc, to clarify the influence of the presence of an interface layer on the device performance. The measured current-voltage characteristics indicate that the interface properties of a Schottky barrier <span class="hlt">diode</span> can be controlled by the presence of an organic interface layer. It is found that the room temperature barrier height of Au/FePc/<span class="hlt">p</span>-Si structure is larger than that of the Au/<span class="hlt">p</span>-Si structure. The obtained forward bias current-voltage characteristics of the Au/FePc/<span class="hlt">p</span>-Si device was analysed by five different analytical methods. It is found that the extracted values of SBD parameters strongly depends on the method used.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhCS.707a2015A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhCS.707a2015A"><span>Effects of Post Annealing on <span class="hlt">I</span>-V-T Characteristics of (Ni/Au)/Al0.09Ga0.91<span class="hlt">N</span> Schottky Barrier <span class="hlt">Diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Akkaya, Abdullah; Ayyıldız, Enise</p> <p>2016-04-01</p> <p>Post annealing is a simple, effective and suitable method for improving the <span class="hlt">diode</span> parameters, especially when the used chemically stable substrates like Si, III-<span class="hlt">N</span> and ternary alloys. In our work, we were applied this method to (Ni/Au)/Al0.09Ga0.91<span class="hlt">N</span> Schottky Barrier <span class="hlt">Diodes</span> (SBDs) and investigated by temperature-dependent current-voltage (<span class="hlt">I</span>-V-T) characteristics at optimum conditions. Optimum annealing temperature was 600°C, which it’s determined with respect to have a highest barrier height value. The temperature-dependent electrical characteristics of the annealed at 600°C (Ni/Au)/Al0.09Ga0.91<span class="hlt">N</span> SBDs were investigated in the wide temperature range of 95-315K. The <span class="hlt">diode</span> parameters such as ideality factor (<span class="hlt">n</span>) and Schottky barrier height (Vb0) were obtained to be strongly temperature dependent. The observed variation in Vb0 and <span class="hlt">n</span> can be attributed to the spatial barrier inhomogeneities in Schottky barrier height by assuming a triple Gaussian distribution (TGD) of barrier heights (BHs) at 95-145K, 145-230K and 230-315K. The modified Richardson plots and T0 analysis was performed to provide an experimental Richardson constants and bias coefficients of the mean barrier height. Furthermore, the chemical composition of the contacts was examined by the XPS depth profile analysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993JCrGr.127...14M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993JCrGr.127...14M"><span>In 0.35Ga 0.65<span class="hlt">P</span> light-emitting <span class="hlt">diodes</span> grown by gas-source MBE</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Masselink, W. Ted; Zachau, Martin</p> <p>1993-02-01</p> <p>This paper describes the growth and optical characteristics of In yGa 1- y<span class="hlt">P</span> with 0.3< y<0.5, and the LED operation of <span class="hlt">p-i-n</span> structures in the same materials system. The InGa<span class="hlt">P</span> is grown using gas-source molecular beam epitaxy (GSMBE). The non-lattice-matched In yGa 1- y<span class="hlt">P</span> grown on GaAs using GSMBE has a specularly smooth surface morphology through the use of unique strained-layer superlattice (SLS) buffer. We have measured the luminescence, luminescence excitation, and Raman spectra of these undoped films and observe strong excitonic luminescence over the entire composition range investigated. The band gap derived from the luminescence excitation spectra corresponds to that of a fully relaxed InGa<span class="hlt">P</span> film with no residual strain, which is confirmed by the Raman measurements. Light-emitting <span class="hlt">diodes</span> with peak (300 K) emission centered at less than 590 nm have been fabricated from <span class="hlt">p-i-n</span> junctions in In 0.35Ga 0.65<span class="hlt">P</span>. This alloy is close to that with the largest direct band gap in the In yGa 1- y <span class="hlt">P</span> system and has lattice mismatch from the GaAs substrate of 1%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22063921-metal-assisted-electroless-fabrication-nanoporous-gan-increasing-light-extraction-efficiency-light-emitting-diodes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22063921-metal-assisted-electroless-fabrication-nanoporous-gan-increasing-light-extraction-efficiency-light-emitting-diodes"><span>Metal-assisted electroless fabrication of nanoporous <span class="hlt">p-GaN</span> for increasing the light extraction efficiency of light emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Wang Ruijun; Liu Duo; Zuo Zhiyuan</p> <p>2012-03-15</p> <p>We report metal-assisted electroless fabrication of nanoporous <span class="hlt">p-GaN</span> to improve the light extraction efficiency of Ga<span class="hlt">N</span>-based light emitting <span class="hlt">diodes</span> (LEDs). Although it has long been believed that <span class="hlt">p-GaN</span> cannot be etched at room temperature, in this study we find that Ag nanocrystals (NCs) on the <span class="hlt">p-GaN</span> surface enable effective etching of <span class="hlt">p-GaN</span> in a mixture of HF and K{sub 2}S{sub 2}O{sub 8} under ultraviolet (UV) irradiation. It is further shown that the roughened Ga<span class="hlt">N</span>/air interface enables strong scattering of photons emitted from the multiple quantum wells (MQWs). The light output power measurements indicate that the nanoporous LEDs obtained after 10more » min etching show a 32.7% enhancement in light-output relative to the conventional LEDs at an injection current of 20 mA without significant increase of the operating voltage. In contrast, the samples etched for 20 min show performance degradation when compared with those etched for 10 min, this is attributed to the current crowding effect and increased surface recombination rate.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27169828','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27169828"><span>Determination and confirmation of isopropyl <span class="hlt">p</span>-toluenesulfonate in cosmetics by HPLC-<span class="hlt">diode</span> array <span class="hlt">detector</span> method and GC-MS.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tay, B Y P; Yung, S C; Teoh, T Y</p> <p>2016-12-01</p> <p>Isopropyl <span class="hlt">p</span>-toluenesulfonate (IPTS) is a potentially genotoxic by-product formed during the esterification of palm oil-based palmitic and palm kernel oil-based myristic acid with isopropanol to produce isopropyl palmitate or isopropyl myristate. There are no methods described for the analysis of IPTS in cosmetic products. In this work, we have established a simple, precise and accurate method to determine the presence and level of IPTS in various finished cosmetic products which contain palm-based esters in their formulations. An Agilent 1200 series high-performance liquid chromatography (HPLC) unit using a <span class="hlt">diode</span>-array <span class="hlt">detector</span> (DAD) has been employed and optimized to detect IPTS in cosmetic products. For the separation, a reverse-phase Hypersil Gold C8 column (5 μm, 4.6 mm <span class="hlt">i</span>.d. 250 mm) 5 mM tetrabutylammonium phosphate buffer 50 : 50, (v/v) solution in acetonitrile as mobile phase, in isocratic mode and a flow rate of 0.8 mL min -1 were used. A second method using a gas chromatography/mass selective <span class="hlt">detector</span> GC-MSD was also developed to confirm the IPTS identity in the cosmetic products. Recoveries of IPTS from cosmetic matrices such as a lotion, cleansing milk and a cream ranged from 94.0% to 101.1% with <5% relative standard deviation (%RSD) showing good accuracy and repeatability of the method. The six-point calibration curves (determined over the range 0.5-50 μg mL -1 ) have a correlation coefficient of 0.9999 (based on HPLC peak area) and 0.9998 (based on HPLC peak height). The intra- and interday precisions (measured by the %RSD) of the method were <2% and <5%, respectively, indicating that the developed method is reliable, precise and reproducible. The detection and quantification limit of the method were found to be 0.5 μg mL -1 and 1.6 μg mL -1 , respectively. Analyses of 83 commercial cosmetics showed no presence of IPTS. The validation data indicated that this method was suitable for the quantitative analysis of IPTS in commercial</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_14 --> <div id="page_15" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="281"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ApPhL..97a3502C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ApPhL..97a3502C"><span>Inverted Al0.25Ga0.75<span class="hlt">N/GaN</span> ultraviolet <span class="hlt">p-i-n</span> photodiodes formed on <span class="hlt">p-GaN</span> template layer grown by metalorganic vapor phase epitaxy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chang, Kuo-Hua; Sheu, Jinn-Kong; Lee, Ming-Lun; Tu, Shang-Ju; Yang, Chih-Ciao; Kuo, Huan-Shao; Yang, J. H.; Lai, Wei-Chih</p> <p>2010-07-01</p> <p>Inverted Al0.25Ga0.75<span class="hlt">N/GaN</span> ultraviolet (UV) <span class="hlt">p-i-n</span> photodiodes (PDs) were grown by selective-area regrowth on <span class="hlt">p-GaN</span> template. The inverted devices with low-resistivity <span class="hlt">n</span>-type AlGa<span class="hlt">N</span> top-contact layers exhibited a typical zero-bias peak responsivity of 66.7 mA/W at 310 nm corresponding to the external quantum efficiency of 26.6%. The typical UV-to-visible (310/400 nm) spectral rejection ratio at zero-bias was over three orders of magnitude. The differential resistance and detectivity were obtained at approximately 6.2×1012 Ω and 3.4×1013 cm Hz1/2 W-1, respectively. Compared with conventional AlGa<span class="hlt">N/GaN</span>-based UV <span class="hlt">p-i-n</span> PDs, the proposed device structure can potentially achieve solar-blind AlGa<span class="hlt">N/GaN</span>-based <span class="hlt">p-i-n</span> PDs with low-aluminum content or aluminum-free <span class="hlt">p</span>-contact layer and reduce excessive tensile strain due to the lattice mismatch between AlGa<span class="hlt">N</span> and Ga<span class="hlt">N</span> layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22350840-ingan-gan-tunnel-junctions-hole-injection-gan-light-emitting-diodes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22350840-ingan-gan-tunnel-junctions-hole-injection-gan-light-emitting-diodes"><span>InGa<span class="hlt">N/GaN</span> tunnel junctions for hole injection in Ga<span class="hlt">N</span> light emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Krishnamoorthy, Sriram, E-mail: krishnamoorthy.13@osu.edu, E-mail: rajan@ece.osu.edu; Akyol, Fatih; Rajan, Siddharth, E-mail: krishnamoorthy.13@osu.edu, E-mail: rajan@ece.osu.edu</p> <p></p> <p>InGa<span class="hlt">N/GaN</span> tunnel junction contacts were grown using plasma assisted molecular beam epitaxy (MBE) on top of a metal-organic chemical vapor deposition (MOCVD)-grown InGa<span class="hlt">N/GaN</span> blue (450 nm) light emitting <span class="hlt">diode</span>. A voltage drop of 5.3 V at 100 mA, forward resistance of 2 × 10{sup −2} Ω cm{sup 2}, and a higher light output power compared to the reference light emitting <span class="hlt">diodes</span> (LED) with semi-transparent <span class="hlt">p</span>-contacts were measured in the tunnel junction LED (TJLED). A forward resistance of 5 × 10{sup −4} Ω cm{sup 2} was measured in a Ga<span class="hlt">N</span> PN junction with the identical tunnel junction contact as the TJLED, grown completely by MBE. Themore » depletion region due to the impurities at the regrowth interface between the MBE tunnel junction and the MOCVD-grown LED was hence found to limit the forward resistance measured in the TJLED.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23849302','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23849302"><span>The fabrication of white light-emitting <span class="hlt">diodes</span> using the <span class="hlt">n-ZnO/NiO/p-GaN</span> heterojunction with enhanced luminescence.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Abbasi, Mazhar Ali; Ibupoto, Zafar Hussain; Hussain, Mushtaque; Nur, Omer; Willander, Magnus</p> <p>2013-07-13</p> <p>Cheap and efficient white light-emitting <span class="hlt">diodes</span> (LEDs) are of great interest due to the energy crisis all over the world. Herein, we have developed heterojunction LEDs based on the well-aligned ZnO nanorods and nanotubes on the <span class="hlt">p</span>-type Ga<span class="hlt">N</span> with the insertion of the NiO buffer layer that showed enhancement in the light emission. Scanning electron microscopy have well demonstrated the arrays of the ZnO nanorods and the proper etching into the nanotubes. X-ray diffraction study describes the wurtzite crystal structure array of ZnO nanorods with the involvement of Ga<span class="hlt">N</span> at the (002) peak. The cathodoluminescence spectra represent strong and broad visible emission peaks compared to the UV emission and a weak peak at 425 nm which is originated from Ga<span class="hlt">N</span>. Electroluminescence study has shown highly improved luminescence response for the LEDs fabricated with NiO buffer layer compared to that without NiO layer. Introducing a sandwich-thin layer of NiO between the <span class="hlt">n</span>-type ZnO and the <span class="hlt">p</span>-type Ga<span class="hlt">N</span> will possibly block the injection of electrons from the ZnO to the Ga<span class="hlt">N</span>. Moreover, the presence of NiO buffer layer might create the confinement effect.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JSemi..38f4001R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JSemi..38f4001R"><span>Schottky barrier parameters and structural properties of rapidly annealed Zr Schottky electrode on <span class="hlt">p</span>-type Ga<span class="hlt">N</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rajagopal Reddy, V.; Asha, B.; Choi, Chel-Jong</p> <p>2017-06-01</p> <p>The Schottky barrier junction parameters and structural properties of Zr/<span class="hlt">p-GaN</span> Schottky <span class="hlt">diode</span> are explored at various annealing temperatures. Experimental analysis showed that the barrier height (BH) of the Zr/<span class="hlt">p-GaN</span> Schottky <span class="hlt">diode</span> increases with annealing at 400 °C (0.92 eV (<span class="hlt">I</span>-V)/1.09 eV (C-V)) compared to the as-deposited one (0.83 eV (<span class="hlt">I</span>-V)/0.93 eV (C-V)). However, the BH decreases after annealing at 500 °C. Also, at different annealing temperatures, the series resistance and BH are assessed by Cheung's functions and their values compared. Further, the interface state density (<span class="hlt">N</span> SS) of the <span class="hlt">diode</span> decreases after annealing at 400 °C and then somewhat rises upon annealing at 500 °C. Analysis reveals that the maximum BH is obtained at 400 °C, and thus the optimum annealing temperature is 400 °C for the <span class="hlt">diode</span>. The XPS and XRD analysis revealed that the increase in BH may be attributed to the creation of Zr-<span class="hlt">N</span> phases with increasing annealing up to 400 °C. The BH reduces for the <span class="hlt">diode</span> annealed at 500 °C, which may be due to the formation of Ga-Zr phases at the junction. The AFM measurements reveal that the overall surface roughness of the Zr film is quite smooth during rapid annealing process. Project supported by the R&D Program for Industrial Core Technology (No. 10045216) and the Transfer Machine Specialized Lighting Core Technology Development Professional Manpower Training Project (No. <span class="hlt">N</span>0001363) Funded by the Ministry of Trade, Industry and Energy (MOTIE), Republic of Korea.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22413026-comprehensive-study-electronic-optical-behavior-highly-degenerate-type-mg-doped-gan-algan','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22413026-comprehensive-study-electronic-optical-behavior-highly-degenerate-type-mg-doped-gan-algan"><span>Comprehensive study of the electronic and optical behavior of highly degenerate <span class="hlt">p</span>-type Mg-doped Ga<span class="hlt">N</span> and AlGa<span class="hlt">N</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Gunning, Brendan P.; Fabien, Chloe A. M.; Merola, Joseph J.</p> <p>2015-01-28</p> <p>The bulk and 2-dimensional (2D) electrical transport properties of heavily Mg-doped <span class="hlt">p</span>-type Ga<span class="hlt">N</span> films grown on Al<span class="hlt">N</span> buffer layers by Metal Modulated Epitaxy are explored. Distinctions are made between three primary <span class="hlt">p</span>-type conduction mechanisms: traditional valence band conduction, impurity band conduction, and 2D conduction within a 2D hole gas at a hetero-interface. The bulk and 2D contributions to the overall carrier transport are identified and the relative contributions are found to vary strongly with growth conditions. Films grown with III/V ratio less than 1.5 exhibit high hole concentrations exceeding 2 × 10{sup 19} cm{sup −3} with effective acceptor activation energies of 51 meV.more » Films with III/V ratios greater than 1.5 exhibit lower overall hole concentrations and significant contributions from 2D transport at the hetero-interface. Films grown with III/V ratio of 1.2 and Mg concentrations exceeding 2 × 10{sup 20} cm{sup −3} show no detectable inversion domains or Mg precipitation. Highly Mg-doped <span class="hlt">p-GaN</span> and <span class="hlt">p-AlGaN</span> with Al fractions up to 27% similarly exhibit hole concentrations exceeding 2 × 10{sup 19} cm{sup −3}. The <span class="hlt">p-GaN</span> and <span class="hlt">p</span>-Al{sub 0.11}Ga{sub 0.89}<span class="hlt">N</span> films show broad ultraviolet (UV) photoluminescence peaks, which intercept the valence band, supporting the presence of a Mg acceptor band. Finally, a multi-quantum-well light-emitting <span class="hlt">diode</span> (LED) and <span class="hlt">p-i-n</span> <span class="hlt">diode</span> are grown, both of which demonstrate rectifying behavior with turn-on voltages of 3–3.5 V and series resistances of 6–10 Ω without the need for any post-metallization annealing. The LED exhibits violet-blue luminescence at 425 nm, while the <span class="hlt">p-i-n</span> <span class="hlt">diode</span> shows UV luminescence at 381 nm, and both devices still show substantial light emission even when submerged in liquid nitrogen at 77 K.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJWC.16201037H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJWC.16201037H"><span>Doping concentration effect on performance of single QW double-heterostructure InGa<span class="hlt">N/AlGaN</span> light emitting <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Halim, N. Syafira Abdul; Wahid, M. Halim A.; Hambali, N. Azura M. Ahmad; Rashid, Shanise; Shahimin, Mukhzeer M.</p> <p>2017-11-01</p> <p>Light emitting <span class="hlt">diode</span> (LED) employed a numerous applications such as displaying information, communication, sensing, illumination and lighting. In this paper, InGa<span class="hlt">N/AlGaN</span> based on one quantum well (1QW) light emitting <span class="hlt">diode</span> (LED) is modeled and studied numerically by using COMSOL Multiphysics 5.1 version. We have selected In0.06Ga0.94<span class="hlt">N</span> as the active layer with thickness 50nm sandwiched between 0.15μm thick layers of <span class="hlt">p</span> and <span class="hlt">n</span>-type Al0.15Ga0.85<span class="hlt">N</span> of cladding layers. We investigated an effect of doping concentration on InGa<span class="hlt">N/AlGaN</span> double heterostructure of light-emitting <span class="hlt">diode</span> (LED). Thus, energy levels, carrier concentration, electron concentration and forward voltage (IV) are extracted from the simulation results. As the doping concentration is increasing, the performance of threshold voltage, Vth on one quantum well (1QW) is also increases from 2.8V to 3.1V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22283048-determination-charge-carrier-diffusion-length-photosensing-layer-hgcdte-photovoltaic-infrared-focal-plane-array-detectors','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22283048-determination-charge-carrier-diffusion-length-photosensing-layer-hgcdte-photovoltaic-infrared-focal-plane-array-detectors"><span>Determination of charge-carrier diffusion length in the photosensing layer of HgCdTe <span class="hlt">n-on-p</span> photovoltaic infrared focal plane array <span class="hlt">detectors</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Vishnyakov, A. V.; Stuchinsky, V. A., E-mail: stuchin@isp.nsc.ru; Brunev, D. V.</p> <p>2014-03-03</p> <p>In the present paper, we propose a method for evaluating the bulk diffusion length of minority charge carriers in the photosensing layer of photovoltaic focal plane array (FPA) photodetectors. The method is based on scanning a strip-shaped illumination spot with one of the <span class="hlt">detector</span> <span class="hlt">diodes</span> at a low level of photocurrents j{sub ph} being registered; such scanning provides data for subsequent analysis of measured spot-scan profiles within a simple diffusion model. The asymptotic behavior of the effective (at j{sub ph} ≠ 0) charge-carrier diffusion length l{sub d} {sub eff} as a function of j{sub ph} for j{sub ph} → 0 inferred frommore » our experimental data proved to be consistent with the behavior of l{sub d} {sub eff} vs j{sub ph} as predicted by the model, while the obtained values of the bulk diffusion length of minority carriers (electrons) in the <span class="hlt">p</span>-HgCdTe film of investigated HgCdTe <span class="hlt">n-on-p</span> FPA photodetectors were found to be in a good agreement with the previously reported carrier diffusion-length values for HgCdTe.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SuMi..113..472C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SuMi..113..472C"><span>On the AlxGa1-x<span class="hlt">N</span>/AlyGa1-y<span class="hlt">N</span>/AlxGa1-x<span class="hlt">N</span> (x>y) <span class="hlt">p</span>-electron blocking layer to improve the hole injection for AlGa<span class="hlt">N</span> based deep ultraviolet light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chu, Chunshuang; Tian, Kangkai; Fang, Mengqian; Zhang, Yonghui; Li, Luping; Bi, Wengang; Zhang, Zi-Hui</p> <p>2018-01-01</p> <p>This work proposes the [0001] oriented AlGa<span class="hlt">N</span>-based deep ultraviolet (DUV) light-emitting <span class="hlt">diode</span> (LED) possessing a specifically designed <span class="hlt">p</span>-electron blocking layer (<span class="hlt">p</span>-EBL) to achieve the high internal quantum efficiency. Both electrons and holes can be efficiently injected into the active region by adopting the Al0.60Ga0.40<span class="hlt">N</span>/Al0.50Ga0.50<span class="hlt">N</span>/Al0.60Ga0.40<span class="hlt">N</span> structured <span class="hlt">p</span>-EBL, in which a <span class="hlt">p</span>-Al0.50Ga0.50<span class="hlt">N</span> layer is embedded into the <span class="hlt">p</span>-EBL. Moreover, the impact of different thicknesses for the <span class="hlt">p</span>-Al0.50Ga0.50<span class="hlt">N</span> insertion layer on the hole and electron injections has also been investigated. Compared with the DUV LED with the bulk <span class="hlt">p</span>-Al0.60Ga0.40<span class="hlt">N</span> as the EBL, the proposed LED architectures improve the light output power if the thickness of the <span class="hlt">p</span>-Al0.50Ga0.50<span class="hlt">N</span> insertion layer is properly designed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002REDS..157..367S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002REDS..157..367S"><span>In situ current-voltage characterization of swift heavy ion irradiated Au/<span class="hlt">n</span>-GaAs Schottky <span class="hlt">diode</span> at low temperature</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Singh, R.; Arora, S. K.; Singh, J. P.; Kanjilal, D.</p> <p></p> <p>A Au/<span class="hlt">n</span>-GaAs(100) Schottky <span class="hlt">diode</span> was irradiated at 80 K by a 180 MeV Ag-107(14+) ion beam. In situ current-voltage (<span class="hlt">I</span>--V) characterization of the <span class="hlt">diode</span> was performed at various irradiation fluences ranging from 1x10(10) to 1x10(13) ions cm(-2) . The semiconductor was heavily doped (carrier concentration=1x10(18) cm(-3)), hence thermionic field emission was assumed to be the dominant current transport mechanism in the <span class="hlt">diode</span>. Systematic variations in various parameters of the Schottky <span class="hlt">diode</span> like characteristic energy E-0 , ideality factor <span class="hlt">n</span> , reverse saturation current <span class="hlt">I</span>-S , flatband barrier height Phi(bf) and reverse leakage current <span class="hlt">I</span>-R have been observed with respect to the irradiation fluence. The nuclear and electronic energy losses of the swift heavy ion affect the interface state density at the metal-semiconductor interface resulting in observed variations in Schottky <span class="hlt">diode</span> parameters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JEMat..44.4676S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JEMat..44.4676S"><span>Restricted-Access Al-Mediated Material Transport in Al Contacting of PureGaB Ge-on-Si <span class="hlt">p</span> + <span class="hlt">n</span> <span class="hlt">Diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sammak, Amir; Qi, Lin; Nanver, Lis K.</p> <p>2015-12-01</p> <p>The effectiveness of using nanometer-thin boron (PureB) layers as interdiffusion barrier to aluminum (Al) is studied for a contacting scheme specifically developed for fabricating germanium-on-silicon (Ge-on-Si) <span class="hlt">p</span> + <span class="hlt">n</span> photodiodes with an oxide-covered light entrance window. Contacting is achieved at the perimeter of the Ge-island anode directly to an Al interconnect metallization. The Ge is grown in oxide windows to the Si wafer and covered by a B and gallium (Ga) layer stack (PureGaB) composed of about a nanometer of Ga for forming the <span class="hlt">p</span> + Ge region and 10 nm of B as an interdiffusion barrier to the Al. To form contact windows, the side-wall oxide is etched away, exposing a small tip of the Ge perimeter to Al that from this point travels about 5 μm into the bulk Ge crystal. In this process, Ge and Si materials are displaced, forming Ge-filled V-grooves at the Si surface. The Al coalesces in grains. This process is studied here by high-resolution cross-sectional transmission electron microscopy and energy dispersive x-ray spectroscopy that confirm the purities of the Ge and Al grains. <span class="hlt">Diodes</span> are fabricated with different geometries and statistical current-voltage characterization reveals a spread that can be related to across-the-wafer variations in the contact processing. The <span class="hlt">I</span>- V behavior is characterized by low dark current, low contact resistance, and breakdown voltages that are suitable for operation in avalanching modes. The restricted access to the Ge of the Al inducing the Ge and Si material transport does not destroy the very good electrical characteristics typical of PureGaB Ge-on-Si <span class="hlt">diodes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26371903','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26371903"><span>Surface plasmon coupling for suppressing <span class="hlt">p-GaN</span> absorption and TM-polarized emission in a deep-UV light-emitting <span class="hlt">diode</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kuo, Yang; Su, Chia-Ying; Hsieh, Chieh; Chang, Wen-Yen; Huang, Chu-An; Kiang, Yean-Woei; Yang, C C</p> <p>2015-09-15</p> <p>The radiated power enhancement (suppression) of an in- (out-of-) plane-oriented radiating dipole at a desired emission wavelength in the deep-ultraviolet (UV) range when it is coupled with a surface plasmon (SP) resonance mode induced on a nearby Al nanoparticle (NP) is demonstrated. Also, it is found that the enhanced radiated power propagates mainly in the direction from the Al NP toward the dipole. Such SP coupling behaviors can be used for suppressing the transverse-magnetic (TM)-polarized emission, enhancing the transverse-electric-polarized emission, and reducing the UV absorption of the <span class="hlt">p-GaN</span> layer in an AlGa<span class="hlt">N</span>-based deep-UV light-emitting <span class="hlt">diode</span> by embedding a sphere-like Al NP in its <span class="hlt">p-AlGaN</span> layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JInst..12P9032P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JInst..12P9032P"><span>Simulation study of signal formation in position sensitive planar <span class="hlt">p-on-n</span> silicon <span class="hlt">detectors</span> after short range charge injection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peltola, T.; Eremin, V.; Verbitskaya, E.; Härkönen, J.</p> <p>2017-09-01</p> <p>Segmented silicon <span class="hlt">detectors</span> (micropixel and microstrip) are the main type of <span class="hlt">detectors</span> used in the inner trackers of Large Hadron Collider (LHC) experiments at CERN. Due to the high luminosity and eventual high fluence of energetic particles, <span class="hlt">detectors</span> with fast response to fit the short shaping time of 20-25 ns and sufficient radiation hardness are required. Charge collection measurements carried out at the Ioffe Institute have shown a reversal of the pulse polarity in the <span class="hlt">detector</span> response to short-range charge injection. Since the measured negative signal is about 30-60% of the peak positive signal, the effect strongly reduces the CCE even in non-irradiated <span class="hlt">detectors</span>. For further investigation of the phenomenon the measurements have been reproduced by TCAD simulations. As for the measurements, the simulation study was applied for the <span class="hlt">p-on-n</span> strip <span class="hlt">detectors</span> similar in geometry to those developed for the ATLAS experiment and for the Ioffe Institute designed <span class="hlt">p-on-n</span> strip <span class="hlt">detectors</span> with each strip having a window in the metallization covering the <span class="hlt">p</span>+ implant, allowing the generation of electron-hole pairs under the strip implant. Red laser scans across the strips and the interstrip gap with varying laser diameters and Si-SiO2 interface charge densities (Qf) were carried out. The results verify the experimentally observed negative response along the scan in the interstrip gap. When the laser spot is positioned on the strip <span class="hlt">p</span>+ implant the negative response vanishes and the collected charge at the active strip increases respectively. The simulation results offer a further insight and understanding of the influence of the oxide charge density in the signal formation. The main result of the study is that a threshold value of Qf, that enables negligible losses of collected charges, is defined. The observed effects and details of the <span class="hlt">detector</span> response for different charge injection positions are discussed in the context of Ramo's theorem.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9974E..0HP','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9974E..0HP"><span>Extended short wavelength infrared HgCdTe <span class="hlt">detectors</span> on silicon substrates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Park, J. H.; Hansel, D.; Mukhortova, A.; Chang, Y.; Kodama, R.; Zhao, J.; Velicu, S.; Aqariden, F.</p> <p>2016-09-01</p> <p>We report high-quality <span class="hlt">n</span>-type extended short wavelength infrared (eSWIR) HgCdTe (cutoff wavelength 2.59 μm at 77 K) layers grown on three-inch diameter CdTe/Si substrates by molecular beam epitaxy (MBE). This material is used to fabricate test <span class="hlt">diodes</span> and arrays with a planar device architecture using arsenic implantation to achieve <span class="hlt">p</span>-type doping. We use different variations of a test structure with a guarded design to compensate for the lateral leakage current of traditional test <span class="hlt">diodes</span>. These test <span class="hlt">diodes</span> with guarded arrays characterize the electrical performance of the active 640 × 512 format, 15 μm pitch <span class="hlt">detector</span> array.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26373094','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26373094"><span>Reverse Current Characteristics of In<span class="hlt">P</span> Gunn <span class="hlt">Diodes</span> for W-Band Waveguide Applications.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Hyun-Seok; Heo, Jun-Woo; Chol, Seok-Gyu; Ko, Dong-Sik; Rhee, Jin-Koo</p> <p>2015-07-01</p> <p>In<span class="hlt">P</span> is considered as the most promising material for millimeter-wave laser-<span class="hlt">diode</span> applications owing to its superior noise performance and wide operating frequency range of 75-110 GHz. In this study, we demonstrate the fabrication of In<span class="hlt">P</span> Gunn <span class="hlt">diodes</span> with a current-limiting structure using rapid thermal annealing to modulate the potential height formed between an <span class="hlt">n</span>-type In<span class="hlt">P</span> active layer and a cathode contact. We also explore the reverse current characteristics of the In<span class="hlt">P</span> Gunn <span class="hlt">diodes</span>. Experimental results indicate a maximum anode current and an oscillation frequency of 200 mA and 93.53 GHz, respectively. The current-voltage characteristics are modeled by considering the Schottky and ohmic contacts, work function variations, negative differential resistance (NDR), and tunneling effect. Although no direct indication of the NDR is observed, the simulation results match the measured data well. The modeling results show that the NDR effect is always present but is masked because of electron emission across the shallow Schottky barrier.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3211177','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3211177"><span>The origin of the red emission in <span class="hlt">n</span>-ZnO nanotubes/<span class="hlt">p-GaN</span> white light emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2011-01-01</p> <p>In this article, the electroluminescence (EL) spectra of zinc oxide (ZnO) nanotubes/<span class="hlt">p-GaN</span> light emitting <span class="hlt">diodes</span> (LEDs) annealed in different ambients (argon, air, oxygen, and nitrogen) have been investigated. The ZnO nanotubes by aqueous chemical growth (ACG) technique on <span class="hlt">p-GaN</span> substrates were obtained. The as-grown ZnO nanotubes were annealed in different ambients at 600°C for 30 min. The EL investigations showed that air, oxygen, and nitrogen annealing ambients have strongly affected the deep level emission bands in ZnO. It was concluded from the EL investigation that more than one deep level defect is involved in the red emission appearing between 620 and 750 nm and that the red emission in ZnO can be attributed to oxygen interstitials (Oi) appearing in the range from 620 nm (1.99 eV) to 690 nm (1.79 eV), and to oxygen vacancies (Vo) appearing in the range from 690 nm (1.79 eV) to 750 nm (1.65 eV). The annealing ambients, especially the nitrogen ambient, were also found to greatly influence the color-rendering properties and increase the CRI of the as - grown LEDs from 87 to 96. PMID:21711671</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21711671','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21711671"><span>The origin of the red emission in <span class="hlt">n</span>-ZnO nanotubes/<span class="hlt">p-GaN</span> white light emitting <span class="hlt">diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Alvi, N H; Ul Hasan, Kamran; Nur, Omer; Willander, Magnus</p> <p>2011-02-10</p> <p>In this article, the electroluminescence (EL) spectra of zinc oxide (ZnO) nanotubes/<span class="hlt">p-GaN</span> light emitting <span class="hlt">diodes</span> (LEDs) annealed in different ambients (argon, air, oxygen, and nitrogen) have been investigated. The ZnO nanotubes by aqueous chemical growth (ACG) technique on <span class="hlt">p-GaN</span> substrates were obtained. The as-grown ZnO nanotubes were annealed in different ambients at 600°C for 30 min. The EL investigations showed that air, oxygen, and nitrogen annealing ambients have strongly affected the deep level emission bands in ZnO. It was concluded from the EL investigation that more than one deep level defect is involved in the red emission appearing between 620 and 750 nm and that the red emission in ZnO can be attributed to oxygen interstitials (Oi) appearing in the range from 620 nm (1.99 eV) to 690 nm (1.79 eV), and to oxygen vacancies (Vo) appearing in the range from 690 nm (1.79 eV) to 750 nm (1.65 eV). The annealing ambients, especially the nitrogen ambient, were also found to greatly influence the color-rendering properties and increase the CRI of the as - grown LEDs from 87 to 96.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26320649','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26320649"><span>High sensitivity Schottky junction <span class="hlt">diode</span> based on monolithically grown aligned polypyrrole nanofibers: Broad range detection of m-dihydroxybenzene.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ameen, Sadia; Akhtar, M Shaheer; Seo, Hyung-Kee; Shin, Hyung Shik</p> <p>2015-07-30</p> <p>Aligned <span class="hlt">p</span>-type polypyrrole (PPy) nanofibers (NFs) thin film was grown on <span class="hlt">n</span>-type silicon (100) substrate by an electrochemical technique to fabricate Schottky junction <span class="hlt">diode</span> for the efficient detection of m-dihydroxybenzene chemical. The highly dense and well aligned PPy NFs with the average diameter (∼150-200 nm) were grown on <span class="hlt">n</span>-type Si substrate. The formation of aligned PPy NFs was confirmed by elucidating the structural, compositional and the optical properties. The electrochemical behavior of the fabricated Pt/<span class="hlt">p</span>-aligned PPy NFs/<span class="hlt">n</span>-silicon Schottky junction <span class="hlt">diode</span> was evaluated by cyclovoltametry (CV) and current (<span class="hlt">I</span>)-voltage (V) measurements with the variation of m-dihydroxybenzene concentration in the phosphate buffer solution (PBS). The fabricated Pt/<span class="hlt">p</span>-aligned PPy NFs/<span class="hlt">n</span>-silicon Schottky junction <span class="hlt">diode</span> exhibited the rectifying behavior of <span class="hlt">I</span>-V curve with the addition of m-dihydroxybenzene chemical, while a weak rectifying <span class="hlt">I</span>-V behavior was observed without m-dihydroxybenzene chemical. This non-linear <span class="hlt">I</span>-V behavior suggested the formation of Schottky barrier at the interface of Pt layer and <span class="hlt">p</span>-aligned PPy NFs/<span class="hlt">n</span>-silicon thin film layer. By analyzing the <span class="hlt">I</span>-V characteristics, the fabricated Pt/<span class="hlt">p</span>-aligned PPy NFs/<span class="hlt">n</span>-silicon Schottky junction <span class="hlt">diode</span> displayed reasonably high sensitivity ∼23.67 μAmM(-1)cm(-2), good detection limit of ∼1.51 mM with correlation coefficient (R) of ∼0.9966 and short response time (10 s). Copyright © 2015 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22119560','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22119560"><span>Investigation on a radiation tolerant betavoltaic battery based on Schottky barrier <span class="hlt">diode</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Yebing; Hu, Rui; Yang, Yuqing; Wang, Guanquan; Luo, Shunzhong; Liu, Ning</p> <p>2012-03-01</p> <p>An Au-Si Schottky barrier <span class="hlt">diode</span> was studied as the energy conversion device of betavoltaic batteries. Its electrical performance under radiation of Ni-63 and H-3 sources and radiation degradation under Am-241 were investigated and compared with those of the <span class="hlt">p-n</span> junction. The results show that the Schottky <span class="hlt">diode</span> had a higher <span class="hlt">I</span>(sc) and harder radiation tolerance but lower V(oc) than the <span class="hlt">p-n</span> junction. The results indicated that the Schottky <span class="hlt">diode</span> can be a promising candidate for energy conversion of betavoltaic batteries. Copyright © 2011 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1833b0080T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1833b0080T"><span>Analysis of aging time dependent electrical characteristics of AuCu/<span class="hlt">n</span>-Si/Ti Schottky type <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Taser, Ahmet; Şenarslan, Elvan; Güzeldir, Betül; Saǧlam, Mustafa</p> <p>2017-04-01</p> <p>The purpose of this study is to fabricate AuCu/<span class="hlt">n</span>-Si/Ti Schottky type <span class="hlt">diode</span> and determine the effects of aging time on the <span class="hlt">diode</span> parameters such as ideality factor, barrier height, series resistance, interface state density and rectification ratio. Gold and copper ratios in the gold-copper alloy used in making the Schottky contact were taken as equal. Schottky barrier contact using AuCu alloy and ohmic contact using Ti metal were made on <span class="hlt">n</span>-Si by thermal evaporation. The electrical characterization of the AuCu/<span class="hlt">n</span>-Si/Ti <span class="hlt">diode</span> was made immediately based on the aging time at room temperature in dark conditions. The <span class="hlt">I</span>-V measurements were also repeated 1, 7, 15, 30 and 90 days after fabrication of the <span class="hlt">diode</span> in order to observe the effect of the aging time. The determined values of the ideality factor are in the range of 1,21 (for immediately)-1,075 (for 90 days). In the same way, values of the barrier height are also in the range of 0,566 eV (for immediately)-0,584 eV (for 90 days). From the <span class="hlt">I</span>-V characteristics, it is seen that the <span class="hlt">diode</span> appears to have a good rectification character.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22559625','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22559625"><span>Characterization of a novel two dimensional <span class="hlt">diode</span> array the "magic plate" as a radiation <span class="hlt">detector</span> for radiation therapy treatment.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wong, J H D; Fuduli, I; Carolan, M; Petasecca, M; Lerch, M L F; Perevertaylo, V L; Metcalfe, P; Rosenfeld, A B</p> <p>2012-05-01</p> <p>Intensity modulated radiation therapy (IMRT) utilizes the technology of multileaf collimators to deliver highly modulated and complex radiation treatment. Dosimetric verification of the IMRT treatment requires the verification of the delivered dose distribution. Two dimensional ion chamber or <span class="hlt">diode</span> arrays are gaining popularity as a dosimeter of choice due to their real time feedback compared to film dosimetry. This paper describes the characterization of a novel 2D <span class="hlt">diode</span> array, which has been named the "magic plate" (MP). It was designed to function as a 2D transmission <span class="hlt">detector</span> as well as a planar <span class="hlt">detector</span> for dose distribution measurements in a solid water phantom for the dosimetric verification of IMRT treatment delivery. The prototype MP is an 11 × 11 <span class="hlt">detector</span> array based on thin (50 μm) epitaxial <span class="hlt">diode</span> technology mounted on a 0.6 mm thick Kapton substrate using a proprietary "drop-in" technology developed by the Centre for Medical Radiation Physics, University of Wollongong. A full characterization of the <span class="hlt">detector</span> was performed, including radiation damage study, dose per pulse effect, percent depth dose comparison with CC13 ion chamber and build up characteristics with a parallel plane ion chamber measurements, dose linearity, energy response and angular response. Postirradiated magic plate <span class="hlt">diodes</span> showed a reproducibility of 2.1%. The MP dose per pulse response decreased at higher dose rates while at lower dose rates the MP appears to be dose rate independent. The depth dose measurement of the MP agrees with ion chamber depth dose measurements to within 0.7% while dose linearity was excellent. MP showed angular response dependency due to the anisotropy of the silicon <span class="hlt">diode</span> with the maximum variation in angular response of 10.8% at gantry angle 180°. Angular dependence was within 3.5% for the gantry angles ± 75°. The field size dependence of the MP at isocenter agrees with ion chamber measurement to within 1.1%. In the beam perturbation study, the</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_15 --> <div id="page_16" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="301"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SeScT..31k5015F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SeScT..31k5015F"><span>Near-field microscopy of waveguide architectures of InGa<span class="hlt">N/GaN</span> <span class="hlt">diode</span> lasers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Friede, Sebastian; Tomm, Jens W.; Kühn, Sergei; Hoffmann, Veit; Wenzel, Hans; Weyers, Markus</p> <p>2016-11-01</p> <p>Waveguide (WG) architectures of 420 nm emitting InGa<span class="hlt">N/GaN</span> <span class="hlt">diode</span> lasers are analyzed by photoluminescence and photocurrent spectroscopy using a nearfield scanning optical microscope that scans along their front facets. The components of the ‘optical active cavity’, quantum wells, WGs, and cladding layers are individually inspected with a spatial resolution of ∼100 nm. Separate analysis of the <span class="hlt">p</span>- and <span class="hlt">n</span>-sections of the WG was achieved, and reveals defect levels in the <span class="hlt">p</span>-part. Moreover, it is demonstrated that the homogeneity of the <span class="hlt">n</span>-WG section directly affects the quantum wells that are grown on top of this layer. Substantially increased carrier capture efficiencies into InGa<span class="hlt">N/GaN</span>-WGs compared to Ga<span class="hlt">N</span>-WGs are demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApPhL.111h2402E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhL.111h2402E"><span>Electric field control of ferromagnetism at room temperature in GaCr<span class="hlt">N</span> (<span class="hlt">p-i-n</span>) device structures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>El-Masry, N. A.; Zavada, J. M.; Reynolds, J. G.; Reynolds, C. L.; Liu, Z.; Bedair, S. M.</p> <p>2017-08-01</p> <p>We have demonstrated a room temperature dilute magnetic semiconductor based on GaCr<span class="hlt">N</span> epitaxial layers grown by metalorganic chemical vapor deposition. Saturation magnetization Ms increased when the GaCr<span class="hlt">N</span> film is incorporated into a (<span class="hlt">p-GaN/i-GaCrN/n-GaN</span>) device structure, due to the proximity of mediated holes present in the <span class="hlt">p-GaN</span> layer. Zero field cooling and field cooling were measured to ascertain the absence of superparamagnetic behavior in the films. A (<span class="hlt">p-GaN/i-GaCrN/n-GaN</span>) device structure with room temperature ferromagnetic (FM) properties that can be controlled by an external applied voltage has been fabricated. In this work, we show that the applied voltage controls the ferromagnetic properties, by biasing the (<span class="hlt">p-i-n</span>) structure. With forward bias, ferromagnetism in the GaCr<span class="hlt">N</span> layer was increased nearly 4 fold of the original value. Such an enhancement is due to carrier injection of holes into the Cr deep level present in the <span class="hlt">i-GaCrN</span> layer. A "memory effect" for the FM behavior of the (<span class="hlt">p-i-n</span>) GaCr<span class="hlt">N</span> device structure persisted for 42 h after the voltage bias was turned off. These measurements also support that the observed ferromagnetism in the GaCr<span class="hlt">N</span> film is not due to superparamagnetic clusters but instead is a hole-mediated phenomenon.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22594651-asymmetric-quantum-well-structures-algan-gan-algan-resonant-tunneling-diodes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22594651-asymmetric-quantum-well-structures-algan-gan-algan-resonant-tunneling-diodes"><span>Asymmetric quantum-well structures for AlGa<span class="hlt">N/GaN/AlGaN</span> resonant tunneling <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Yang, Lin'an, E-mail: layang@xidian.edu.cn; Li, Yue; Wang, Ying</p> <p></p> <p>Asymmetric quantum-well (QW) structures including the asymmetric potential-barrier and the asymmetric potential-well are proposed for AlGa<span class="hlt">N/GaN/AlGaN</span> resonant tunneling <span class="hlt">diodes</span> (RTDs). Theoretical investigation gives that an appropriate decrease in Al composition and thickness for emitter barrier as well as an appropriate increase of both for collector barrier can evidently improve the negative-differential-resistance characteristic of RTD. Numerical simulation shows that RTD with a 1.5-nm-thick Ga<span class="hlt">N</span> well sandwiched by a 1.3-nm-thick Al{sub 0.15}Ga{sub 0.85}<span class="hlt">N</span> emitter barrier and a 1.7-nm-thick Al{sub 0.25}Ga{sub 0.75}<span class="hlt">N</span> collector barrier can yield the <span class="hlt">I</span>-V characteristic having the peak current (Ip) and the peak-to-valley current ratio (PVCR) of 0.39 A andmore » 3.6, respectively, about double that of RTD with a 1.5-nm-thick Al{sub 0.2}Ga{sub 0.8}<span class="hlt">N</span> for both barriers. It is also found that an introduction of InGa<span class="hlt">N</span> sub-QW into the <span class="hlt">diode</span> can change the tunneling mode and achieve higher transmission coefficient of electron. The simulation demonstrates that RTD with a 2.8-nm-thick In{sub 0.03}Ga{sub 0.97}<span class="hlt">N</span> sub-well in front of a 2.0-nm-thick Ga<span class="hlt">N</span> main-well can exhibit the <span class="hlt">I</span>-V characteristic having Ip and PVCR of 0.07 A and 11.6, about 7 times and double the value of RTD without sub-QW, respectively. The purpose of improving the structure of Ga<span class="hlt">N</span>-based QW is to solve apparent contradiction between the device structure and the device manufacturability of new generation RTDs for sub-millimeter and terahertz applications.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26838391','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26838391"><span>A handheld laser-induced fluorescence <span class="hlt">detector</span> for multiple applications.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fang, Xiao-Xia; Li, Han-Yang; Fang, Pan; Pan, Jian-Zhang; Fang, Qun</p> <p>2016-04-01</p> <p>In this paper, we present a compact handheld laser-induced fluorescence (LIF) <span class="hlt">detector</span> based on a 450 nm laser <span class="hlt">diode</span> and quasi-confocal optical configuration with a total size of 9.1 × 6.2 × 4.1 cm(3). Since there are few reports on the use of 450 nm laser <span class="hlt">diode</span> in LIF detection, especially in miniaturized LIF <span class="hlt">detector</span>, we systematically investigated various optical arrangements suitable for the requirements of 450 nm laser <span class="hlt">diode</span> and system miniaturization, including focusing lens, filter combination, and pinhole, as well as Raman effect of water at 450 nm excitation wavelength. As the result, the handheld LIF <span class="hlt">detector</span> integrates the light source (450 nm laser <span class="hlt">diode</span>), optical circuit module (including a 450 nm band-pass filter, a dichroic mirror, a collimating lens, a 525 nm band-pass filter, and a 1.0mm aperture), optical <span class="hlt">detector</span> (miniaturized photomultiplier tube), as well as electronic module (including signal recording, processing and displaying units). This <span class="hlt">detector</span> is capable of working independently with a cost of ca. $2000 for the whole instrument. The detection limit of the instrument for sodium fluorescein solution is 0.42 <span class="hlt">n</span>M (S/<span class="hlt">N</span>=3). The broad applicability of the present system was demonstrated in capillary electrophoresis separation of fluorescein isothiocyanate (FITC) labeled amino acids and in flow cytometry of tumor cells as an on-line LIF <span class="hlt">detector</span>, as well as in droplet array chip analysis as a LIF scanner. We expect such a compact LIF <span class="hlt">detector</span> could be applied in flow analysis systems as an on-line <span class="hlt">detector</span>, and in field analysis and biosensor analysis as a portable universal LIF <span class="hlt">detector</span>. Copyright © 2015 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11686742','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11686742"><span>In vivo dosimetry using a single <span class="hlt">diode</span> for megavoltage photon beam radiotherapy: implementation and response characterization.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Colussi, V C; Beddar, A S; Kinsella, T J; Sibata, C H</p> <p>2001-01-01</p> <p>The AAPM Task Group 40 reported that in vivo dosimetry can be used to identify major deviations in treatment delivery in radiation therapy. In this paper, we investigate the feasibility of using one single <span class="hlt">diode</span> to perform in vivo dosimetry in the entire radiotherapeutic energy range regardless of its intrinsic buildup material. The only requirement on <span class="hlt">diode</span> selection would be to choose a <span class="hlt">diode</span> with the adequate build up to measure the highest beam energy. We have tested the new <span class="hlt">diodes</span> from Sun Nuclear Corporation (called QED and ISORAD-<span class="hlt">p</span>--both <span class="hlt">p</span>-type) for low-, intermediate-, and high-energy range. We have clinically used both <span class="hlt">diode</span> types to monitor entrance doses. In general, we found that the dose readings from the ISORAD (<span class="hlt">p</span>-type) are closer of the dose expected than QED <span class="hlt">diodes</span> in the clinical setting. In this paper we report on the response of these newly available ISORAD (<span class="hlt">p</span>-type) <span class="hlt">diode</span> <span class="hlt">detectors</span> with respect to certain radiation field parameters such as source-to-surface distance, field size, wedge beam modifiers, as well as other parameters that affect <span class="hlt">detector</span> characteristics (temperature and <span class="hlt">detector</span>-beam orientation). We have characterized the response of the high-energy ISORAD (<span class="hlt">p</span>-type) <span class="hlt">diode</span> in the low- (1-4 MV), intermediate- (6-12 MV), and high-energy (15-25 MV) range. Our results showed that the total variation of the response of high-energy ISORAD (<span class="hlt">p</span>-type) <span class="hlt">diodes</span> to all the above parameters are within +/-5% in most encountered clinical patient treatment setups in the megavoltage photon beam radiotherapy. The usage of the high-energy buildup <span class="hlt">diode</span> has the additional benefit of amplifying the response of the <span class="hlt">diode</span> reading in case the wrong energy is used for patient treatment. In the light of these findings, we have since then switched to using only one single <span class="hlt">diode</span> type, namely the "red" <span class="hlt">diode</span>; manufacturer designation of the ISORAD (<span class="hlt">p</span>-type) high-energy (15-25 MV) range <span class="hlt">diode</span>, for all energies in our institution and satellites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26886870','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26886870"><span>Metal-Insulator-Semiconductor <span class="hlt">Diode</span> Consisting of Two-Dimensional Nanomaterials.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jeong, Hyun; Oh, Hye Min; Bang, Seungho; Jeong, Hyeon Jun; An, Sung-Jin; Han, Gang Hee; Kim, Hyun; Yun, Seok Joon; Kim, Ki Kang; Park, Jin Cheol; Lee, Young Hee; Lerondel, Gilles; Jeong, Mun Seok</p> <p>2016-03-09</p> <p>We present a novel metal-insulator-semiconductor (MIS) <span class="hlt">diode</span> consisting of graphene, hexagonal BN, and monolayer MoS2 for application in ultrathin nanoelectronics. The MIS heterojunction structure was fabricated by vertically stacking layered materials using a simple wet chemical transfer method. The stacking of each layer was confirmed by confocal scanning Raman spectroscopy and device performance was evaluated using current versus voltage (<span class="hlt">I</span>-V) and photocurrent measurements. We clearly observed better current rectification and much higher current flow in the MIS <span class="hlt">diode</span> than in the <span class="hlt">p-n</span> junction and the metal-semiconductor <span class="hlt">diodes</span> made of layered materials. The <span class="hlt">I</span>-V characteristic curve of the MIS <span class="hlt">diode</span> indicates that current flows mainly across interfaces as a result of carrier tunneling. Moreover, we observed considerably high photocurrent from the MIS <span class="hlt">diode</span> under visible light illumination.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10460E..1CW','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10460E..1CW"><span>Ga<span class="hlt">N</span> ultraviolet <span class="hlt">p-i-n</span> photodetectors with enhanced deep ultraviolet quantum efficiency</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Guosheng; Xie, Feng; Wang, Jun; Guo, Jin</p> <p>2017-10-01</p> <p>Ga<span class="hlt">N</span> ultraviolet (UV) <span class="hlt">p-i-n</span> photodetectors (PDs) with a thin <span class="hlt">p-AlGaN/GaN</span> contact layer are designed and fabricated. The PD exhibits a low dark current density of˜7 <span class="hlt">n</span>A/cm2 under -5 V, and a zero-bias peak responsivity of ˜0.16 A/W at 360 nm, which corresponds to a maximum quantum efficiency of 55%. It is found that, in the wavelength range between 250 and 365 nm, the PD with thin <span class="hlt">p-AlGaN/GaN</span> contact layer exhibits enhanced quantum efficiency especially in a deep-UV wavelength range, than that of the control PD with conventional thin <span class="hlt">p-GaN</span> contact layer. The improved quantum efficiency of the PD with thin <span class="hlt">p-AlGaN/GaN</span> contact layer in the deep-UV wavelength range is mainly attributed to minority carrier reflecting properties of thin <span class="hlt">p-AlGaN/GaN</span> heterojunction which could reduce the surface recombination loss of photon-generated carriers and improve light current collection efficiency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22493975-su-quantitative-evaluation-dose-distributions-from-axial-helical-cone-beam-ct-imaging-measurement-using-two-dimensional-diode-array-detector','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22493975-su-quantitative-evaluation-dose-distributions-from-axial-helical-cone-beam-ct-imaging-measurement-using-two-dimensional-diode-array-detector"><span>SU-E-<span class="hlt">I</span>-15: Quantitative Evaluation of Dose Distributions From Axial, Helical and Cone-Beam CT Imaging by Measurement Using a Two-Dimensional <span class="hlt">Diode</span>-Array <span class="hlt">Detector</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Chacko, M; Aldoohan, S; Sonnad, J</p> <p>2015-06-15</p> <p>Purpose: To evaluate quantitatively dose distributions from helical, axial and cone-beam CT clinical imaging techniques by measurement using a two-dimensional (2D) <span class="hlt">diode</span>-array <span class="hlt">detector</span>. Methods: 2D-dose distributions from selected clinical protocols used for axial, helical and cone-beam CT imaging were measured using a <span class="hlt">diode</span>-array <span class="hlt">detector</span> (MapCheck2). The MapCheck2 is composed from solid state <span class="hlt">diode</span> <span class="hlt">detectors</span> that are arranged in horizontal and vertical lines with a spacing of 10 mm. A GE-Light-Speed CT-simulator was used to acquire axial and helical CT images and a kV on-board-imager integrated with a Varian TrueBeam-STx machine was used to acquire cone-beam CT (CBCT) images. Results: Themore » dose distributions from axial, helical and cone-beam CT were non-uniform over the region-of-interest with strong spatial and angular dependence. In axial CT, a large dose gradient was measured that decreased from lateral sides to the middle of the phantom due to large superficial dose at the side of the phantom in comparison with larger beam attenuation at the center. The dose decreased at the superior and inferior regions in comparison to the center of the phantom in axial CT. An asymmetry was found between the right-left or superior-inferior sides of the phantom which possibly to angular dependence in the dose distributions. The dose level and distribution varied from one imaging technique into another. For the pelvis technique, axial CT deposited a mean dose of 3.67 cGy, helical CT deposited a mean dose of 1.59 cGy, and CBCT deposited a mean dose of 1.62 cGy. Conclusions: MapCheck2 provides a robust tool to measure directly 2D-dose distributions for CT imaging with high spatial resolution <span class="hlt">detectors</span> in comparison with ionization chamber that provides a single point measurement or an average dose to the phantom. The dose distributions measured with MapCheck2 consider medium heterogeneity and can represent specific patient dose.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhEn...7b2502W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhEn...7b2502W"><span>Design of thin InGaAs<span class="hlt">N</span>(Sb) <span class="hlt">n-i-p</span> junctions for use in four-junction concentrating photovoltaic devices</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wilkins, Matthew M.; Gupta, James; Jaouad, Abdelatif; Bouzazi, Boussairi; Fafard, Simon; Boucherif, Abderraouf; Valdivia, Christopher E.; Arès, Richard; Aimez, Vincent; Schriemer, Henry P.; Hinzer, Karin</p> <p>2017-04-01</p> <p>Four-junction solar cells for space and terrestrial applications require a junction with a band gap of ˜1 eV for optimal performance. InGaAs<span class="hlt">N</span> or InGaAs<span class="hlt">N</span>(Sb) dilute nitride junctions have been demonstrated for this purpose, but in achieving the 14 mA/cm2 short-circuit current needed to match typical GaIn<span class="hlt">P</span> and GaAs junctions, the open-circuit voltage (VOC) and fill factor of these junctions are compromised. In multijunction devices incorporating materials with short diffusion lengths, we study the use of thin junctions to minimize sensitivity to varying material quality and ensure adequate transmission into lower junctions. An <span class="hlt">n-i-p</span> device with 0.65-μm absorber thickness has sufficient short-circuit current, however, it relies less heavily on field-aided collection than a device with a 1-μm absorber. Our standard cell fabrication process, which includes a rapid thermal anneal of the contacts, yields a significant improvement in diffusion length and device performance. By optimizing a four-junction cell around a smaller 1-sun short-circuit current of 12.5 mA/cm2, we produced an InGaAs<span class="hlt">N</span>(Sb) junction with open-circuit voltage of 0.44 V at 1000 suns (1 sun=100 mW/cm2), <span class="hlt">diode</span> ideality factor of 1.4, and sufficient light transmission to allow >12.5 mA/cm2 in all four subcells.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApPhA.123..234W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhA.123..234W"><span>High-performance tandem organic light-emitting <span class="hlt">diodes</span> based on a buffer-modified <span class="hlt">p/n</span>-type planar organic heterojunction as charge generation layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, Yukun; Sun, Ying; Qin, Houyun; Hu, Shoucheng; Wu, Qingyang; Zhao, Yi</p> <p>2017-04-01</p> <p>High-performance tandem organic light-emitting <span class="hlt">diodes</span> (TOLEDs) were realized using a buffer-modified <span class="hlt">p/n</span>-type planar organic heterojunction (OHJ) as charge generation layer (CGL) consisting of common organic materials, and the configuration of this <span class="hlt">p/n</span>-type CGL was "LiF/<span class="hlt">N,N'-diphenyl-N,N</span>'-bis(1-napthyl)-1,1'-biphenyl-4,4'-diamine (NPB)/4,7-diphenyl-1,10-phenanthroline (Bphen)/molybdenum oxide (MoOx)". The optimized TOLED exhibited a maximum current efficiency of 77.6 cd/A without any out-coupling techniques, and the efficiency roll-off was greatly improved compared to the single-unit OLED. The working mechanism of the <span class="hlt">p/n</span>-type CGL was discussed in detail. It is found that the NPB/Bphen heterojunction generated enough charges under a forward applied voltage and the carrier extraction was a tunneling process. These results could provide a new method to fabricate high-performance TOLEDs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004APS..MARD26001Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004APS..MARD26001Z"><span>Bipolar Spintronics: From magnetic <span class="hlt">diodes</span> to magnetic bipolar transistors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zutic, Igor</p> <p>2004-03-01</p> <p>We develop a theory of bipolar (electrons and holes) spin-polarized transport [1,2] in semiconductors and discuss its implications for spintronic devices [3]. In our proposal for magnetic bipolar transistors [4,5] we show how bipolar spintronics can lead to spin and magnetic field controlled active devices, not limited by the magnetoresistive effects used in all-metallic structures [3]. We focus on magnetic <span class="hlt">p-n</span> <span class="hlt">diodes</span> [1,2] with spatially dependent spin splitting (Zeeman or exchange) of carrier bands. An exchange splitting can be provided by ferromagnetic semiconductors [6], while a large Zeeman splitting can be realized in the presence of magnetic field in magnetically doped or narrow band gap semiconductors [3]. Our theory of magnetic <span class="hlt">diodes</span> [1,2] can be directly applied to magnetic bipolar transistors--the three-terminal devices which consist of two magnetic <span class="hlt">p-n</span> <span class="hlt">diodes</span> connected in series [4,5]. Predictions of exponentially large magnetoresistance [1] and a strong coupling between the spin and charge transport leading to the spin-voltaic effect [1,7] for magnetic <span class="hlt">diodes</span> are also relevant for magnetic bipolar transistors. In particular, in <span class="hlt">n-p-n</span> transistors, we show the importance of considering the nonequilibrium spin leading to the spin-voltaic effect. In addition to the applied magnetic filed, the injected nonequilibrium spin can be used to dynamically control the current amplification (gain). Recent experimental progress [8,9] supports the viability of our theoretical proposals. [1] <span class="hlt">I</span>. Zutic, J. Fabian, S. Das Sarma, Phys. Rev. Lett. 88, 066603 (2002). [2] J. Fabian, <span class="hlt">I</span>. Zutic, S. Das Sarma, Phys. Rev. B 66, 165301 (2002). [3] <span class="hlt">I</span>. Zutic, J. Fabian, S. Das Sarma, Rev. Mod. Phys., in press. [4] J. Fabian, <span class="hlt">I</span>. Zutic, S. Das Sarma, cond-mat/0211639; cond-mat/0307014, Appl. Phys. Lett., in press. [5] J. Fabian and <span class="hlt">I</span>. Zutic, cond-mat/0311456. [6] H. Ohno, Science 281, 951 (1998). [7] <span class="hlt">I</span>. Zutic, J. Fabian, S. Das Sarma, Appl. Phys. Lett. 82, 221 (2003). [8] <span class="hlt">N</span>. Samarth</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NIMPA.877...34B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NIMPA.877...34B"><span>RESONEUT: A <span class="hlt">detector</span> system for spectroscopy with (d,<span class="hlt">n</span>) reactions in inverse kinematics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baby, L. T.; Kuvin, S. A.; Wiedenhöver, I.; Anastasiou, M.; Caussyn, D.; Colbert, K.; Quails, N.; Gay, D.</p> <p>2018-01-01</p> <p>The RESONEUT <span class="hlt">detector</span> setup is described, which was developed for resonance spectroscopy using (d,<span class="hlt">n</span>) reactions with radioactive beams in inverse kinematics and at energies around the Coulomb barrier. The goal of experiments with this setup is to determine the spectrum and proton-transfer strengths of the low-lying resonances, which have an impact on astrophysical reaction rates. The setup is optimized for l = 0 proton transfers in inverse kinematics, for which most neutrons are emitted at backward angles with energies in the 80-300 keV range. The <span class="hlt">detector</span> system is comprised of 9 <span class="hlt">p</span>-terphenyl scintillators as neutron <span class="hlt">detectors</span>, two annular silicon-strip <span class="hlt">detectors</span> for light charged particles, one position-resolving gas ionization chamber for heavy ion detection, and a barrel of Na<span class="hlt">I-detectors</span> for the detection of γ-rays. The <span class="hlt">detector</span> commissioning and performance characteristics are described with an emphasis on the neutron-<span class="hlt">detector</span> components.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23938509','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23938509"><span>Improvement of UV electroluminescence of <span class="hlt">n-ZnO/p-GaN</span> heterojunction LED by ZnS interlayer.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Lichun; Li, Qingshan; Shang, Liang; Wang, Feifei; Qu, Chong; Zhao, Fengzhou</p> <p>2013-07-15</p> <p><span class="hlt">n-ZnO/p-GaN</span> heterojunction light emitting <span class="hlt">diodes</span> with different interfacial layers were fabricated by pulsed laser deposition. The electroluminescence (EL) spectra of the <span class="hlt">n-ZnO/p-GaN</span> <span class="hlt">diodes</span> display a broad blue-violet emission centered at 430 nm, whereas the <span class="hlt">n-ZnO/ZnS/p-GaN</span> and <span class="hlt">n-ZnO/AlN/p-GaN</span> devices exhibit ultraviolet (UV) emission. Compared with the Al<span class="hlt">N</span> interlayer, which is blocking both electron and hole at hetero-interface, the utilization of ZnS as intermediate layer can lower the barrier height for holes and keep an effective blocking for electron. Thus, an improved UV EL intensity and a low turn-on voltage (~5V) were obtained. The results were studied by peak-deconvolution with Gaussian functions and were discussed using the band diagram of heterojunctions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22489048-ingan-based-micro-light-emitting-diodes-featuring-buried-gan-tunnel-junction','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22489048-ingan-based-micro-light-emitting-diodes-featuring-buried-gan-tunnel-junction"><span>InGa<span class="hlt">N</span> based micro light emitting <span class="hlt">diodes</span> featuring a buried Ga<span class="hlt">N</span> tunnel junction</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Malinverni, M., E-mail: marco.malinverni@epfl.ch; Martin, D.; Grandjean, N.</p> <p></p> <p>Ga<span class="hlt">N</span> tunnel junctions (TJs) are grown by ammonia molecular beam epitaxy. High doping levels are achieved with a net acceptor concentration close to ∼10{sup 20 }cm{sup −3}, thanks to the low growth temperature. This allows for the realization of <span class="hlt">p-n</span> junctions with ultrathin depletion width enabling efficient interband tunneling. <span class="hlt">n-p-n</span> structures featuring such a TJ exhibit low leakage current densities, e.g., <5 × 10{sup −5} A cm{sup −2} at reverse bias of 10 V. Under forward bias, the voltage is 3.3 V and 4.8 V for current densities of 20 A cm{sup −2} and 2000 A cm{sup −2}, respectively. The specific series resistance of the whole device ismore » 3.7 × 10{sup −4} Ω cm{sup 2}. Then micro-light emitting <span class="hlt">diodes</span> (μ-LEDs) featuring buried TJs are fabricated. Excellent current confinement is demonstrated together with homogeneous electrical injection, as seen on electroluminescence mapping. Finally, the <span class="hlt">I</span>-V characteristics of μ-LEDs with various diameters point out the role of the access resistance at the current aperture edge.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22492338-temperature-dependent-electrical-characterisation-pt-hfo-sub-gan-metal-insulator-semiconductor-mis-schottky-diodes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22492338-temperature-dependent-electrical-characterisation-pt-hfo-sub-gan-metal-insulator-semiconductor-mis-schottky-diodes"><span>Temperature dependent electrical characterisation of Pt/HfO{sub 2}/<span class="hlt">n-GaN</span> metal-insulator-semiconductor (MIS) Schottky <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Shetty, Arjun, E-mail: arjun@ece.iisc.ernet.in; Vinoy, K. J.; Roul, Basanta</p> <p>2015-09-15</p> <p>This paper reports an improvement in Pt/<span class="hlt">n-GaN</span> metal-semiconductor (MS) Schottky <span class="hlt">diode</span> characteristics by the introduction of a layer of HfO{sub 2} (5 nm) between the metal and semiconductor interface. The resulting Pt/HfO{sub 2}/<span class="hlt">n-GaN</span> metal-insulator-semiconductor (MIS) Schottky <span class="hlt">diode</span> showed an increase in rectification ratio from 35.9 to 98.9(@ 2V), increase in barrier height (0.52 eV to 0.63eV) and a reduction in ideality factor (2.1 to 1.3) as compared to the MS Schottky. Epitaxial <span class="hlt">n</span>-type Ga<span class="hlt">N</span> films of thickness 300nm were grown using plasma assisted molecular beam epitaxy (PAMBE). The crystalline and optical qualities of the films were confirmed using high resolutionmore » X-ray diffraction and photoluminescence measurements. Metal-semiconductor (Pt/<span class="hlt">n-GaN</span>) and metal-insulator-semiconductor (Pt/HfO{sub 2}/<span class="hlt">n-GaN</span>) Schottky <span class="hlt">diodes</span> were fabricated. To gain further understanding of the Pt/HfO{sub 2}/Ga<span class="hlt">N</span> interface, <span class="hlt">I</span>-V characterisation was carried out on the MIS Schottky <span class="hlt">diode</span> over a temperature range of 150 K to 370 K. The barrier height was found to increase (0.3 eV to 0.79 eV) and the ideality factor decreased (3.6 to 1.2) with increase in temperature from 150 K to 370 K. This temperature dependence was attributed to the inhomogeneous nature of the contact and the explanation was validated by fitting the experimental data into a Gaussian distribution of barrier heights.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1375367-all-perovskite-junction-based-transparent-conducting-la-sr-cro-epitaxial-layers','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1375367-all-perovskite-junction-based-transparent-conducting-la-sr-cro-epitaxial-layers"><span>An all-perovskite <span class="hlt">p-n</span> junction based on transparent conducting <span class="hlt">p</span> -La 1-x Sr x CrO 3 epitaxial layers</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Du, Yingge; Li, Chen; Zhang, Kelvin H. L.</p> <p>2017-08-07</p> <p>Transparent, conducting <span class="hlt">p</span> -La 1-x Sr x CrO 3 epitaxial layers were deposited on Nb-doped SrTiO 3(001) by oxygen-assisted molecular beam epitaxy to form structurally coherent <span class="hlt">p-n</span> junctions. X-ray photoelectron spectroscopy reveals a type II or “staggered” band alignment, with valence and conduction band offsets of 2.0 eV and 0.9 eV, respectively. <span class="hlt">Diodes</span> fabricated from these heterojunctions exhibit rectifying behavior, and the <span class="hlt">I</span>-V characteristics are different from those for traditional semiconductor <span class="hlt">p-n</span> junctions. A rather large ideality factor is ascribed to the complex nature of the interface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22590995-beam-related-response-vivo-diode-detectors-external-radiotherapy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22590995-beam-related-response-vivo-diode-detectors-external-radiotherapy"><span>Beam related response of in vivo <span class="hlt">diode</span> <span class="hlt">detectors</span> for external radiotherapy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Baci, Syrja, E-mail: sbarci2013@gmail.com; Telhaj, Ervis; Malkaj, Partizan</p> <p>2016-03-25</p> <p>In Vivo Dosimetry (IVD) is a set of methods used in cancer treatment clinics to determine the real dose of radiation absorbed by target volume in a patient’s body. IVD has been widely implemented in radiotherapy treatment centers and is now recommended part of Quality Assurance program by many International health and radiation organizations. Because of cost and lack of specialized personnel, IVD has not been practiced as yet, in Albanian radiotherapy clinics. At Hygeia Hospital Tirana, patients are irradiated with high energy photons generated by Elekta Synergy Accelerators. We have recently started experimenting with the purpose of establishing anmore » IVD practice at this hospital. The first set of experiments was aimed at calibration of <span class="hlt">diodes</span> that are going to be used for IVD. PMMA, phantoms by PTW were used to calibrate <span class="hlt">p</span> – type Si, semiconductor <span class="hlt">diode</span> dosimeters, made by PTW Freiburg for entrance dose. Response of the <span class="hlt">detectors</span> is affected by energy of the beam, accumulated radiation dose, dose rate, temperature, angle against the beam axis, etc. Here we present the work done for calculating calibration factor and correction factors of source to surface distance, field size, and beam incidence for the entrance dose for both 6 MV photon beam and 18 MV photon beam. Dependence of dosimeter response was found to be more pronounced with source to surface distance as compared to other variables investigated.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APExp...9f1004M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APExp...9f1004M"><span>InGa<span class="hlt">N</span> laser <span class="hlt">diode</span> with metal-free laser ridge using <span class="hlt">n+-GaN</span> contact layers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Malinverni, Marco; Tardy, Camille; Rossetti, Marco; Castiglia, Antonino; Duelk, Marcus; Vélez, Christian; Martin, Denis; Grandjean, Nicolas</p> <p>2016-06-01</p> <p>We report on InGa<span class="hlt">N</span> edge emitting laser <span class="hlt">diodes</span> with a top metal electrode located beside the laser ridge. Current spreading over the ridge is achieved via a highly doped <span class="hlt">n</span>+-type Ga<span class="hlt">N</span> layer deposited on top of the structure. The low sheet resistance of the <span class="hlt">n+-GaN</span> layer ensures excellent lateral current spreading, while carrier injection is confined all along the ridge thanks to current tunneling at the interface between the <span class="hlt">n+-GaN</span> top layer and the <span class="hlt">p++-GaN</span> layer. Continuous-wave lasing at 400 nm with an output power of 100 mW is demonstrated on uncoated facet devices with a threshold current density of 2.4 kA·cm-2.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22395576-embeded-photonic-crystal-interface-gan-ag-reflector-improve-light-extraction-gan-based-flip-chip-light-emitting-diode','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22395576-embeded-photonic-crystal-interface-gan-ag-reflector-improve-light-extraction-gan-based-flip-chip-light-emitting-diode"><span>Embeded photonic crystal at the interface of <span class="hlt">p-GaN</span> and Ag reflector to improve light extraction of Ga<span class="hlt">N</span>-based flip-chip light-emitting <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Zhen, Aigong; Ma, Ping, E-mail: maping@semi.ac.cn; Zhang, Yonghui</p> <p>2014-12-22</p> <p>In this experiment, a flip-chip light-emitting <span class="hlt">diode</span> with photonic crystal was fabricated at the interface of <span class="hlt">p-GaN</span> and Ag reflector via nanospheres lithography technique. In this structure, photonic crystal could couple with the guide-light efficiently by reason of the little distance between photonic crystal and active region. The light output power of light emitting <span class="hlt">diode</span> with embedded photonic crystal was 1.42 times larger than that of planar flip-chip light-emitting <span class="hlt">diode</span>. Moreover, the embedded photonic crystal structure makes the far-field divergence angle decreased by 18° without spectra shift. The three-dimensional finite difference time domain simulation results show that photonic crystal couldmore » improve the light extraction, and enhance the light absorption caused by Ag reflector simultaneously, because of the roughed surface. The depth of photonic crystal is the key parameter affecting the light extraction and absorption. Light extraction efficiency increases with the depth photonic crystal structure rapidly, and reaches the maximum at the depth 80 nm, beyond which light extraction decrease drastically.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890056098&hterms=tunnel+diodes&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtunnel%2Bdiodes','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890056098&hterms=tunnel+diodes&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtunnel%2Bdiodes"><span>Submicron nickel-oxide-gold tunnel <span class="hlt">diode</span> <span class="hlt">detectors</span> for rectennas</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hoofring, A. B.; Kapoor, V. J.; Krawczonek, W.</p> <p>1989-01-01</p> <p>The characteristics of a metal-oxide-metal (MOM) tunnel <span class="hlt">diode</span> made of nickel, nickel-oxide, and gold, designed and fabricated by standard integrated circuit technology for use in FIR rectennas, are presented. The MOM tunnel <span class="hlt">diode</span> was formed by overlapping a 0.8-micron-wide layer of 1000-A of nickel, which was oxidized to form a thin layer of nickel oxide, with a 1500 A-thick layer of gold. The dc current-voltage characteristics of the MOM <span class="hlt">diode</span> showed that the current dependence on voltage was linear about zero bias up to a bias of about 70 mV. The maximum detection of a low-level signal (10-mV ac) was determined to be at a dc voltage of 70 mV across the MOM <span class="hlt">diode</span>. The rectified output signal due to a chopped 10.6-micron CO2 laser incident upon the rectenna device was found to increase with dc bias, with a maximum value of 1000 <span class="hlt">n</span>V for a junction bias of 100 mV at room temperature.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29624304','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29624304"><span>Reduced Graphene Oxide/Single-Walled Carbon Nanotube Hybrid Films Using Various <span class="hlt">p</span>-Type Dopants and Their Application to Ga<span class="hlt">N</span>-Based Light-Emitting <span class="hlt">Diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lee, Byeong Ryong; Kim, Tae Geun</p> <p>2017-01-01</p> <p>This article reports the electrical and optical properties of the reduced graphene oxide (RGO)/single-walled carbon nanotube (SWCNT) films using various <span class="hlt">p</span>-type dopants and their application to Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span>. To enhance the current injection and spreading of the RGO/SWCNT films on the light-emitting <span class="hlt">diodes</span> (LEDs), we increased the work function (Φ) of the films using chemical doping with AuCl₃, poly(3,4-ethylenedioxythiophene) oxidized with poly(4-styrenesulfonate) (PEDOT:PSS) and MoO₃; thereby reduced the Schottky barrier height between the RGO/SWCNT films and <span class="hlt">p-GaN</span>. By comparison, LEDs fabricated with work-function-tuned RGO/SWCNT film doped with MoO₃ exhibited the decrease of the forward voltage from 5.3 V to 5.02 V at 20 mA and the increase of the output power up to 1.26 times. We also analyzed the current injection mechanism using ultraviolet photoelectron spectroscopy and X-ray photoelectron spectroscopy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27427691','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27427691"><span>Reduced Graphene Oxide/Single-Walled Carbon Nanotube Hybrid Film Using Various <span class="hlt">p</span>-Type Dopants and Its Application to Ga<span class="hlt">N</span>-Based Light-Emitting <span class="hlt">Diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lee, Byeong Ryong; Kim, Tae Geun</p> <p>2016-06-01</p> <p>This paper reports the electrical and optical properties of the reduced graphene oxide (RGO)/single-walled carbon nanotube (SWNT) films using various <span class="hlt">p</span>-type dopants and its application to Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span>. To enhance the current injection and spreading of the RGO/SWNT films on the light-emitting <span class="hlt">diodes</span> (LEDs), we increased the work function (φ) of the films using chemical doping with AuCl3, poly(3,4-ethylenedioxythiophene) oxidized with poly(4-styrenesulfonate) ( PSS) and MoO3; thereby reduced the Schottky barrier height between the RGO/SWNT films and <span class="hlt">p-GaN</span>. By comparison, LEDs fabricated with work-function-tuned RGO/SWNT film doped with MoO3 exhibited the decrease of the forward voltage from 5.3 V to 5.02 V at 20 mA and the increase of the output power up to 1.26 times. We also analyzed the current injection mechanism using ultraviolet photoelectron spectroscopy and X-ray photoelectron spectroscopy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Colorimeter&id=EJ1033281','ERIC'); return false;" href="https://eric.ed.gov/?q=Colorimeter&id=EJ1033281"><span>A Simple, Small-Scale Lego Colorimeter with a Light-Emitting <span class="hlt">Diode</span> (LED) Used as <span class="hlt">Detector</span></span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Asheim, Jonas; Kvittingen, Eivind V.; Kvittingen, Lise; Verley, Richard</p> <p>2014-01-01</p> <p>This article describes how to construct a simple, inexpensive, and robust colorimeter from a few Lego bricks, in which one light-emitting <span class="hlt">diode</span> (LED) is used as a light source and a second LED as a light <span class="hlt">detector</span>. The colorimeter is suited to various grades and curricula.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790009079','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790009079"><span><span class="hlt">Diode</span> step stress program, JANTX1<span class="hlt">N</span>5614</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1978-01-01</p> <p>The reliability of switching <span class="hlt">diode</span> JANTX1<span class="hlt">N</span>5614 was tested. The effect of power/temperature step stress on the <span class="hlt">diode</span> was determined. Control sample units were maintained for verification of the electrical parametric testing. Results are reported.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5421009','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/5421009"><span>Improved method of preparing <span class="hlt">p-i-n</span> junctions in amorphous silicon semiconductors</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Madan, A.</p> <p>1984-12-10</p> <p>A method of preparing <span class="hlt">p</span>/sup +/-<span class="hlt">i-n</span>/sup +/ junctions for amorphous silicon semiconductors includes depositing amorphous silicon on a thin layer of trivalent material, such as aluminum, indium, or gallium at a temperature in the range of 200/sup 0/C to 250/sup 0/C. At this temperature, the layer of trivalent material diffuses into the amorphous silicon to form a graded <span class="hlt">p</span>/sup +/-<span class="hlt">i</span> junction. A layer of <span class="hlt">n</span>-type doped material is then deposited onto the intrinsic amorphous silicon layer in a conventional manner to finish forming the <span class="hlt">p</span>/sup +/-<span class="hlt">i-n</span>/sup +/ junction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21992363','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21992363"><span>Extraction of depth-dependent perturbation factors for silicon <span class="hlt">diodes</span> using a plastic scintillation <span class="hlt">detector</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lacroix, Frederic; Guillot, Mathieu; McEwen, Malcolm; Gingras, Luc; Beaulieu, Luc</p> <p>2011-10-01</p> <p>This work presents the experimental extraction of the perturbation factor in megavoltage electron beams for three models of silicon <span class="hlt">diodes</span> (IBA Dosimetry, EFD and SFD, and the PTW 60012 unshielded) using a plastic scintillation <span class="hlt">detector</span> (PSD). The authors used a single scanning PSD mounted on a high-precision scanning tank to measure depth-dose curves in 6-, 12-, and 18-MeV clinical electron beams. They also measured depth-dose curves using the IBA Dosimetry, EFD and SFD, and the PTW 60012 unshielded <span class="hlt">diodes</span>. The authors used the depth-dose curves measured with the PSD as a perturbation-free reference to extract the perturbation factors of the <span class="hlt">diodes</span>. The authors found that the perturbation factors for the <span class="hlt">diodes</span> increased substantially with depth, especially for low-energy electron beams. The experimental results show the same trend as published Monte Carlo simulation results for the EFD <span class="hlt">diode</span>; however, the perturbations measured experimentally were greater. They found that using an effective point of measurement (EPOM) placed slightly away from the source reduced the variation of perturbation factors with depth and that the optimal EPOM appears to be energy dependent. The manufacturer recommended EPOM appears to be incorrect at low electron energy (6 MeV). In addition, the perturbation factors for <span class="hlt">diodes</span> may be greater than predicted by Monte Carlo simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070020162','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070020162"><span>Bias Selectable Dual Band AlGa<span class="hlt">N</span> Ultra-violet <span class="hlt">Detectors</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yan, Feng; Miko, Laddawan; Franz, David; Guan, Bing; Stahle, Carl M.</p> <p>2007-01-01</p> <p>Bias selectable dual band AlGa<span class="hlt">N</span> ultra-violet (UV) <span class="hlt">detectors</span>, which can separate UV-A and UV-B using one <span class="hlt">detector</span> in the same pixel by bias switching, have been designed, fabricated and characterized. A two-terminal <span class="hlt">n-p-n</span> photo-transistor-like structure was used. When a forward bias is applied between the top electrode and the bottom electrode, the <span class="hlt">detectors</span> can successfully detect W-A and reject UV-B. Under reverse bias, they can detect UV-B and reject UV-A. The proof of concept design shows that it is feasible to fabricate high performance dual-band UV <span class="hlt">detectors</span> based on the current AlGa<span class="hlt">N</span> material growth and fabrication technologies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5711122','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5711122"><span>Clinical radiation therapy measurements with a new commercial synthetic single crystal diamond <span class="hlt">detector</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Crilly, Richard</p> <p>2014-01-01</p> <p>A commercial version of a synthetic single crystal diamond <span class="hlt">detector</span> (SCDD) in a Schottky <span class="hlt">diode</span> configuration was recently released as the new type 60019 microDiamond <span class="hlt">detector</span> (PTW‐Freiburg, Germany). In this study we investigate the dosimetric properties of this <span class="hlt">detector</span> to independently confirm that findings from the developing group of the SCDDs still hold true for the commercial version of the SCDDs. We further explore if the use of the microDiamond <span class="hlt">detector</span> can be expanded to high‐energy photon beams of up to 15 MV and to large field measurements. Measurements were performed with an Elekta Synergy linear accelerator delivering 6, 10, and 15 MV X‐rays, as well as 6, 9, 12, 15, and 20 MeV electron beams. The dependence of the microdiamond <span class="hlt">detector</span> response on absorbed dose after connecting the <span class="hlt">detector</span> was investigated. Furthermore, the dark current of the diamond <span class="hlt">detector</span> was observed after irradiation. Results are compared to similar results from measurements with a diamond <span class="hlt">detector</span> type 60003. Energy dependency was investigated, as well. Photon depth‐dose curves were measured for field sizes 3×3,10×10, and 30×30cm2. PDDs were measured with the Semiflex type 31010 <span class="hlt">detector</span>, microLion type 31018 <span class="hlt">detector</span>, <span class="hlt">P</span> <span class="hlt">Diode</span> type 60016, SRS <span class="hlt">Diode</span> type 60018, and the microDiamond type 60019 <span class="hlt">detector</span> (all PTW‐Freiburg). Photon profiles were measured at a depth of 10 cm. Electron depth‐dose curves normalized to the dose maximum were measured with the 14×14cm2 electron cone. PDDs were measured with a Markus chamber type 23343, an E <span class="hlt">Diode</span> type 60017 and the microDiamond type 60019 <span class="hlt">detector</span> (all PTW‐Freiburg). Profiles were measured with the E <span class="hlt">Diode</span> and microDiamond at half of D90,D90,D70, and D50 depths and for electron cone sizes of 6×6cm2, 14×14cm2, and 20×20cm2. Within a tolerance of 0.5% <span class="hlt">detector</span> response of the investigated <span class="hlt">detector</span> was stable without any preirradiation. After preirradition with approximately 250 cGy the <span class="hlt">detector</span> response was stable</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JaJAP..57f7201T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JaJAP..57f7201T"><span>Various vibration modes in a silicon ring resonator driven by p–<span class="hlt">n</span> <span class="hlt">diode</span> actuators formed in the lateral direction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsushima, Takafumi; Asahi, Yoichi; Tanigawa, Hiroshi; Furutsuka, Takashi; Suzuki, Kenichiro</p> <p>2018-06-01</p> <p>In this paper, we describe p–<span class="hlt">n</span> <span class="hlt">diode</span> actuators that are formed in the lateral direction on resonators. Because previously reported p–<span class="hlt">n</span> <span class="hlt">diode</span> actuators, which were driven by a force parallel to the electrostatic force induced in a p–<span class="hlt">n</span> <span class="hlt">diode</span>, were fabricated in the perpendicular direction to the surface, the fabrication process to satisfy the requirement of realizing a p–<span class="hlt">n</span> junction set in the middle of the plate thickness has been difficult. The resonators in this work are driven by p–<span class="hlt">n</span> <span class="hlt">diodes</span> formed in the lateral direction, making the process easy. We have fabricated a silicon ring resonator that has in-plane vibration using p–n–<span class="hlt">p</span> and n–p–<span class="hlt">n</span> <span class="hlt">diode</span> actuators formed in the lateral direction. First, we consider a space charge model that can sufficiently accurately describe the force induced in p–<span class="hlt">n</span> <span class="hlt">diode</span> actuators and compare it with the capacitance model used in most computer simulations. Then, we show that multiplying the vibration amplitude calculated by computer simulation by the modification coefficient of 4/3 provides the vibration amplitude in the p–<span class="hlt">n</span> <span class="hlt">diode</span> actuators. Good agreement of the theory with experimental results of the in-plane vibration measured for silicon ring resonators is obtained. The computer simulation is very useful for evaluating various vibration modes in resonators driven by the p–<span class="hlt">n</span> <span class="hlt">diode</span> actuators. The small amplitude of the p–<span class="hlt">n</span> <span class="hlt">diode</span> actuator measured in this work is expected to increase greatly with increased doping of the actuator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17854162','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17854162"><span>Quenching of <span class="hlt">I</span>(2<span class="hlt">P</span>1/2) by NO2, <span class="hlt">N</span>2O4, and <span class="hlt">N</span>2O.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kabir, Md Humayun; Azyazov, Valeriy N; Heaven, Michael C</p> <p>2007-10-11</p> <p>Quenching of excited iodine atoms (<span class="hlt">I</span>(5<span class="hlt">p</span>5, 2<span class="hlt">P</span>1/2)) by nitrogen oxides are processes of relevance to discharge-driven oxygen iodine lasers. Rate constants at ambient and elevated temperatures (293-380 K) for quenching of <span class="hlt">I</span>(2<span class="hlt">P</span>1/2) atoms by NO2, <span class="hlt">N</span>2O4, and <span class="hlt">N</span>2O have been measured using time-resolved <span class="hlt">I</span>(2<span class="hlt">P</span>1/2) --> <span class="hlt">I</span>(2<span class="hlt">P</span>3/2) 1315 nm emission. The excited atoms were generated by pulsed laser photodissociation of CF3<span class="hlt">I</span> at 248 nm. The rate constants for <span class="hlt">I</span>(2<span class="hlt">P</span>1/2) quenching by NO2 and <span class="hlt">N</span>2O were found to be independent of temperature over the range examined with average values of (2.9 +/- 0.3) x 10(-15) and (1.4 +/- 0.1) x 10(-15) cm3 s(-1), respectively. The rate constant for quenching of <span class="hlt">I</span>(2<span class="hlt">P</span>1/2) by <span class="hlt">N</span>2O4 was found to be (3.5 +/- 0.5) x 10(-13) cm3 s(-1) at ambient temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22852669','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22852669"><span>An ultra low noise telecom wavelength free running single photon <span class="hlt">detector</span> using negative feedback avalanche <span class="hlt">diode</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yan, Zhizhong; Hamel, Deny R; Heinrichs, Aimee K; Jiang, Xudong; Itzler, Mark A; Jennewein, Thomas</p> <p>2012-07-01</p> <p>It is challenging to implement genuine free running single-photon <span class="hlt">detectors</span> for the 1550 nm wavelength range with simultaneously high detection efficiency (DE), low dark noise, and good time resolution. We report a novel read out system for the signals from a negative feedback avalanche <span class="hlt">diode</span> (NFAD) [M. A. Itzler, X. Jiang, B. Nyman, and K. Slomkowski, "Quantum sensing and nanophotonic devices VI," Proc. SPIE 7222, 72221K (2009); X. Jiang, M. A. Itzler, K. ODonnell, M. Entwistle, and K. Slomkowski, "Advanced photon counting techniques V," Proc. SPIE 8033, 80330K (2011); M. A. Itzler, X. Jiang, B. M. Onat, and K. Slomkowski, "Quantum sensing and nanophotonic devices VII," Proc. SPIE 7608, 760829 (2010)], which allows useful operation of these devices at a temperature of 193 K and results in very low darkcounts (∼100 counts per second (CPS)), good time jitter (∼30 ps), and good DE (∼10%). We characterized two NFADs with a time-correlation method using photons generated from weak coherent pulses and photon pairs produced by spontaneous parametric down conversion. The inferred <span class="hlt">detector</span> efficiencies for both types of photon sources agree with each other. The best noise equivalent power of the device is estimated to be 8.1 × 10(-18) W Hz(-1/2), more than 10 times better than typical In<span class="hlt">P</span>/InGaAs single photon avalanche <span class="hlt">diodes</span> (SPADs) show in free running mode. The afterpulsing probability was found to be less than 0.1% per ns at the optimized operating point. In addition, we studied the performance of an entanglement-based quantum key distribution (QKD) using these <span class="hlt">detectors</span> and develop a model for the quantum bit error rate that incorporates the afterpulsing coefficients. We verified experimentally that using these NFADs it is feasible to implement QKD over 400 km of telecom fiber. Our NFAD photon <span class="hlt">detector</span> system is very simple, and is well suited for single-photon applications where ultra-low noise and free-running operation is required, and some afterpulsing</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AIPC.1665h0012D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AIPC.1665h0012D"><span>Capacitance and conductance-frequency characteristics of In-<span class="hlt">p</span>Si Schottky barrier <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dhimmar, J. M.; Desai, H. N.; Modi, B. P.</p> <p>2015-06-01</p> <p>The Schottky barrier height (SBH) values have been calculated by using the reverse bias capacitance-voltage (C-V) characteristics at temperature range of 120-360K. The forward bias capacitance-frequency (C-f) and conductance- frequency (G-f) measurement of In-<span class="hlt">p</span>Si SBD have been carried out from 0-1.0 V with a step up 0.05 V whereby the energy distribution of the interface state has been determined from the forward bias <span class="hlt">I</span>-V data taking the bias dependence of the effective barrier height and series resistance (RS) into account. The high value of ideality factor (<span class="hlt">n</span>=2.12) was attributing to high density of interface states and interfacial oxide layer at metal semiconductor interface. The interface state density (NSS) shows a decrease with bias from bottom of conduction band toward the mid gap. In order to examine frequency dependence NSS, RS, C-V and G(ω)/ω-f measurement of the <span class="hlt">diode</span> were performed at room temperature in the frequency range of 100Hz-100KHz. Experimental result confirmed that there is an influence in the electrical characteristic of Schottky <span class="hlt">diode</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29402030','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29402030"><span>Demonstration of enhanced continuous-wave operation of blue laser <span class="hlt">diodes</span> on a semipolar 202¯1¯ Ga<span class="hlt">N</span> substrate using indium-tin-oxide/thin-<span class="hlt">p-GaN</span> cladding layers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mehari, Shlomo; Cohen, Daniel A; Becerra, Daniel L; Nakamura, Shuji; DenBaars, Steven P</p> <p>2018-01-22</p> <p>The benefits of utilizing transparent conductive oxide on top of a thin <span class="hlt">p-GaN</span> layer for continuous-wave (CW) operation of blue laser <span class="hlt">diodes</span> (LDs) were investigated. A very low operating voltage of 5.35 V at 10 kA/cm 2 was obtained for LDs with 250 nm thick <span class="hlt">p-GaN</span> compared to 7.3 V for LDs with conventional 650 nm thick <span class="hlt">p-GaN</span>. An improved thermal performance was also observed for the thin <span class="hlt">p-GaN</span> samples resulting in a 40% increase in peak light output power and a 32% decrease in surface temperature. Finally, a tradeoff was demonstrated between low operating voltage and increased optical modal loss in the indium tin oxide (ITO) with thinner <span class="hlt">p-GaN</span>. LDs lasing at 445 nm with 150 nm thick <span class="hlt">p-GaN</span> had an excess modal loss while LDs with an optimal 250 nm thick <span class="hlt">p-GaN</span> resulted in optical output power of 1.1 W per facet without facet coatings and a wall-plug efficiency of 15%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22280300-selective-photodetector-resonant-tunneling','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22280300-selective-photodetector-resonant-tunneling"><span>Selective <span class="hlt">p-i-n</span> photodetector with resonant tunneling</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Mil'shtein, S.; Wilson, S.; Pillai, A.</p> <p>2014-05-15</p> <p>There are different fundamental approaches to designing selective photodetectors, where the selectivity of optical spectra is produced by a filtering aperture. However, manufacturing of multilayered filters is cumbersome for epitaxial technology. In the current study, we offer a novel approach in design of selective photodetectors. A <span class="hlt">p-i-n</span> photodetector with superlattices in top <span class="hlt">n</span>-layer becomes transparent for photons where hν<>E{sub ng}+E{sub <span class="hlt">n</span>1}, the light will be absorbed, simultaneously producing high energy (hot) electrons. The designed thickness of the structure does prevent thermal relaxation of high energy electrons by thus enhancing the selectivity of the photodetector. However the most important selectivity elementmore » is the resonant tunneling which does happen only for electrons occupying E{sub <span class="hlt">n</span>1} energy levels as they transfer to levels E{sub <span class="hlt">i</span>1}aligned under reverse biasing.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21263645','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21263645"><span>Improving light extraction of InGa<span class="hlt">N</span>-based light emitting <span class="hlt">diodes</span> with a roughened <span class="hlt">p-GaN</span> surface using CsCl nano-islands.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wei, Tongbo; Kong, Qingfeng; Wang, Junxi; Li, Jing; Zeng, Yiping; Wang, Guohong; Li, Jinmin; Liao, Yuanxun; Yi, Futing</p> <p>2011-01-17</p> <p>InGa<span class="hlt">N</span>-based light emitting <span class="hlt">diodes</span> (LEDs) with a top nano-roughened <span class="hlt">p-GaN</span> surface are fabricated using self-assembled CsCl nano-islands as etch masks. Following formation of hemispherical Ga<span class="hlt">N</span> nano-island arrays, electroluminescence (EL) spectra of roughened LEDs display an obvious redshift due to partial compression release in quantum wells through Inductively Coupled Plasma (ICP) etching. At a 350-mA current, the enhancement of light output power of LEDs subjected to ICP treatment with durations of 50, 150 and 250 sec compared with conventional LED have been determined to be 9.2, 70.6, and 42.3%, respectively. Additionally, the extraction enhancement factor can be further improved by increasing the size of CsCl nano-island. The economic and rapid method puts forward great potential for high performance lighting devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170011504','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170011504"><span><span class="hlt">P</span>-Compensated and <span class="hlt">P</span>-Doped Superlattice Infrared <span class="hlt">Detectors</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Khoshakhlagh, Arezou (Inventor); Ting, David Z. (Inventor); Gunapala, Sarath D. (Inventor)</p> <p>2017-01-01</p> <p>Barrier infrared <span class="hlt">detectors</span> configured to operate in the long-wave (LW) infrared regime are provided. The barrier infrared <span class="hlt">detector</span> systems may be configured as pin, pbp, barrier and double heterostructrure infrared <span class="hlt">detectors</span> incorporating optimized <span class="hlt">p</span>-doped absorbers capable of taking advantage of high mobility (electron) minority carriers. The absorber may be a <span class="hlt">p</span>-doped Ga-free InAs/InAsSb material. The <span class="hlt">p</span>-doping may be accomplished by optimizing the Be doping levels used in the absorber material. The barrier infrared <span class="hlt">detectors</span> may incorporate individual superlattice layers having narrower periodicity and optimization of Sb composition to achieve cutoff wavelengths of.about.10.mu.m.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/869528','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/869528"><span>Poly (<span class="hlt">p</span>-phenyleneneacetylene) light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Shinar, Joseph; Swanson, Leland S.; Lu, Feng; Ding, Yiwei; Barton, Thomas J.; Vardeny, Zeev V.</p> <p>1994-10-04</p> <p>Acetylene containing poly(<span class="hlt">p</span>-phenyleneacetylene) (PPA) - based light-emitting <span class="hlt">diodes</span> (LEDs) are provided. The LEDs are fabricated by coating a hole-injecting electrode, preferably an indium tin oxide (ITO) coated glass substrate, with a PPA polymer, such as a 2,5-dibutoxy or a 2,5-dihexoxy derivative of PPA, dissolved in an organic solvent. This is then followed by evaporating a layer of material capable of injecting electrons, such as Al or Al/Ca, onto the polymer to form a base electrode. This composition is then annealed to form efficient EL <span class="hlt">diodes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6885539','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/6885539"><span>Poly (<span class="hlt">p</span>-phenyleneacetylene) light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Shinar, J.; Swanson, L.S.; Lu, F.; Ding, Y.; Barton, T.J.; Vardeny, Z.V.</p> <p>1994-10-04</p> <p>Acetylene containing poly(<span class="hlt">p</span>-phenyleneacetylene) (PPA) - based light-emitting <span class="hlt">diodes</span> (LEDs) are provided. The LEDs are fabricated by coating a hole-injecting electrode, preferably an indium tin oxide (ITO) coated glass substrate, with a PPA polymer, such as a 2,5-dibutoxy or a 2,5-dihexoxy derivative of PPA, dissolved in an organic solvent. This is then followed by evaporating a layer of material capable of injecting electrons, such as Al or Al/Ca, onto the polymer to form a base electrode. This composition is then annealed to form efficient EL <span class="hlt">diodes</span>. 8 figs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1236482-vertical-gan-power-diodes-bilayer-edge-termination','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1236482-vertical-gan-power-diodes-bilayer-edge-termination"><span>Vertical Ga<span class="hlt">N</span> power <span class="hlt">diodes</span> with a bilayer edge termination</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Dickerson, Jeramy R.; Allerman, Andrew A.; Bryant, Benjamin N.; ...</p> <p>2015-12-07</p> <p>Vertical Ga<span class="hlt">N</span> power <span class="hlt">diodes</span> with a bilayer edge termination (ET) are demonstrated. The Ga<span class="hlt">N</span> <span class="hlt">p-n</span> junction is formed on a low threading dislocation defect density (10 4 - 10 5 cm -2) Ga<span class="hlt">N</span> substrate, and has a 15-μm-thick <span class="hlt">n</span>-type drift layer with a free carrier concentration of 5 × 10 15 cm -3. The ET structure is formed by <span class="hlt">N</span> implantation into the <span class="hlt">p+-GaN</span> epilayer just outside the <span class="hlt">p</span>-type contact to create compensating defects. The implant defect profile may be approximated by a bilayer structure consisting of a fully compensated layer near the surface, followed by a 90% compensated (<span class="hlt">p</span>)more » layer near the <span class="hlt">n</span>-type drift region. These devices exhibit avalanche breakdown as high as 2.6 kV at room temperature. In addition simulations show that the ET created by implantation is an effective way to laterally distribute the electric field over a large area. This increases the voltage at which impact ionization occurs and leads to the observed higher breakdown voltages.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NIMPA.893...39Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NIMPA.893...39Z"><span>High-temperature performance of gallium-nitride-based pin alpha-particle <span class="hlt">detectors</span> grown on sapphire substrates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Zhifu; Zhang, Heqiu; Liang, Hongwei; Tang, Bin; Peng, Xincun; Liu, Jianxun; Yang, Chao; Xia, Xiaochuan; Tao, Pengcheng; Shen, Rensheng; Zou, Jijun; Du, Guotong</p> <p>2018-06-01</p> <p>The temperature-dependent radiation-detection performance of an alpha-particle <span class="hlt">detector</span> that was based on a gallium-nitride (Ga<span class="hlt">N</span>)-based pin structure was studied from 290 K to 450 K. Current-voltage-temperature measurements (<span class="hlt">I</span>-V-T) of the reverse bias show the exponential dependence of leakage currents on the voltage and temperature. The current transport mechanism of the Ga<span class="hlt">N</span>-based pin <span class="hlt">diode</span> from the reverse bias <span class="hlt">I</span>-V fitting was analyzed. The temperature-dependent pulse-height spectra of the <span class="hlt">detectors</span> were studied using an 241 Am alpha-particle source at a reverse bias of 10 V, and the peak positions shifted from 534 keV at 290 K to 490 keV at 450 K. The variation of full width at half maximum (FWHM) from 282 keV at 290 K to 292 keV at 450 K is almost negligible. The Ga<span class="hlt">N</span>-based pin <span class="hlt">detectors</span> are highly promising for high-temperature environments up to 450 K.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_17 --> <div id="page_18" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="341"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JCrGr.484...86E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JCrGr.484...86E"><span>Careful stoichiometry monitoring and doping control during the tunneling interface growth of an <span class="hlt">n</span> + InAs(Si)/<span class="hlt">p</span> + GaSb(Si) Esaki <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>El Kazzi, S.; Alian, A.; Hsu, B.; Verhulst, A. S.; Walke, A.; Favia, P.; Douhard, B.; Lu, W.; del Alamo, J. A.; Collaert, N.; Merckling, C.</p> <p>2018-02-01</p> <p>In this work, we report on the growth of pseudomorphic and highly doped InAs(Si)/GaSb(Si) heterostructures on <span class="hlt">p</span>-type (0 0 1)-oriented GaSb substrate and the fabrication and characterization of <span class="hlt">n+/p</span>+ Esaki tunneling <span class="hlt">diodes</span>. We particularly study the influence of the Molecular Beam Epitaxy shutter sequences on the structural and electrical characteristics of InAs(Si)/GaSb(Si) Esaki <span class="hlt">diodes</span> structures. We use real time Reflection High Electron Diffraction analysis to monitor different interface stoichiometry at the tunneling interface. With Atomic Force Microscopy, X-ray diffraction and Transmission Electron Microscopy analyses, we demonstrate that an "InSb-like" interface leads to a sharp and defect-free interface exhibiting high quality InAs(Si) crystal growth contrary to the "GaAs-like" one. We then prove by means of Secondary Ion Mass Spectroscopy profiles that Si-diffusion at the interface allows the growth of highly Si-doped InAs/GaSb <span class="hlt">diodes</span> without any III-V material deterioration. Finally, simulations are conducted to explain our electrical results where a high Band to Band Tunneling (BTBT) peak current density of Jp = 8 mA/μm2 is achieved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4189621','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4189621"><span>Electroluminescence and Photocurrent Generation from Atomically Sharp WSe2/MoS2 Heterojunction p–<span class="hlt">n</span> <span class="hlt">Diodes</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2015-01-01</p> <p>The p–<span class="hlt">n</span> <span class="hlt">diodes</span> represent the most fundamental device building blocks for diverse optoelectronic functions, but are difficult to achieve in atomically thin transition metal dichalcogenides (TMDs) due to the challenges in selectively doping them into <span class="hlt">p</span>- or <span class="hlt">n</span>-type semiconductors. Here, we demonstrate that an atomically thin and sharp heterojunction p–<span class="hlt">n</span> <span class="hlt">diode</span> can be created by vertically stacking <span class="hlt">p</span>-type monolayer tungsten diselenide (WSe2) and <span class="hlt">n</span>-type few-layer molybdenum disulfide (MoS2). Electrical measurements of the vertically staked WSe2/MoS2 heterojunctions reveal excellent current rectification behavior with an ideality factor of 1.2. Photocurrent mapping shows rapid photoresponse over the entire overlapping region with a highest external quantum efficiency up to 12%. Electroluminescence studies show prominent band edge excitonic emission and strikingly enhanced hot-electron luminescence. A systematic investigation shows distinct layer-number dependent emission characteristics and reveals important insight about the origin of hot-electron luminescence and the nature of electron–orbital interaction in TMDs. We believe that these atomically thin heterojunction p–<span class="hlt">n</span> <span class="hlt">diodes</span> represent an interesting system for probing the fundamental electro-optical properties in TMDs and can open up a new pathway to novel optoelectronic devices such as atomically thin photodetectors, photovoltaics, as well as spin- and valley-polarized light emitting <span class="hlt">diodes</span>, on-chip lasers. PMID:25157588</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1344458-detection-modeling-leakage-current-algan-based-deep-ultraviolet-light-emitting-diodes','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1344458-detection-modeling-leakage-current-algan-based-deep-ultraviolet-light-emitting-diodes"><span>Detection and modeling of leakage current in AlGa<span class="hlt">N</span>-based deep ultraviolet light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Moseley, Michael William; Allerman, Andrew A.; Crawford, Mary H.; ...</p> <p>2015-03-01</p> <p>Current-voltage (IV) characteristics of two AlGa<span class="hlt">N</span>-based deep ultraviolet (DUV) light-emitting <span class="hlt">diodes</span> (LEDs) with differing densities of open-core threading dislocations (nanopipes) are analyzed. A three-<span class="hlt">diode</span> circuit is simulated to emulate the IV characteristics of the DUV-LEDs, but is only able to accurately model the lower leakage current, lower nanopipe density DUV-LED. It was found that current leakage through the nanopipes in these structures is rectifying, despite nanopipes being previously established as inherently <span class="hlt">n</span>-type. Using defect-sensitive etching, the nanopipes are revealed to terminate within the <span class="hlt">p</span>-type Ga<span class="hlt">N</span> capping layer of the DUV-LEDs. The circuit model is modified to account for another <span class="hlt">p</span>-nmore » junction between the <span class="hlt">n</span>-type nanopipes and the <span class="hlt">p</span>-type Ga<span class="hlt">N</span>, and an excellent fit to the IV characteristics of the leaky DUV-LED is achieved.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ApPhL..96d1110Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ApPhL..96d1110Z"><span>A route to improved extraction efficiency of light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, H.; Shan, C. X.; Wang, L. K.; Yang, Y.; Zhang, J. Y.; Yao, B.; Shen, D. Z.; Fan, X. W.</p> <p>2010-01-01</p> <p>The electroluminescence from an <span class="hlt">n-MgZnO/i-ZnO/MgO/p-GaN</span> asymmetric double heterojunction has been demonstrated. With the injection of electrons from <span class="hlt">n</span>-MgZnO and holes from <span class="hlt">p-GaN</span>, an intense ultraviolet emission coming from the ZnO active layer was observed. It is revealed that the emission intensity of the <span class="hlt">diode</span> recorded from the MgZnO side is significantly larger than that from the MgO side because of the asymmetric waveguide structure formed by the lower refractive index of MgO than that of MgZnO. The asymmetric waveguide structure reported in this letter may promise a simple and effective route to light-emitting <span class="hlt">diodes</span> with improved light-extraction efficiency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9571E..0JN','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9571E..0JN"><span>Carrier-injection studies in Ga<span class="hlt">N</span>-based light-emitting-<span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nguyen, Dinh Chuong; Vaufrey, David; Leroux, Mathieu</p> <p>2015-09-01</p> <p>Although <span class="hlt">p</span>-type Ga<span class="hlt">N</span> has been achieved by Mg doping, the low hole-mobility still remains a difficulty for Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> (LEDs). Due to the lack of field-dependent-velocity model for holes, in Ga<span class="hlt">N</span>-based LED simulations, the hole mobility is usually supposed to remain constant. However, as the <span class="hlt">p-GaN</span>-layer conductivity is lower than the <span class="hlt">n-GaN</span>-layer conductivity, a strong electric-field exists in the <span class="hlt">p</span>-side of an LED when the applied voltage exceeds the LED's built-in voltage. Under the influence of this field, the mobilities of electrons and holes are expected to decrease. Based on a field-dependent-velocity model that is usually used for narrow-bandgap materials, an LED structure is modelled with three arbitrarily chosen hole saturation-velocities. The results show that a hole saturation-velocity lower than 4x106 cm/s can negatively affect the LED's behaviors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27607696','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27607696"><span>Exciton localization and ultralow onset ultraviolet emission in ZnO nanopencils-based heterojunction <span class="hlt">diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jiang, Junyan; Zhang, Yuantao; Chi, Chen; Long, Yan; Han, Xu; Wu, Bin; Zhang, Baolin; Du, Guotong</p> <p>2016-09-05</p> <p><span class="hlt">n-GaN/i-ZnO/p-GaN</span> double heterojunction <span class="hlt">diodes</span> were constructed by vertically binding <span class="hlt">p-GaN</span> wafer on the tip of ZnO nanopencil arrays grown on <span class="hlt">n-GaN</span>/sapphire substrates. An increased quantum confinement in the tip of ZnO nanopencils has been verified by photoluminescence measurements combined with quantitative analyses. Under forward bias, a sharp ultraviolet emission at ~375 nm due to localized excitons recombination can be observed in ZnO. The electroluminescence mechanism of the studied <span class="hlt">diode</span> is tentatively elucidated using a simplified quantum confinement model. Additionally, the improved performance of the studied <span class="hlt">diode</span> featuring an ultralow emission onset, a good operation stability and an enhanced ultraviolet emission shows the potential of our approach. This work provides a new route for the design and development of ZnO-based excitonic optoelectronic devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24103966','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24103966"><span>Excitability and optical pulse generation in semiconductor lasers driven by resonant tunneling <span class="hlt">diode</span> photo-<span class="hlt">detectors</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Romeira, Bruno; Javaloyes, Julien; Ironside, Charles N; Figueiredo, José M L; Balle, Salvador; Piro, Oreste</p> <p>2013-09-09</p> <p>We demonstrate, experimentally and theoretically, excitable nanosecond optical pulses in optoelectronic integrated circuits operating at telecommunication wavelengths (1550 nm) comprising a nanoscale double barrier quantum well resonant tunneling <span class="hlt">diode</span> (RTD) photo-<span class="hlt">detector</span> driving a laser <span class="hlt">diode</span> (LD). When perturbed either electrically or optically by an input signal above a certain threshold, the optoelectronic circuit generates short electrical and optical excitable pulses mimicking the spiking behavior of biological neurons. Interestingly, the asymmetric nonlinear characteristic of the RTD-LD allows for two different regimes where one obtain either single pulses or a burst of multiple pulses. The high-speed excitable response capabilities are promising for neurally inspired information applications in photonics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22565753','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22565753"><span>Effects of overgrown <span class="hlt">p</span>-layer on the emission characteristics of the InGa<span class="hlt">N/GaN</span> quantum wells in a high-indium light-emitting <span class="hlt">diode</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Chih-Yen; Hsieh, Chieh; Liao, Che-Hao; Chung, Wei-Lun; Chen, Hao-Tsung; Cao, Wenyu; Chang, Wen-Ming; Chen, Horng-Shyang; Yao, Yu-Feng; Ting, Shao-Ying; Kiang, Yean-Woei; Yang, Chih-Chung C C; Hu, Xiaodong</p> <p>2012-05-07</p> <p>The counteraction between the increased carrier localization effect due to the change of composition nanostructure in the quantum wells (QWs), which is caused by the thermal annealing process, and the enhanced quantum-confined Stark effect in the QWs due to the increased piezoelectric field, which is caused by the increased <span class="hlt">p</span>-type layer thickness, when the <span class="hlt">p</span>-type layer is grown at a high temperature on the InGa<span class="hlt">N/GaN</span> QWs of a high-indium light-emitting <span class="hlt">diode</span> (LED) is demonstrated. Temperature- and excitation power-dependent photoluminescence (PL) measurements are performed on three groups of sample, including 1) the samples with both effects of thermal annealing and increased <span class="hlt">p</span>-type thickness, 2) those only with the similar thermal annealing process, and 3) those with increased overgrowth thickness and minimized thermal annealing effect. From the comparisons of emission wavelength, internal quantum efficiency (IQE), spectral shift with increasing PL excitation level, and calibrated activation energy of carrier localization between various samples in the three groups, one can clearly see the individual effects of thermal annealing and increased <span class="hlt">p</span>-type layer thickness. The counteraction leads to increased IQE and blue-shifted emission spectrum with increasing <span class="hlt">p</span>-type thickness when the thickness is below a certain value (20-nm <span class="hlt">p-AlGaN</span> plus 60-nm <span class="hlt">p-GaN</span> under our growth conditions). Beyond this thickness, the IQE value decreases and the emission spectrum red shifts with increasing <span class="hlt">p</span>-type thickness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT........91B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT........91B"><span>The Development of Ultraviolet Light Emitting <span class="hlt">Diodes</span> on <span class="hlt">p</span>-SiC Substrates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brummer, Gordon</p> <p></p> <p>Ultraviolet (UV) light emitting <span class="hlt">diodes</span> (LEDs) are promising light sources for purification, phototherapy, and resin curing applications. Currently, commercial UV LEDs are composed of AlGa<span class="hlt">N</span>-based <span class="hlt">n-i-p</span> junctions grown on sapphire substrates. These devices suffer from defects in the active region, inefficient <span class="hlt">p</span>-type doping, and poor light extraction efficiency. This dissertation addresses the development of a novel UV LED device structure, grown on <span class="hlt">p</span>-SiC substrates. In this device structure, the AlGa<span class="hlt">N</span>-based intrinsic (<span class="hlt">i</span>) and <span class="hlt">n</span>-layers are grown directly on the <span class="hlt">p</span>-type substrate, forming a <span class="hlt">p-i-n</span> junction. The intrinsic layer (active region) is composed of an Al<span class="hlt">N</span> buffer layer followed by three Al<span class="hlt">N</span>/Al0.30Ga0.70<span class="hlt">N</span> quantum wells. After the intrinsic layer, the <span class="hlt">n</span>-layer is formed from <span class="hlt">n</span>-type AlGa<span class="hlt">N</span>. This device architecture addresses the deficiencies of UV LEDs on sapphire substrates while providing a vertical device geometry, reduced fabrication complexity, and improved thermal management. The device layers were grown by molecular beam epitaxy (MBE). The material properties were optimized by considering varying growth conditions and by considering the role of the layer within the device. Al<span class="hlt">N</span> grown at 825 C and with a Ga surfactant yielded material with screw dislocation density of 1x10 7 cm-2 based on X-ray diffraction (XRD) analysis. AlGa<span class="hlt">N</span> alloys grown in this work contained compositional inhomogeneity, as verified by high-resolution XRD, photoluminescence, and absorption measurements. Based on Stokes shift measurements, the degree of compositional inhomogeneity was correlated with the amount of excess Ga employed during growth. Compositional inhomogeneity yields carrier localizing potential fluctuations, which are advantages in light emitting device layers. Therefore, excess Ga growth conditions were used to grow Al<span class="hlt">N</span>/Al0.30Ga0.70<span class="hlt">N</span> quantum wells (designed using a wurtzite k.<span class="hlt">p</span> model) with 35% internal quantum efficiency. Potential fluctuations limit the mobility of carriers</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..MAR.J5007L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..MAR.J5007L"><span>Effect of Dopant Activation on Device Characteristics of InGa<span class="hlt">N</span>-based Light Emitting <span class="hlt">Diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lacroce, Nicholas; Liu, Guangyu; Tan, Chee-Keong; Arif, Ronald A.; Lee, Soo Min; Tansu, Nelson</p> <p>2015-03-01</p> <p>Achieving high uniformity in growths and device characteristics of InGa<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> (LEDs) is important for large scale manufacturing. Dopant activation and maintaining control of variables affecting dopant activation are critical steps in the InGa<span class="hlt">N</span>-based light emitting <span class="hlt">diodes</span> (LEDs) fabrication process. In the epitaxy of large scale production LEDs, in-situ post-growth annealing is used for activating the Mg acceptor dopant in the <span class="hlt">p-AlGaN</span> and <span class="hlt">p-GaN</span> of the LEDs. However, the annealing temperature varies with respect to position in the reactor chamber, leading to severe uniform dopant activation issue across the devices. Thus, it is important to understand how the temperature gradient and the resulting variance in Mg acceptor activation will alter the device properties. In this work, we examine the effect of varying <span class="hlt">p</span>-type doping levels in the <span class="hlt">p-GaN</span> layers and AlGa<span class="hlt">N</span> electron blocking layer of the Ga<span class="hlt">N</span> LEDs on the optoelectronic properties including the band profile, carrier concentration, current density, output power and quantum efficiency. By understanding the variations and its effect, the identification of the most critical <span class="hlt">p</span>-type doping layer strategies to address this variation will be clarified.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17301890','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17301890"><span>Molecular <span class="hlt">diodes</span> and ultra-thin organic rectifying junctions: Au-S-CnH2<span class="hlt">n</span>-Q3CNQ and TCNQ derivatives.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ashwell, Geoffrey J; Moczko, Katarzyna; Sujka, Marta; Chwialkowska, Anna; Hermann High, L R; Sandman, Daniel J</p> <p>2007-02-28</p> <p>Attempts to obtain derivatives of the molecular <span class="hlt">diode</span>, 2-{4-[1-cyano-2-(1-(omega-acetylsulfanylalkyl)-1H-quinolin-4-ylidene)-ethylidene]-cyclohexa-2,5-dienylidene}-malonitrile [1, CH(3)CO-S-C(<span class="hlt">n</span>)H(2<span class="hlt">n</span>)-Q3CNQ], from either 2,3,5,6-tetrafluoro-7,7,8,8-tetracyano-<span class="hlt">p</span>-quinodimethane (TCNQF(4)) or 2,3,5,6-tetramethyl-7,7,8,8-tetracyano-<span class="hlt">p</span>-quinodimethane (TMTCNQ) result in ring closure via the cyano group of the pi-bridge and yield di-substituted analogues: 2-{2,3,5,6-tetrafluoro-4-[6-(10-acetylsulfanyldecyl)-3-(1-(10-acetylsulfanyldecyl)-1H-quinolin-4-ylidenemethyl)-6H-benzo[f][1,7]naphthyridin-2-ylidene]-cyclohexa-2,5-dienylidene}-malonitrile (2a) and the 2,3,5,6-tetramethyl derivative (2b). Self-assembled monolayers (SAMs) of these donor-(pi-bridge)-acceptor molecular <span class="hlt">diodes</span> exhibit asymmetric current-voltage characteristics with electron flow at forward bias from the top contact to surface C(CN)(2) groups. Comparison is made with <span class="hlt">I</span>-V curves from ultra-thin films of an organic rectifying junction in which TCNQ(-) is electron-donating and a donor-(sigma-bridge)-acceptor <span class="hlt">diode</span> in which TCNQ degrees is electron-accepting.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017OptMa..72...20S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017OptMa..72...20S"><span>Simultaneous dual-functioning InGa<span class="hlt">N/GaN</span> multiple-quantum-well <span class="hlt">diode</span> for transferrable optoelectronics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shi, Zheng; Yuan, Jialei; Zhang, Shuai; Liu, Yuhuai; Wang, Yongjin</p> <p>2017-10-01</p> <p>We propose a wafer-level procedure for the fabrication of 1.5-mm-diameter dual functioning InGa<span class="hlt">N/GaN</span> multiple-quantum-well (MQW) <span class="hlt">diodes</span> on a Ga<span class="hlt">N</span>-on-silicon platform for transferrable optoelectronics. Nitride semiconductor materials are grown on (111) silicon substrates with intermediate Al-composition step-graded buffer layers, and membrane-type MQW-<span class="hlt">diode</span> architectures are obtained by a combination of silicon removal and III-nitride film backside thinning. Suspended MQW-<span class="hlt">diodes</span> are directly transferred from silicon to foreign substrates such as metal, glass and polyethylene terephthalate by mechanically breaking the support beams. The transferred MQW-<span class="hlt">diodes</span> display strong electroluminescence under current injection and photodetection under light irradiation. Interestingly, they demonstrate a simultaneous light-emitting light-detecting function, endowing the 1.5-mm-diameter MQW-<span class="hlt">diode</span> with the capability of producing transferrable optoelectronics for adjustable displays, wearable optical sensors, multifunctional energy harvesting, flexible light communication and monolithic photonic circuit.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28818326','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28818326"><span>Dual-wavelength light-emitting <span class="hlt">diode</span>-based ultraviolet absorption <span class="hlt">detector</span> for nano-flow capillary liquid chromatography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Xie, Xiaofeng; Tolley, Luke T; Truong, Thy X; Tolley, H Dennis; Farnsworth, Paul B; Lee, Milton L</p> <p>2017-11-10</p> <p>The design of a miniaturized LED-based UV-absorption <span class="hlt">detector</span> was significantly improved for on-column nanoflow LC. The <span class="hlt">detector</span> measures approximately 27mm×24mm×10mm and weighs only 30g. Detection limits down to the nanomolar range and linearity across 3 orders of magnitude were obtained using sodium anthraquinone-2-sulfonate as a test analyte. Using two miniaturized <span class="hlt">detectors</span>, a dual-<span class="hlt">detector</span> system was assembled containing 255nm and 275nm LEDs with only 216<span class="hlt">n</span>L volume between the <span class="hlt">detectors</span> A 100μm slit was used for on-column detection with a 150μm <span class="hlt">i</span>.d. packed capillary column. Chromatographic separation of a phenol mixture was demonstrated using the dual-<span class="hlt">detector</span> system, with each <span class="hlt">detector</span> producing a unique chromatogram. Less than 6% variation in the ratios of absorbances measured at the two wavelengths for specific analytes was obtained across 3 orders of magnitude concentration, which demonstrates the potential of using absorption ratio measurements for target analyte detection. The dual-<span class="hlt">detector</span> system was used for simple, but accurate, mobile phase flow rate measurement at the exit of the column. With a flow rate range from 200 to 2000<span class="hlt">n</span>L/min, less than 3% variation was observed. Copyright © 2017 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1072839-characteristics-signals-originating-near-lithium-diffused-n+-contact-high-purity-germanium-type-point-contact-detectors','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1072839-characteristics-signals-originating-near-lithium-diffused-n+-contact-high-purity-germanium-type-point-contact-detectors"><span>Characteristics of signals originating near the lithium-diffused <span class="hlt">N</span>+ contact of high purity germanium <span class="hlt">p</span>-type point contact <span class="hlt">detectors</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Aguayo, E.; Amman, M.; Avignone, F. T.; ...</p> <p>2012-11-09</p> <p>A study of signals originating near the lithium-diffused <span class="hlt">n</span>+ contact of <span class="hlt">p</span>-type point contact (PPC) high purity germanium <span class="hlt">detectors</span> (HPGe) is presented. The transition region between the active germanium and the fully dead layer of the <span class="hlt">n</span>+ contact is examined. Energy depositions in this transition region are shown to result in partial charge collection. This provides a mechanism for events with a well defined energy to contribute to the continuum of the energy spectrum at lower energies. A novel technique to quantify the contribution from this source of background is introduced. Furthermore, experiments that operate germanium <span class="hlt">detectors</span> with a verymore » low energy threshold may benefit from the methods presented herein.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22300071-nanospherical-lens-lithographical-ag-nanodisk-arrays-embedded-gan-localized-surface-plasmon-enhanced-blue-light-emitting-diodes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22300071-nanospherical-lens-lithographical-ag-nanodisk-arrays-embedded-gan-localized-surface-plasmon-enhanced-blue-light-emitting-diodes"><span>Nanospherical-lens lithographical Ag nanodisk arrays embedded in <span class="hlt">p-GaN</span> for localized surface plasmon-enhanced blue light emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Wei, Tongbo, E-mail: tbwei@semi.ac.cn; Wu, Kui; Sun, Bo</p> <p>2014-06-15</p> <p>Large-scale Ag nanodisks (NDs) arrays fabricated using nanospherical-lens lithography (NLL) are embedded in <span class="hlt">p-GaN</span> layer of an InGa<span class="hlt">N/GaN</span> light-emitting <span class="hlt">diode</span> (LED) for generating localized surface plasmon (LSP) coupling with the radiating dipoles in the quantum-well (QWs). Based on the Ag NDs with the controlled surface coverage, LSP leads to the improved crystalline quality of regrowth <span class="hlt">p-GaN</span>, increased photoluminescence (PL) intensity, reduced PL decay time, and enhanced output power of LED. Compared with the LED without Ag NDs, the optical output power at a current of 350 mA of the LSP-enhanced LEDs with Ag NDs having a distance of 20 andmore » 35 nm to QWs is increased by 26.7% and 31.1%, respectively. The electrical characteristics and optical properties of LEDs with embedded Ag NPs are dependent on the distance of between Ag NPs and QWs region. The LED with Ag NDs array structure is also found to exhibit reduced emission divergence, compared to that without Ag NDs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010IJMPB..24.1129C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010IJMPB..24.1129C"><span>Red Light Emitting Schottky <span class="hlt">Diodes</span> on <span class="hlt">p</span>-TYPE Ga<span class="hlt">N/AlN</span>/Si(111) Substrate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chuah, L. S.; Hassan, Z.; Abu Hassan, H.</p> <p></p> <p>High quality Ga<span class="hlt">N</span> layers doped with Mg were grown on Si(111) substrates using high temperature Al<span class="hlt">N</span> as buffer layer by radio-frequency molecular beam epitaxy. From the Hall measurements, fairly uniform high hole concentration as high as (4-5) × 1020 cm-3 throughout the Ga<span class="hlt">N</span> was achieved. The fabrication of the device is very simple. Nickel ohmic contacts and Schottky contacts using indium were fabricated on Mg-doped <span class="hlt">p-GaN</span> films. The light emission has been obtained from these thin film electroluminescent devices. Thin film electroluminescent devices were operated under direct current bias. Schottky and ohmic contacts used as cathode and anode were employed in these investigations. Alternatively, two Schottky contacts could be probed as cathode and anode. Thin film electroluminescent devices were able to emit light. However, electrical and optical differences could be observed from the two different probing methods. The red light color could be observed when the potential between the electrodes was increased gradually under forward bias of 8 V at room temperature. Electrical properties of these thin film electroluminescent devices were characterized by current-voltage (<span class="hlt">I</span>-V) system, the heights of barriers determined from the <span class="hlt">I</span>-V measurements were found to be related to the electroluminescence.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JTePh..62.1787P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JTePh..62.1787P"><span>The Numerical Simulation of the Nanosecond Switching of a <span class="hlt">p</span>-SOS <span class="hlt">Diode</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Podolska, N. I.; Lyublinskiy, A. G.; Grekhov, I. V.</p> <p>2017-12-01</p> <p>Abrupt high-density reverse current interruption has been numerically simulated for switching from forward to reverse bias in a silicon <span class="hlt">p</span> + <span class="hlt">P</span> 0 <span class="hlt">n</span> + structure ( <span class="hlt">p</span>-SOS <span class="hlt">diode</span>). It has been shown that the current interruption in this structure occurs as a result of the formation of two dynamic domains of a strong electric field in regions in which the free carrier concentration substantially exceeds the concentration of the doping impurity. The first domain is formed in the <span class="hlt">n</span> + region at the <span class="hlt">n</span> + <span class="hlt">P</span> 0 junction, while the second domain is formed in the <span class="hlt">P</span> 0 region at the interface with the <span class="hlt">p</span> + layer. The second domain expands much faster, and this domain mainly determines the current interruption rate. Good agreement is achieved between the simulation results and the experimental data when the actual electric circuit determining the electron-hole plasma pumping in and out is accurately taken into account.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JEMat..46.6502M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JEMat..46.6502M"><span>Electrical Investigation of Nanostructured Fe2O3/<span class="hlt">p</span>-Si Heterojunction <span class="hlt">Diode</span> Fabricated Using the Sol-Gel Technique</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mansour, Shehab A.; Ibrahim, Mervat M.</p> <p>2017-11-01</p> <p>Iron oxide (α-Fe2O3) nanocrystals have been synthesized via the sol-gel technique. The structural and morphological features of these nanocrystals were studied using x-ray diffraction, Fourier transform-infrared spectroscopy and transmission electron microscopy. Colloidal solution of synthesized α-Fe2O3 (hematite) was spin-coated onto a single-crystal <span class="hlt">p</span>-type silicon (<span class="hlt">p</span>-Si) wafer to fabricate a heterojunction <span class="hlt">diode</span> with Mansourconfiguration Ag/Fe2O3/<span class="hlt">p</span>-Si/Al. This <span class="hlt">diode</span> was electrically characterized at room temperature using current-voltage (<span class="hlt">I</span>-V) characteristics in the voltage range from -9 V to +9 V. The fabricated <span class="hlt">diode</span> showed a good rectification behavior with a rectification factor 1.115 × 102 at 6 V. The junction parameters such as ideality factor, barrier height, series resistance and shunt resistance are determined using conventional <span class="hlt">I</span>-V characteristics. For low forward voltage, the conduction mechanism is dominated by the defect-assisted tunneling process with conventional electron-hole recombination. However, at higher voltage, <span class="hlt">I</span>-V ohmic and space charge-limited current conduction was became less effective with the contribution of the trapped-charge-limited current at the highest voltage range.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19830032707&hterms=Intrinsic+extrinsic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DIntrinsic%2Bextrinsic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19830032707&hterms=Intrinsic+extrinsic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DIntrinsic%2Bextrinsic"><span>Simple phenomenological modeling of transition-region capacitance of forward-biased <span class="hlt">p-n</span> junction <span class="hlt">diodes</span> and transistor <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lindholm, F. A.</p> <p>1982-01-01</p> <p>The derivation of a simple expression for the capacitance C(V) associated with the transition region of a <span class="hlt">p-n</span> junction under a forward bias is derived by phenomenological reasoning. The treatment of C(V) is based on the conventional Shockley equations, and simpler expressions for C(V) result that are in general accord with the previous analytical and numerical results. C(V) consists of two components resulting from changes in majority carrier concentration and from free hole and electron accumulation in the space-charge region. The space-charge region is conceived as the intrinsic region of an <span class="hlt">n-i-p</span> structure for a space-charge region markedly wider than the extrinsic Debye lengths at its edges. This region is excited in the sense that the forward bias creates hole and electron densities orders of magnitude larger than those in equilibrium. The recent Shirts-Gordon (1979) modeling of the space-charge region using a dielectric response function is contrasted with the more conventional Schottky-Shockley modeling.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10123E..08F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10123E..08F"><span>Analysis of waveguide architectures of InGa<span class="hlt">N/GaN</span> <span class="hlt">diode</span> lasers by nearfield optical microscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Friede, Sebastian; Tomm, Jens W.; Kühn, Sergei; Hoffmann, Veit; Wenzel, Hans</p> <p>2017-02-01</p> <p>Waveguide (WG) architectures of 420-nm emitting InAlGa<span class="hlt">N/GaN</span> <span class="hlt">diode</span> lasers are analyzed by photoluminescence (PL) and photocurrent (PC) spectroscopy using a nearfield scanning optical microscope (NSOM) for excitation and detection. The measurements with a spatial resolution of 100 nm are implemented by scanning the fiber tip along the unprepared front facets of standard devices. PL is collected by the fiber tip, whereas PCs are extracted from the contacts that are anyway present for power supply. The mechanisms of signal generation are addressed in detail. The components of the `optical active region', multiple quantum wells (MQW), WGs, and cladding layers are separately inspected. Even separate analysis of <span class="hlt">p</span>- and <span class="hlt">n</span>-sections of the WG become possible. Defect levels are detected in the <span class="hlt">p</span>-part of the WG. Their presence is consistent with the doping by Mg. An increased efficiency of carrier capture into InGa<span class="hlt">N/GaN</span> WGs compared to Ga<span class="hlt">N</span> WGs is observed. Thus, beyond the improved optical confinement, the electrical confinement is improved, as well. NSOM PL and PC at Ga<span class="hlt">N</span> based devices do not reach the clarity and spatial resolution for WG mode analysis as seen before for GaAs based devices. This is due to higher modal absorption and higher WG losses. NSOM based optical analysis turns out to be an efficient tool for analysis of single layers grown into InAlGa<span class="hlt">N/GaN</span> <span class="hlt">diode</span> laser structures, even if this analysis is done at a packaged ready-to-work device.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012RScI...83g3105Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012RScI...83g3105Y"><span>An ultra low noise telecom wavelength free running single photon <span class="hlt">detector</span> using negative feedback avalanche <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yan, Zhizhong; Hamel, Deny R.; Heinrichs, Aimee K.; Jiang, Xudong; Itzler, Mark A.; Jennewein, Thomas</p> <p>2012-07-01</p> <p>It is challenging to implement genuine free running single-photon <span class="hlt">detectors</span> for the 1550 nm wavelength range with simultaneously high detection efficiency (DE), low dark noise, and good time resolution. We report a novel read out system for the signals from a negative feedback avalanche <span class="hlt">diode</span> (NFAD) [M. A. Itzler, X. Jiang, B. Nyman, and K. Slomkowski, "Quantum sensing and nanophotonic devices VI," Proc. SPIE 7222, 72221K (2009), 10.1117/12.814669; X. Jiang, M. A. Itzler, K. ODonnell, M. Entwistle, and K. Slomkowski, "Advanced photon counting techniques V," Proc. SPIE 8033, 80330K (2011), 10.1117/12.883543; M. A. Itzler, X. Jiang, B. M. Onat, and K. Slomkowski, "Quantum sensing and nanophotonic devices VII," Proc. SPIE 7608, 760829 (2010), 10.1117/12.843588], which allows useful operation of these devices at a temperature of 193 K and results in very low darkcounts (˜100 counts per second (CPS)), good time jitter (˜30 ps), and good DE (˜10%). We characterized two NFADs with a time-correlation method using photons generated from weak coherent pulses and photon pairs produced by spontaneous parametric down conversion. The inferred <span class="hlt">detector</span> efficiencies for both types of photon sources agree with each other. The best noise equivalent power of the device is estimated to be 8.1 × 10-18 W Hz-1/2, more than 10 times better than typical In<span class="hlt">P</span>/InGaAs single photon avalanche <span class="hlt">diodes</span> (SPADs) show in free running mode. The afterpulsing probability was found to be less than 0.1% per ns at the optimized operating point. In addition, we studied the performance of an entanglement-based quantum key distribution (QKD) using these <span class="hlt">detectors</span> and develop a model for the quantum bit error rate that incorporates the afterpulsing coefficients. We verified experimentally that using these NFADs it is feasible to implement QKD over 400 km of telecom fiber. Our NFAD photon <span class="hlt">detector</span> system is very simple, and is well suited for single-photon applications where ultra-low noise and free</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NIMPB.422....7M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NIMPB.422....7M"><span>Experimental validation and testing of a Na<span class="hlt">I</span> boron-lined neutron <span class="hlt">detector</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Metwally, Walid A.; Emam, Amira G.</p> <p>2018-05-01</p> <p>Effective neutron detection systems are critical in various nuclear fields. Most of the current detection systems rely on He-3 <span class="hlt">detectors</span> due to their high neutron cross section. However, the limited sizes and worldwide scarcity of He-3 lead to major research efforts to find alternative neutron <span class="hlt">detectors</span>. One of the proposed cost-effective alternatives is using boron-lined Na<span class="hlt">I</span> <span class="hlt">detectors</span> to detect the gamma ray resulting from the 10B(<span class="hlt">n</span>,α)7Li reaction. The proposed <span class="hlt">detector</span> assembly has been experimentally tested and its results were compared with those from a He-3 <span class="hlt">detector</span>. In addition to detecting the gamma rays from the source and surrounding medium, the boron-lined Na<span class="hlt">I</span> <span class="hlt">detector</span> showed a good sensitivity to changes in neutron flux distributions and a higher efficiency when compared to the He-3 <span class="hlt">detector</span> used.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018OptCo.419..108X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018OptCo.419..108X"><span>Emission enhancement of light-emitting <span class="hlt">diode</span> by localized surface plasmon induced by Ag/<span class="hlt">p-GaN</span> double grating</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xie, Ruijie; Li, Zhiquan; Li, Xin; Gu, Erdan; Niu, Liyong; Sha, Xiaopeng</p> <p>2018-07-01</p> <p>In this paper, a new type of light-emitting <span class="hlt">diodes</span> (LEDs) structure is designed to enhance the light emission efficiency of Ga<span class="hlt">N</span>-based LEDs. The structure mainly includes Ag grating, ITO layer and <span class="hlt">p-GaN</span> grating. The principle of stimulating the localized surface plasmon to improve the luminous characteristics of the LED by using this structure is discussed. Based on the COMSOL software, the finite element method is used to simulate the LED structure. The normalized radiated powers, the normalized absorbed powers under different wavelength and geometric parameters, and the distribution of the electric field with the particular geometric parameters are obtained. The simulation results show that with a local ITO thickness of 32 nm, an etching depth of 29 nm, a grating period of 510 nm and a duty ratio of 0.5, the emission intensity of the designed Ga<span class="hlt">N</span>-based LED structure has increased by nearly 55 times than the ordinary LED providing a reliable foundation for the development of high-performance Ga<span class="hlt">N</span>-based LEDs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4435138','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4435138"><span>Calculation of the Electronic Parameters of an Al/DNA/<span class="hlt">p</span>-Si Schottky Barrier <span class="hlt">Diode</span> Influenced by Alpha Radiation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Al-Ta’ii, Hassan Maktuff Jaber; Amin, Yusoff Mohd; Periasamy, Vengadesh</p> <p>2015-01-01</p> <p>Many types of materials such as inorganic semiconductors have been employed as <span class="hlt">detectors</span> for nuclear radiation, the importance of which has increased significantly due to recent nuclear catastrophes. Despite the many advantages of this type of materials, the ability to measure direct cellular or biological responses to radiation might improve <span class="hlt">detector</span> sensitivity. In this context, semiconducting organic materials such as deoxyribonucleic acid or DNA have been studied in recent years. This was established by studying the varying electronic properties of DNA-metal or semiconductor junctions when exposed to radiation. In this work, we investigated the electronics of aluminium (Al)/DNA/silicon (Si) rectifying junctions using their current-voltage (<span class="hlt">I</span>-V) characteristics when exposed to alpha radiation. <span class="hlt">Diode</span> parameters such as ideality factor, barrier height and series resistance were determined for different irradiation times. The observed results show significant changes with exposure time or total dosage received. An increased deviation from ideal <span class="hlt">diode</span> conditions (7.2 to 18.0) was observed when they were bombarded with alpha particles for up to 40 min. Using the conventional technique, barrier height values were observed to generally increase after 2, 6, 10, 20 and 30 min of radiation. The same trend was seen in the values of the series resistance (0.5889–1.423 Ω for 2–8 min). These changes in the electronic properties of the DNA/Si junctions could therefore be utilized in the construction of sensitive alpha particle <span class="hlt">detectors</span>. PMID:25730484</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780003355','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780003355"><span>JAN transistor and <span class="hlt">diode</span> characterization test program, JANTX <span class="hlt">diode</span> 1<span class="hlt">N</span>5619</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Takeda, H.</p> <p>1977-01-01</p> <p>A statistical summary of electrical characterization was performed on JANTX 1<span class="hlt">N</span>5619 silicon <span class="hlt">diodes</span>. Parameters are presented with test conditions, mean, standard deviation, lowest reading, 10% point, 90% point, and highest reading.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApPhA.124..291N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApPhA.124..291N"><span>Temperature-dependent electrical characteristics and carrier transport mechanism of <span class="hlt">p</span>-Cu2ZnSnS4/<span class="hlt">n-GaN</span> heterojunctions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Niteesh Reddy, Varra; Reddy, M. Siva Pratap; Gunasekhar, K. R.; Lee, Jung-Hee</p> <p>2018-04-01</p> <p>This work explores the temperature-dependent electrical characteristics and carrier transport mechanism of Au/<span class="hlt">p</span>-Cu2ZnSnS4/<span class="hlt">n</span>-type Ga<span class="hlt">N</span> heterojunction (HJ) <span class="hlt">diodes</span> with a CZTS interlayer. The electrical characteristics were examined by current-voltage-temperature, turn-on voltage-temperature and series resistance-temperature in the high-temperature range of 300-420 K. It is observed that an exponential decrease in the series resistance ( R S) and increase in the ideality factor ( <span class="hlt">n</span>) and barrier height ( ϕ b) with increase in temperature. The thermal coefficient ( K j) is determined to be - 1.3 mV K-1 at ≥ 300 K. The effective ϕ b is determined to be 1.21 eV. This obtained barrier height is consistent with the theoretical one. The characteristic temperature ( T 0) resulting from the Cheung's functions [d V/d(ln <span class="hlt">I</span>) vs. <span class="hlt">I</span> and H( <span class="hlt">I</span>) vs. <span class="hlt">I</span>], is seen that there is good agreement between the T 0 values from both Cheung's functions. The relevant carrier transport mechanisms of Au/<span class="hlt">p-CZTS/n</span>-type Ga<span class="hlt">N</span> HJ are explained based on the thermally decreased energy band gap of <span class="hlt">n</span>-type Ga<span class="hlt">N</span> layers, thermally activated deep donors and increased further activated shallow donors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27711489','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27711489"><span>Gate-tunable <span class="hlt">diode</span>-like current rectification and ambipolar transport in multilayer van der Waals ReSe2/WS2 <span class="hlt">p-n</span> heterojunctions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Cong; Yang, Shengxue; Xiong, Wenqi; Xia, Congxin; Cai, Hui; Chen, Bin; Wang, Xiaoting; Zhang, Xinzheng; Wei, Zhongming; Tongay, Sefaattin; Li, Jingbo; Liu, Qian</p> <p>2016-10-12</p> <p>Vertically stacked van der Waals (vdW) heterojunctions of two-dimensional (2D) transition metal dichalcogenides (TMDs) have attracted a great deal of attention due to their fascinating properties. In this work, we report two important gate-tunable phenomena in new artificial vdW <span class="hlt">p-n</span> heterojunctions created by vertically stacking <span class="hlt">p</span>-type multilayer ReSe 2 and <span class="hlt">n</span>-type multilayer WS 2 : (1) well-defined strong gate-tunable <span class="hlt">diode</span>-like current rectification across the <span class="hlt">p-n</span> interface is observed, and the tunability of the electronic processes is attributed to the tunneling-assisted interlayer recombination induced by majority carriers across the vdW interface; (2) the distinct ambipolar behavior under gate voltage modulation both at forward and reverse bias voltages is found in the vdW ReSe 2 /WS 2 heterojunction transistors and a corresponding transport model is proposed for the tunable polarity behaviors. The findings may provide some new opportunities for building nanoscale electronic and optoelectronic devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApPhL.112s2107H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApPhL.112s2107H"><span>Transport properties of doped Al<span class="hlt">P</span> for the development of conductive Al<span class="hlt">P/GaP</span> distributed Bragg reflectors and their integration into light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hestroffer, Karine; Sperlich, Dennis; Dadgostar, Shabnam; Golz, Christian; Krumland, Jannis; Masselink, William Ted; Hatami, Fariba</p> <p>2018-05-01</p> <p>The transport properties of <span class="hlt">n</span>- and <span class="hlt">p</span>-doped Al<span class="hlt">P</span> layers grown by gas-source molecular beam epitaxy are investigated. <span class="hlt">n</span>- and <span class="hlt">p</span>-types of conductivities are achieved using Si and Be with peak room-temperature mobilities of 59.6 cm2/Vs and 65.0 cm2/Vs for electrons and holes, respectively. Si-doping results are then used for the design of <span class="hlt">n</span>-doped Al<span class="hlt">P/GaP</span> distributed Bragg reflectors (DBRs) with an ohmic resistance of about 7.5 ± 0.1 Ω. The DBRs are integrated as bottom mirrors in Ga<span class="hlt">P</span>-based light-emitting <span class="hlt">diodes</span> (LEDs) containing InGa<span class="hlt">P/GaP</span> quantum dots. The functionality of the LED structure and the influence of the DBRs on the InGa<span class="hlt">P/GaP</span> electroluminescence spectra are demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22420235-high-efficiency-single-ag-nanowire-gan-substrate-schottky-junction-based-ultraviolet-light-emitting-diodes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22420235-high-efficiency-single-ag-nanowire-gan-substrate-schottky-junction-based-ultraviolet-light-emitting-diodes"><span>High efficiency single Ag nanowire/<span class="hlt">p-GaN</span> substrate Schottky junction-based ultraviolet light emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Wu, Y.; Li, X.; Xu, P.</p> <p>2015-02-02</p> <p>We report a high efficiency single Ag nanowire (NW)/<span class="hlt">p-GaN</span> substrate Schottky junction-based ultraviolet light emitting <span class="hlt">diode</span> (UV-LED). The device demonstrates deep UV free exciton electroluminescence at 362.5 nm. The dominant emission, detectable at ultralow (<1 μA) forward current, does not exhibit any shifts when the forward current is increased. External quantum efficiency (EQE) as high as 0.9% is achieved at 25 μA current at room temperature. Experiments and simulation analysis show that devices fabricated with thinner Ag NWs have higher EQE. However, for very thin Ag NWs (diameter < 250 nm), this trend breaks down due to heat accumulation in the NWs. Our simple device architecturemore » offers a potentially cost-effective scheme to fabricate high efficiency Schottky junction-based UV-LEDs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1014501','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1014501"><span>Ultra-high current density thin-film Si <span class="hlt">diode</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Wang; Qi</p> <p>2008-04-22</p> <p>A combination of a thin-film .mu.c-Si and a-Si:H containing <span class="hlt">diode</span> structure characterized by an ultra-high current density that exceeds 1000 A/cm.sup.2, comprising: a substrate; a bottom metal layer disposed on the substrate; an <span class="hlt">n</span>-layer of .mu.c-Si deposited the bottom metal layer; an <span class="hlt">i</span>-layer of .mu.c-Si deposited on the <span class="hlt">n</span>-layer; a buffer layer of a-Si:H deposited on the <span class="hlt">i</span>-layer, a <span class="hlt">p</span>-layer of .mu.c-Si deposited on the buffer layer; and a top metal layer deposited on the <span class="hlt">p</span>-layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18965421','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18965421"><span>A dual-wavelength light-emitting <span class="hlt">diode</span> based <span class="hlt">detector</span> for flow-injection analysis process analysers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Huang, J; Liu, H; Tan, A; Xu, J; Zhao, X</p> <p>1992-06-01</p> <p>In this paper, a small dual-wavelength light-emitting <span class="hlt">diode</span> (LED) based <span class="hlt">detector</span> for FIA process analysers is designed. The <span class="hlt">detector</span>'s optical parts include a flow cell, a dual-wavelength LED and a photodiode. Neither mirrors nor lenses are used. The optical paths for the different light beams are almost the same, distinguishing it from previously reported LED based <span class="hlt">detectors</span>. The <span class="hlt">detector</span>'s electronic components, including a signal amplifier, an A/D and D/A converter, and an Intel 8031 single-chip microcomputer, are integrated on one small board. In order to obtain response signals of approximate intensity for the two colours, the D/A converter and a multiplexer are used to adjust the emission intensity of the two colours respectively. Under microcomputer control, light beams are rapidly electronically modulated. Therefore, dark current and intensity of the light beams are measured almost simultaneously; as a result, the effect of drift is negligible. While a solution of absorbance 0.875 was measured repeatedly, an RSD (relative standard deviation) of 0.24% could be reached. Furthermore, such a <span class="hlt">detector</span> with a red/yellow LED has been coupled with the FIA technique for the determination of 10(-6)M levels of cobalt.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1051287','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1051287"><span>Novel High Power Type-<span class="hlt">I</span> Quantum Well Cascade <span class="hlt">Diode</span> Lasers</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2017-08-30</p> <p>Novel High Power Type-<span class="hlt">I</span> Quantum Well Cascade <span class="hlt">Diode</span> Lasers The views, opinions and/or findings contained in this report are those of the author(s...SECURITY CLASSIFICATION OF: 1. REPORT DATE (DD-MM-YYYY) 4. TITLE AND SUBTITLE 13. SUPPLEMENTARY NOTES 12. DISTRIBUTION AVAILIBILITY STATEMENT 6... High Power Type-<span class="hlt">I</span> Quantum Well Cascade <span class="hlt">Diode</span> Lasers Report Term: 0-Other Email: leon.shterengas@stonybrook.edu Distribution Statement: 1-Approved</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhDT.......282G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhDT.......282G"><span>Fabrication, characterization and simulation of 4H-SiC Schottky <span class="hlt">diode</span> alpha particle <span class="hlt">detectors</span> for pyroprocessing actinide monitoring</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Garcia, Timothy Richard</p> <p></p> <p>Pyroprocessing is a method of using high-temperature molten salts and electric fields to separate and collect fuel isotopes of used nuclear fuel. It has been has been tested in the U.S. at Idaho National Laboratory as a key step in closing the nuclear fuel cycle. One technical problem with the pyroprocessing method is a lack of knowledge regarding the actinide concentrations in the salt bath during operation, since on-line techniques for measuring these concentrations are not presently available. 4H-SiC Schottky <span class="hlt">diode</span> <span class="hlt">detectors</span> can potentially fulfill this need. Such <span class="hlt">detectors</span> would operate in contact with the molten salt, and measure concentrations via alpha-particle spectroscopy. This work seeks to fabricate and characterize 4H-SiC Schottky <span class="hlt">diode</span> <span class="hlt">detectors</span> at high temperature, model the alpha particle spectrum expected in a molten salt, and model the operation of the <span class="hlt">detectors</span> to confirm the physics of operation is as expected. In this work, 4H-SiC Schottky <span class="hlt">diode</span> <span class="hlt">detectors</span> were fabricated at OSU Nanotech West. After fabrication, these <span class="hlt">detectors</span> were characterized using both <span class="hlt">I</span>-V curves and Am-241 alpha-particle energy spectra. All measurements were made as a function of temperature, from room temperature up to 500°C. The average energy required to create an electron-hole pair was observed to decrease with an increase of temperature, due to a decrease of both the 4H-SiC bandgap and non-linear energy loss terms. Furthermore, the FWHM of the spectra was observed to be dependent on the leakage current at a certain temperature, and not dependent on the temperature itself. Secondly, the alpha particle energy spectrum in the pyroprocessing environment was modeled using SRIM. The molten salt was modeled in 3 different geometries, with or without a protective cover material on top of the <span class="hlt">detector</span>. Due to the loss of alpha-particle energy in the molten salt itself, a high-energy alpha emitter may completely cover the spectrum from a lower-energy alpha emitter. Each of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26963627','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26963627"><span>Enhanced Thermionic Emission and Low 1/f Noise in Exfoliated Graphene/Ga<span class="hlt">N</span> Schottky Barrier <span class="hlt">Diode</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kumar, Ashutosh; Kashid, Ranjit; Ghosh, Arindam; Kumar, Vikram; Singh, Rajendra</p> <p>2016-03-01</p> <p>Temperature-dependent electrical transport characteristics of exfoliated graphene/Ga<span class="hlt">N</span> Schottky <span class="hlt">diodes</span> are investigated and compared with conventional Ni/Ga<span class="hlt">N</span> Schottky <span class="hlt">diodes</span>. The ideality factor of graphene/Ga<span class="hlt">N</span> and Ni/Ga<span class="hlt">N</span> <span class="hlt">diodes</span> are measured to be 1.33 and 1.51, respectively, which is suggestive of comparatively higher thermionic emission current in graphene/Ga<span class="hlt">N</span> <span class="hlt">diode</span>. The barrier height values for graphene/Ga<span class="hlt">N</span> <span class="hlt">diode</span> obtained using thermionic emission model and Richardson plots are found to be 0.60 and 0.72 eV, respectively, which are higher than predicted barrier height ∼0.40 eV as per the Schottky-Mott model. The higher barrier height is attributed to hole doping of graphene due to graphene-Au interaction which shifts the Fermi level in graphene by ∼0.3 eV. The magnitude of flicker noise of graphene/Ga<span class="hlt">N</span> Schottky <span class="hlt">diode</span> increases up to 175 K followed by its decrease at higher temperatures. This indicates that diffusion currents and barrier inhomogeneities dominate the electronic transport at lower and higher temperatures, respectively. The exfoliated graphene/Ga<span class="hlt">N</span> <span class="hlt">diode</span> is found to have lower level of barrier inhomogeneities than conventional Ni/Ga<span class="hlt">N</span> <span class="hlt">diode</span>, as well as earlier reported graphene/Ga<span class="hlt">N</span> <span class="hlt">diode</span> fabricated using chemical vapor deposited graphene. The lesser barrier inhomogeneities in graphene/Ga<span class="hlt">N</span> <span class="hlt">diode</span> results in lower flicker noise by 2 orders of magnitude as compared to Ni/Ga<span class="hlt">N</span> <span class="hlt">diode</span>. Enhanced thermionic emission current, lower level of inhomogeneities, and reduced flicker noise suggests that graphene-Ga<span class="hlt">N</span> Schottky <span class="hlt">diodes</span> may have the underlying trend for replacing metal-Ga<span class="hlt">N</span> Schottky <span class="hlt">diodes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JEMat..45.5655R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JEMat..45.5655R"><span>Temperature-Dependent Electrical Properties and Carrier Transport Mechanisms of TMAH-Treated Ni/Au/Al2O3/Ga<span class="hlt">N</span> MIS <span class="hlt">Diode</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Reddy, M. Siva Pratap; Puneetha, Peddathimula; Reddy, V. Rajagopal; Lee, Jung-Hee; Jeong, Seong-Hoon; Park, Chinho</p> <p>2016-11-01</p> <p>The temperature-dependent electrical properties and carrier transport mechanisms of tetramethylammonium hydroxide (TMAH)-treated Ni/Au/Al2O3/Ga<span class="hlt">N</span> metal-insulator-semiconductor (MIS) <span class="hlt">diodes</span> have been investigated by current-voltage ( <span class="hlt">I</span>- V) and capacitance-voltage ( C- V) measurements. The experimental results reveal that the barrier height ( <span class="hlt">I</span>- V) increases whereas the ideality factor decreases with increasing temperature. The TMAH-treated Ni/Au/Al2O3/Ga<span class="hlt">N</span> MIS <span class="hlt">diode</span> showed nonideal behaviors which indicate the presence of a nonuniform distribution of interface states ( <span class="hlt">N</span> SS) and effect of series resistance ( R S). The obtained R S and <span class="hlt">N</span> SS were found to decrease with increasing temperature. Furthermore, it was found that different transport mechanisms dominated in the TMAH-treated Ni/Au/Al2O3/Ga<span class="hlt">N</span> MIS <span class="hlt">diode</span>. At 150 K to 250 K, Poole-Frenkel emission (PFE) was found to be responsible for the reverse leakage, while Schottky emission (SE) was the dominant mechanism at high electric fields in the temperature range from 300 K to 400 K. Feasible energy band diagrams and possible carrier transport mechanisms for the TMAH-treated Ni/Au/Al2O3/Ga<span class="hlt">N</span> MIS <span class="hlt">diode</span> are discussed based on PFE and SE.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996JCrGr.164..154V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996JCrGr.164..154V"><span>III-<span class="hlt">N</span> light emitting <span class="hlt">diodes</span> fabricated using RF nitrogen gas source MBE</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Van Hove, J. M.; Carpenter, G.; Nelson, E.; Wowchak, A.; Chow, P. P.</p> <p>1996-07-01</p> <p>Homo- and heterojunction III-<span class="hlt">N</span> light emitting <span class="hlt">diodes</span> using RF atomic nitrogen plasma molecular beam epitaxy have been grown. Ga<span class="hlt">N</span> films deposited on sapphire using this growth technique exhibited an extremely sharp X-ray diffraction with a full width half maximum of 112 arc sec. <span class="hlt">p</span>-type doping of the nitride films was done with elemental Mg and resulted in as-grown <span class="hlt">p</span>-type material with resistivities as low as 2 Ω · cm. Both homo- and heterojunction LEDs showed clear rectification. Emission from the Ga<span class="hlt">N</span> homojunction deposited on <span class="hlt">n</span>-type SiC was peaked at 410 nm while the AlGaNGa<span class="hlt">N(Zn)AlGaN</span> double heterojunction LEDs emission was centered about 520 nm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SCPMA..57..887H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SCPMA..57..887H"><span>High efficiency and enhanced ESD properties of UV LEDs by inserting <span class="hlt">p-GaN/p-AlGaN</span> superlattice</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huang, Yong; Li, PeiXian; Yang, Zhuo; Hao, Yue; Wang, XiaoBo</p> <p>2014-05-01</p> <p>Significantly improved electrostatic discharge (ESD) properties of InGa<span class="hlt">N/GaN</span>-based UV light-emitting <span class="hlt">diode</span> (LED) with inserting <span class="hlt">p-GaN/p-AlGaN</span> superlattice (<span class="hlt">p</span>-SLs) layers (instead of <span class="hlt">p-AlGaN</span> single layer) between multiple quantum wells and Mg-doped Ga<span class="hlt">N</span> layer are reported. The pass yield of the LEDs increased from 73.53% to 93.81% under negative 2000 V ESD pulses. In addition, the light output power (LOP) and efficiency droop at high injection current were also improved. The mechanism of the enhanced ESD properties was then investigated. After excluding the effect of capacitance modulation, high-resolution X-ray diffraction (XRD) and atomic force microscope (AFM) measurements demonstrated that the dominant mechanism of the enhanced ESD properties is the material quality improved by <span class="hlt">p</span>-SLs, which indicated less leakage paths, rather than the current spreading improved by <span class="hlt">p</span>-SLs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhDT.......103L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhDT.......103L"><span>Design and fabrication of a novel self-powered solid-state neutron <span class="hlt">detector</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>LiCausi, Nicholas</p> <p></p> <p>There is a strong interest in intercepting special nuclear materials (SNM) at national and international borders and ports for homeland security applications. Detection of SNM such as U and Pu is often accomplished by sensing their natural or induced neutron emission. Such <span class="hlt">detector</span> systems typically use thermal neutron <span class="hlt">detectors</span> inside a plastic moderator. In order to achieve high detection efficiency gas filled <span class="hlt">detectors</span> are often used; these <span class="hlt">detectors</span> require high voltage bias for operation, which complicates the system when tens or hundreds of <span class="hlt">detectors</span> are deployed. A better type of <span class="hlt">detector</span> would be an inexpensive solid-state <span class="hlt">detector</span> that can be mass-produced like any other computer chip. Research surrounding solid-state <span class="hlt">detectors</span> has been underway since the late 1990's. A simple solid-state <span class="hlt">detector</span> employs a planar solar-cell type <span class="hlt">p-n</span> junction and a thin conversion material that converts incident thermal neutrons into detectable alpha-particles and 7Li ions. Existing work has typically used 6LiF or 10B as this conversion layer. Although a simple planar <span class="hlt">detector</span> can act as a highly portable, low cost <span class="hlt">detector</span>, it is limited to relatively low detection efficiency (˜10%). To increase the efficiency, 3D perforated <span class="hlt">p-i-n</span> silicon devices were proposed. To get high efficiency, these <span class="hlt">detectors</span> need to be biased, resulting in increased leakage current and hence <span class="hlt">detector</span> noise. In this research, a new type of <span class="hlt">detector</span> structure was proposed, designed and fabricated. Among several <span class="hlt">detector</span> structures evaluated, a honeycomb-like silicon <span class="hlt">p-n</span> structure was selected, which is filled with natural boron as the neutron converter. A silicon <span class="hlt">p+-n</span> <span class="hlt">diode</span> formed on the thin silicon wall of the honeycomb structure detects the energetic alpha-particles emitted from the boron conversion layer. The silicon detection layer is fabricated to be fully depleted with an integral step during the boron filling process. This novel feature results in a simplified fabrication process. Three</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000004525','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000004525"><span>Study of Bulk and Elementary Screw Dislocation Assisted Reverse Breakdown in Low-Voltage (<250 V) 4H-SiC <span class="hlt">p+n</span> Junction <span class="hlt">Diodes</span> - Part 1: DC Properties</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Neudeck, Philip G.; Huang, Wei; Dudley, Michael</p> <p>1999-01-01</p> <p>Given the high density (approx. 10(exp 4)/sq cm) of elementary screw dislocations (Burgers vector = lc with no hollow core) in commercial SiC wafers and epilayers, all appreciable current (greater than 1 A) SiC power devices will likely contain elementary screw dislocations for the foreseeable future. It is therefore important to ascertain the electrical impact of these defects, particularly in high-field vertical power device topologies where SiC is expected to enable large performance improvements in solid-state high-power systems. This paper compares the DC-measured reverse-breakdown characteristics of low-voltage (less than 250 V) small-area (less than 5 x 10(exp -4) sq cm) 4H-SiC <span class="hlt">p(+)n</span> <span class="hlt">diodes</span> with and without elementary screw dislocations. Compared to screw dislocation-free devices, <span class="hlt">diodes</span> containing elementary screw dislocations exhibited higher pre-breakdown reverse leakage currents, softer reverse breakdown <span class="hlt">I</span>-V knees, and highly localized microplasmic breakdown current filaments. The observed localized 4H-SiC breakdown parallels microplasmic breakdowns observed in silicon and other semiconductors, in which space-charge effects limit current conduction through the local microplasma as reverse bias is increased.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA582470','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA582470"><span>Electronic Characteristics of Rare Earth Doped Ga<span class="hlt">N</span> Schottky <span class="hlt">Diodes</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2013-03-21</p> <p>REPORT TYPE Master’s Thesis 3. DATES COVERED (From – To) 04 Sep 2011 - Mar 2013 4. TITLE AND SUBTITLE ELECTRONIC CHARACTERISTICS OF RARE EARTH ...ELECTRONIC CHARACTERISTICS OF RARE EARTH DOPED Ga<span class="hlt">N</span> SCHOTTKY <span class="hlt">DIODES</span> THESIS Aaron B. Blanning...United States. AFIT-ENP-13-M-03 Electronic Characteristics of Rare Earth Doped Ga<span class="hlt">N</span> Schottky <span class="hlt">Diodes</span> THESIS Presented to the Faculty</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9748E..19N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9748E..19N"><span>AlGaIn<span class="hlt">N</span> laser <span class="hlt">diode</span> technology for systems applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Najda, S. P.; Perlin, P.; Suski, T.; Marona, L.; Bockowski, M.; Leszczyński, M.; Wisniewski, P.; Czernecki, R.; Kucharski, R.; Targowski, G.; Watson, S.; Kelly, A. E.</p> <p>2016-02-01</p> <p>Gallium Nitride (Ga<span class="hlt">N</span>) laser <span class="hlt">diodes</span> fabricated from the AlGaIn<span class="hlt">N</span> material system is an emerging technology that allows laser <span class="hlt">diodes</span> to be fabricated over a very wide wavelength range from u.v. to the visible, and is a key enabler for the development of new system applications such as (underwater and terrestrial) telecommunications, quantum technologies, display sources and medical instrumentation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993ElL....29.1714K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993ElL....29.1714K"><span>Ultrahigh-speed phaselocked-loop type clock recovery circuit using a travelling-wave laser <span class="hlt">diode</span> amplifier as a 50 GHz phase <span class="hlt">detector</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kawanishi, S.; Takara, H.; Saruwatari, M.; Kitoh, T.</p> <p>1993-09-01</p> <p>Successful operation of a phase-locked loop is demonstrated using a traveling-wave laser-<span class="hlt">diode</span> amplifier as a 50 GHz phase <span class="hlt">detector</span>. Optical gain modulation in the laser <span class="hlt">diode</span> amplifier and an all-optical clock multiplication technique using a silica-based guided-wave optical circuit are used to achieve the extremely high-speed operation. Also discussed is the possibility of more than 100 GHz operation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007NIMPA.583...71H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007NIMPA.583...71H"><span>Low-temperature TCT characterization of heavily proton irradiated <span class="hlt">p</span>-type magnetic Czochralski silicon <span class="hlt">detectors</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Härkönen, J.; Tuovinen, E.; Luukka, P.; Kassamakov, I.; Autioniemi, M.; Tuominen, E.; Sane, P.; Pusa, P.; Räisänen, J.; Eremin, V.; Verbitskaya, E.; Li, Z.</p> <p>2007-12-01</p> <p><span class="hlt">n</span> +/<span class="hlt">p</span> -/<span class="hlt">p</span> + pad <span class="hlt">detectors</span> processed at the Microelectronics Center of Helsinki University of Technology on boron-doped <span class="hlt">p</span>-type high-resistivity magnetic Czochralski (MCz-Si) silicon substrates have been investigated by the transient current technique (TCT) measurements between 100 and 240 K. The <span class="hlt">detectors</span> were irradiated by 9 MeV protons at the Accelerator Laboratory of University of Helsinki up to 1 MeV neutron equivalent fluence of 2×10 15 <span class="hlt">n</span>/cm 2. In some of the <span class="hlt">detectors</span> the thermal donors (TD) were introduced by intentional heat treatment at 430 °C. Hole trapping time constants and full depletion voltage values were extracted from the TCT data. We observed that hole trapping times in the order of 10 ns were found in heavily (above 1×10 15 <span class="hlt">n</span> eq/cm 2) irradiated samples. These <span class="hlt">detectors</span> could be fully depleted below 500 V in the temperature range of 140-180 K.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9360E..0WK','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9360E..0WK"><span>Influence of bilayer resist processing on <span class="hlt">p-i-n</span> OLEDs: towards multicolor photolithographic structuring of organic displays</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krotkus, Simonas; Nehm, Frederik; Janneck, Robby; Kalkura, Shrujan; Zakhidov, Alex A.; Schober, Matthias; Hild, Olaf R.; Kasemann, Daniel; Hofmann, Simone; Leo, Karl; Reineke, Sebastian</p> <p>2015-03-01</p> <p>Recently, bilayer resist processing combined with development in hydrofluoroether (HFE) solvents has been shown to enable single color structuring of vacuum-deposited state-of-the-art organic light-emitting <span class="hlt">diodes</span> (OLED). In this work, we focus on further steps required to achieve multicolor structuring of <span class="hlt">p-i-n</span> OLEDs using a bilayer resist approach. We show that the green phosphorescent OLED stack is undamaged after lift-off in HFEs, which is a necessary step in order to achieve RGB pixel array structured by means of photolithography. Furthermore, we investigate the influence of both, double resist processing on red OLEDs and exposure of the devices to ambient conditions, on the basis of the electrical, optical and lifetime parameters of the devices. Additionally, water vapor transmission rates of single and bilayer system are evaluated with thin Ca film conductance test. We conclude that diffusion of propylene glycol methyl ether acetate (PGMEA) through the fluoropolymer film is the main mechanism behind OLED degradation observed after bilayer processing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8e5231H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8e5231H"><span>Improving performance of Si/CdS micro-/nanoribbon <span class="hlt">p-n</span> heterojunction light emitting <span class="hlt">diodes</span> by trenched structure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huang, Shiyuan; Wu, Yuanpeng; Ma, Xiangyang; Yang, Zongyin; Liu, Xu; Yang, Qing</p> <p>2018-05-01</p> <p>Realizing high performance silicon based light sources has been an unremitting pursuit for researchers. In this letter, we propose a simple structure to enhance electroluminescence emission and reduce the threshold of injected current of silicon/CdS micro-/nanoribbon <span class="hlt">p-n</span> heterojunction visible light emitting <span class="hlt">diodes</span>, by fabricating trenched structure on silicon substrate to mount CdS micro-/nanoribbon. A series of experiments and simulation analysis favors the rationality and validity of our mounting design. After mounting the CdS micro-/nanoribbon, the optical field confinement increases, and absorption and losses from high refractive silicon substrate are effectively reduced. Meanwhile the sharp change of silicon substrate near heterojunction also facilitates the balance between electron current and hole current, which substantially conduces to the stable amplification of electroluminescence emission in CdS micro-/nanoribbon.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22409878-variation-sub-sub-sub-sub-sub-sub-sub-sub-sup-sub-sub-sub-sub-sub-sub-sub-small-field-dosimetric-parameters-percentage-depth-dose-tissue-maximum-ratio-off-axis-ratio','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22409878-variation-sub-sub-sub-sub-sub-sub-sub-sub-sup-sub-sub-sub-sub-sub-sub-sub-small-field-dosimetric-parameters-percentage-depth-dose-tissue-maximum-ratio-off-axis-ratio"><span>Variation of k{sub Q{sub c{sub l{sub <span class="hlt">i</span>{sub <span class="hlt">n</span>,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub <span class="hlt">i</span>}{sub <span class="hlt">n</span>},f{sub m}{sub s}{sub r}}}}}}}}} for the small-field dosimetric parameters percentage depth dose, tissue-maximum ratio, and off-axis ratio</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Francescon, Paolo, E-mail: paolo.francescon@ulssvicenza.it; Satariano, Ninfa; Beddar, Sam</p> <p></p> <p>Purpose: Evaluate the ability of different dosimeters to correctly measure the dosimetric parameters percentage depth dose (PDD), tissue-maximum ratio (TMR), and off-axis ratio (OAR) in water for small fields. Methods: Monte Carlo (MC) simulations were used to estimate the variation of k{sub Q{sub c{sub l{sub <span class="hlt">i</span>{sub <span class="hlt">n</span>,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub <span class="hlt">i</span>}{sub <span class="hlt">n</span>},f{sub m}{sub s}{sub r}}}}}}}}} for several types of microdetectors as a function of depth and distance from the central axis for PDD, TMR, and OAR measurements. The variation of k{sub Q{sub c{sub l{sub <span class="hlt">i</span>{sub <span class="hlt">n</span>,Q{sub m{sub s{sub r}{sup f{sub c}{sub l}{sub <span class="hlt">i</span>}{sub <span class="hlt">n</span>},f{sub m}{sub s}{sub r}}}}}}}}}more » enables one to evaluate the ability of a <span class="hlt">detector</span> to reproduce the PDD, TMR, and OAR in water and consequently determine whether it is necessary to apply correction factors. The correctness of the simulations was verified by assessing the ratios between the PDDs and OARs of 5- and 25-mm circular collimators used with a linear accelerator measured with two different types of dosimeters (the PTW 60012 <span class="hlt">diode</span> and PTW PinPoint 31014 microchamber) and the PDDs and the OARs measured with the Exradin W1 plastic scintillator <span class="hlt">detector</span> (PSD) and comparing those ratios with the corresponding ratios predicted by the MC simulations. Results: MC simulations reproduced results with acceptable accuracy compared to the experimental results; therefore, MC simulations can be used to successfully predict the behavior of different dosimeters in small fields. The Exradin W1 PSD was the only dosimeter that reproduced the PDDs, TMRs, and OARs in water with high accuracy. With the exception of the EDGE <span class="hlt">diode</span>, the stereotactic <span class="hlt">diodes</span> reproduced the PDDs and the TMRs in water with a systematic error of less than 2% at depths of up to 25 cm; however, they produced OAR values that were significantly different from those in water, especially in the tail region (lower than 20% in some cases). The microchambers could be used for PDD</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29619312','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29619312"><span>Impact of Plasma Electron Flux on Plasma Damage-Free Sputtering of Ultrathin Tin-Doped Indium Oxide Contact Layer on <span class="hlt">p-GaN</span> for InGa<span class="hlt">N/GaN</span> Light-Emitting <span class="hlt">Diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Son, Kwang Jeong; Kim, Tae Kyoung; Cha, Yu-Jung; Oh, Seung Kyu; You, Shin-Jae; Ryou, Jae-Hyun; Kwak, Joon Seop</p> <p>2018-02-01</p> <p>The origin of plasma-induced damage on a <span class="hlt">p</span> -type wide-bandgap layer during the sputtering of tin-doped indium oxide (ITO) contact layers by using radiofrequency-superimposed direct current (DC) sputtering and its effects on the forward voltage and light output power (LOP) of light-emitting <span class="hlt">diodes</span> (LEDs) with sputtered ITO transparent conductive electrodes (TCE) is systematically studied. Changing the DC power voltage from negative to positive bias reduces the forward voltages and enhances the LOP of the LEDs. The positive DC power drastically decreases the electron flux in the plasma obtained by plasma diagnostics using a cutoff probe and a Langmuir probe, suggesting that the repulsion of plasma electrons from the <span class="hlt">p</span> -Ga<span class="hlt">N</span> surface can reduce plasma-induced damage to the <span class="hlt">p</span> -Ga<span class="hlt">N</span>. Furthermore, electron-beam irradiation on <span class="hlt">p</span> -Ga<span class="hlt">N</span> prior to ITO deposition significantly increases the forward voltages, showing that the plasma electrons play an important role in plasma-induced damage to the <span class="hlt">p</span> -Ga<span class="hlt">N</span>. The plasma electrons can increase the effective barrier height at the ITO/deep-level defect (DLD) band of <span class="hlt">p</span> -Ga<span class="hlt">N</span> by compensating DLDs, resulting in the deterioration of the forward voltage and LOP. Finally, the plasma damage-free sputtered-ITO TCE enhances the LOP of the LEDs by 20% with a low forward voltage of 2.9 V at 20 mA compared to LEDs with conventional e-beam-evaporated ITO TCE.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3695550','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3695550"><span>A Self-Synchronized Optoelectronic Oscillator based on an RTD Photo-<span class="hlt">Detector</span> and a Laser <span class="hlt">Diode</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Romeira, Bruno; Seunarine, Kris; Ironside, Charles N.; Kelly, Anthony E.; Figueiredo, José M. L.</p> <p>2013-01-01</p> <p>We propose and demonstrate a simple and stable low-phase noise optoelectronic oscillator (OEO) that uses a laser <span class="hlt">diode</span>, an optical fiber delay line and a resonant tunneling <span class="hlt">diode</span> (RTD) free-running oscillator that is monolithic integrated with a waveguide photo-<span class="hlt">detector</span>. The RTD-OEO exhibits single-side band phase noise power below −100 dBc/Hz with more than 30 dB noise suppression at 10 kHz from the center free-running frequency for fiber loop lengths around 1.2 km. The oscillator power consumption is below 0.55 W, and can be controlled either by the injected optical power or the fiber delay line. The RTD-OEO stability is achieved without using other high-speed optical/optoelectronic components and amplification. PMID:23814452</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1995PhDT........63Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1995PhDT........63Y"><span>Measurement of Effective Drift Velocities of Electrons and Holes in Shallow Multiple Quantum Well <span class="hlt">P-I</span> Modulators</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Ching-Mei</p> <p>1995-01-01</p> <p><span class="hlt">P-i-n</span> <span class="hlt">diodes</span> containing multiple quantum wells (MQWs) in the <span class="hlt">i</span>-region are the building blocks for photonic devices. When we apply electric field across these devices and illuminate it with light, photo-carriers are created in the <span class="hlt">i</span>-region. These carriers escape from the wells and drift toward the electrodes; thus photo-voltage is created. The rise- and decay-times of photo-voltages are related to the transport of carriers. In this dissertation, we present theoretical and experimental studies on carrier transport mechanisms of three shallow MQW GaAs/Al _{x}Ga_{1-x}As <span class="hlt">p-i-n</span> <span class="hlt">diodes</span> (x = 0.02, 0.04, 0.08) at various bias voltages. We start with the description of the sample structures and their package. We then present the characteristics of these samples including their transmission spectra and responsivity. We will demonstrate that the over-all high quality of these samples, including a strong exciton resonant absorption, ~100% internal quantum efficiencies and completely depleted <span class="hlt">i</span>-region at bias between +0.75 V to -5 V bias. In our theoretical studies, we first discuss the possible carrier sweep-out mechanisms and estimate the response times associated with these mechanisms. Based on our theoretical model, we conclude that only the drift times of carriers and enhanced diffusion times are important for shallow MQW <span class="hlt">p-i-n</span> <span class="hlt">diodes</span>: at high bias, the fast drift times of electrons and holes control the rise-times; at low bias, the slow drift times of holes and the enhanced diffusion times control the decay-times. We have performed picosecond time-resolved pump/probe electro-absorption measurements on these samples. We then obtained the drift times, effective drift velocities and effective mobilities of electrons and holes for these devices. We find that the carrier effective drift velocities (especially for holes) seemed insensitive to the Al concentration in the barriers (in the range of x = 2% to 8%), even though the x = 2% sample does show an overall faster response</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApPhL.112r3103L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApPhL.112r3103L"><span>Homogeneous molybdenum disulfide tunnel <span class="hlt">diode</span> formed via chemical doping</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Xiaochi; Qu, Deshun; Choi, Min Sup; Lee, Changmin; Kim, Hyoungsub; Yoo, Won Jong</p> <p>2018-04-01</p> <p>We report on a simple, controllable chemical doping method to fabricate a lateral homogeneous MoS2 tunnel <span class="hlt">diode</span>. MoS2 was doped to degenerate <span class="hlt">n</span>- (1.6 × 1013 cm-2) and <span class="hlt">p</span>-type (1.1 × 1013 cm-2) by benzyl viologen and AuCl3, respectively. The <span class="hlt">n</span>- and <span class="hlt">p</span>-doping can be patterned on the same MoS2 flake, and the high doping concentration can be maintained by Al2O3 masking together with vacuum annealing. A forward rectifying <span class="hlt">p-n</span> <span class="hlt">diode</span> and a band-to-band tunneling induced backward rectifying <span class="hlt">diode</span> were realized by modulating the doping concentration of both the <span class="hlt">n</span>- and <span class="hlt">p</span>-sides. Our approach is a universal stratagem to fabricate diverse 2D homogeneous <span class="hlt">diodes</span> with various functions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JEE....66...45M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JEE....66...45M"><span>Fabrication and Characterization of <span class="hlt">N</span>-Type Zinc Oxide/<span class="hlt">P</span>-Type Boron Doped Diamond Heterojunction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marton, Marián; Mikolášek, Miroslav; Bruncko, Jaroslav; Novotný, Ivan; Ižák, Tibor; Vojs, Marian; Kozak, Halyna; Varga, Marián; Artemenko, Anna; Kromka, Alexander</p> <p>2015-09-01</p> <p>Diamond and ZnO are very promising wide-bandgap materials for electronic, photovoltaic and sensor applications because of their excellent electrical, optical, physical and electrochemical properties and biocompatibility. In this contribution we show that the combination of these two materials opens up the potential for fabrication of bipolar heterojunctions. Semiconducting boron doped diamond (BDD) thin films were grown on Si and UV grade silica glass substrates by HFCVD method with various boron concentration in the gas mixture. Doped zinc oxide (ZnO:Al, ZnO:Ge) thin layers were deposited by <span class="hlt">diode</span> sputtering and pulsed lased deposition as the second semiconducting layer on the diamond films. The amount of dopants within the films was varied to obtain optimal semiconducting properties to form a bipolar <span class="hlt">p-n</span> junction. Finally, different ZnO/BDD heterostructures were prepared and analyzed. Raman spectroscopy, SEM, Hall constant and <span class="hlt">I</span>-V measurements were used to investigate the quality, structural and electrical properties of deposited heterostructures, respectively. <span class="hlt">I</span>-V measurements of ZnO/BDD <span class="hlt">diodes</span> show a rectifying ratio of 55 at ±4 V. We found that only very low dopant concentrations for both semiconducting materials enabled us to fabricate a functional <span class="hlt">p-n</span> junction. Obtained results are promising for fabrication of optically transparent ZnO/BDD bipolar heterojunction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990018454','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990018454"><span>Breakdown Degradation Associated with Elementary Screw Dislocations in 4H-SiC <span class="hlt">P(+)N</span> Junction Rectifiers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Neudeck, P. G.; Huang, W.; Dudley, M.</p> <p>1998-01-01</p> <p>It is well-known that SiC wafer quality deficiencies are delaying the realization of outstandingly superior 4H-SiC power electronics. While efforts to date have centered on eradicating micropipes (<span class="hlt">i</span>.e., hollow core super-screw dislocations with Burgers vector greater than 2c), 4H-SiC wafers and epilayers also contain elementary screw dislocations (<span class="hlt">i</span>.e., Burgers vector = lc with no hollow core) in densities on the order of thousands per sq cm, nearly 100-fold micropipe densities. This paper describes an initial study into the impact of elementary screw dislocations on the reverse-bias current-voltage (<span class="hlt">I</span>-V) characteristics of 4H-SiC <span class="hlt">p(+)n</span> <span class="hlt">diodes</span>. First, Synchrotron White Beam X-ray Topography (SWBXT) was employed to map the exact locations of elementary screw dislocations within small-area 4H-SiC <span class="hlt">p(+)n</span> mesa <span class="hlt">diodes</span>. Then the high-field reverse leakage and breakdown properties of these <span class="hlt">diodes</span> were subsequently characterized on a probing station outfitted with a dark box and video camera. Most devices without screw dislocations exhibited excellent characteristics, with no detectable leakage current prior to breakdown, a sharp breakdown <span class="hlt">I</span>-V knee, and no visible concentration of breakdown current. In contrast devices that contained at least one elementary screw dislocation exhibited a 5% to 35% reduction in breakdown voltage, a softer breakdown <span class="hlt">I</span>-V knee, and visible microplasmas in which highly localized breakdown current was concentrated. The locations of observed breakdown microplasmas corresponded exactly to the locations of elementary screw dislocations identified by SWBXT mapping. While not as detrimental to SiC device performance as micropipes, the undesirable breakdown characteristics of elementary screw dislocations could nevertheless adversely affect the performance and reliability of 4H-SiC power devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006SPIE.6127..216F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006SPIE.6127..216F"><span>Electrical and optical performance of InAs/GaSb superlattice LWIR <span class="hlt">detectors</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Field, M.; Sullivan, G. J.; Ikhlassi, A.; Grein, C.; Flatté, M. E.; Yang, H.; Zhong, M.; Weimer, M.</p> <p>2006-02-01</p> <p>InAs/GaSb superlattices are a promising technology for long-wave and very-long-wave infrared photodetectors. Present <span class="hlt">detectors</span> at these wavelengths are mostly built using bulk HgCdTe (MCT) alloys, where the bandgap is controlled by the mercury-cadmium ratio. In contrast, InAs/GaSb heterostructures control the bandgap by engineering the widths of the layers making up the superlattice. This approach is expected to have important advantages over MCT, notably the tighter control of bandgap uniformity across a sample and the suppression of Auger recombination. InAs/GaSb superlattices have a potential advantage in temperature of operation, uniformity and yield. To realize their inherent potential, however, superlattice materials with low defect density and improved device characteristics must be demonstrated. Here, we report on the growth and characterization of a 9.7 μm cutoff wavelength InAs/GaSb superlattice <span class="hlt">detector</span>, with a resistance-area product of R 0A = 11 Ωcm2 at 78 K, and an 8.5 μm cutoff <span class="hlt">diode</span> with a resistance-area product of R 0A = 160 Ωcm2 at 78 K. The devices are <span class="hlt">p-i-n</span> <span class="hlt">diodes</span> with a relatively thin intrinsic region of depth 0.5 μm as the active absorbing region. The measured external quantum efficiencies of 7.1% and 5.4 % at 7.9 μm are not yet large enough to challenge the incumbent MCT technology, but suggest scaling the intrinsic region could be a way forward to potentially useful <span class="hlt">detectors</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24738402','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24738402"><span>Electrical transport characterization of PEDOT:PSS/<span class="hlt">n</span>-Si Schottky <span class="hlt">diodes</span> and their applications in solar cells.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Khurelbaatar, Zagarzusem; Hyung, Jung-Hwan; Kim, Gil-Sung; Park, No-Won; Shim, Kyu-Hwan; Lee, Sang-Kwon</p> <p>2014-06-01</p> <p>We demonstrate locally contacted PEDOT:PSS Schottky <span class="hlt">diodes</span> with excellent rectifying behavior, fabricated on <span class="hlt">n</span>-type Si substrates using a spin-coating process and a reactive-ion etching process. Electrical transport characterizations of these Schottky <span class="hlt">diodes</span> were investigated by both current-voltage (<span class="hlt">I</span>-V) and capacitance-voltage (C-V) measurements. We found that these devices exhibit excellent modulation in the current with an on/off ratio of - 10(6). Schottky junction solar cells composed of PEDOT:PSS and <span class="hlt">n</span>-Si structures were also examined. From the current density-voltage (J-V) measurement of a solar cell under illumination, the short circuit current (<span class="hlt">I</span>(sc)), open circuit voltage (V(oc)), and conversion efficiency (eta) were - 19.7 mA/cm2, - 578.5 mV, and - 6.5%, respectively. The simple and low-cost fabrication process of the PEDOT:PSS/<span class="hlt">n</span>-Si Schottky junctions makes them a promising candidate for further high performance solar cell applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApPhL.108g2102O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApPhL.108g2102O"><span>Backward <span class="hlt">diodes</span> using heavily Mg-doped Ga<span class="hlt">N</span> growth by ammonia molecular-beam epitaxy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Okumura, Hironori; Martin, Denis; Malinverni, Marco; Grandjean, Nicolas</p> <p>2016-02-01</p> <p>We grew heavily Mg-doped Ga<span class="hlt">N</span> using ammonia molecular-beam epitaxy. The use of low growth temperature (740 °C) allows decreasing the incorporation of donor-like defects (<3 × 1017 cm-3) responsible for <span class="hlt">p</span>-type doping compensation. As a result, a net acceptor concentration of 7 × 1019 cm-3 was achieved, and the hole concentration measured by Hall effect was as high as 2 × 1019 cm-3 at room temperature. Using such a high Mg doping level, we fabricated Ga<span class="hlt">N</span> backward <span class="hlt">diodes</span> without polarization-assisted tunneling. The backward <span class="hlt">diodes</span> exhibited a tunneling-current density of 225 A/cm2 at a reverse bias of -1 V at room temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006SuMi...40..567H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006SuMi...40..567H"><span>New Ga<span class="hlt">N</span> Schottky barrier <span class="hlt">diode</span> employing a trench on AlGa<span class="hlt">N/GaN</span> heterostructure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ha, Min-Woo; Lee, Seung-Chul; Choi, Young-Hwan; Kim, Soo-Seong; Yun, Chong-Man; Han, Min-Koo</p> <p>2006-10-01</p> <p>A new Ga<span class="hlt">N</span> Schottky barrier <span class="hlt">diode</span> employing a trench structure, which is proposed and fabricated, successfully decreases a forward voltage drop without sacrificing any other electric characteristics. The trench is located in the middle of Schottky contact during a mesa etch. The Schottky metal of Pt/Mo/Ti/Au is e-gun evaporated on the 300 nm-deep trench as well as the surface of the proposed Ga<span class="hlt">N</span> Schottky barrier <span class="hlt">diode</span>. The trench forms the vertical Au Schottky contact and lateral Pt Schottky contact due to the evaporation sequence of Schottky metal. The forward voltage drops of the proposed <span class="hlt">diode</span> and conventional one are 0.73 V and 1.25 V respectively because the metal work function (5.15 eV) of the vertical Au Schottky contact is considerably less than that of the lateral Pt Schottky contact (5.65 eV). The proposed <span class="hlt">diode</span> exhibits the low on-resistance of 1.58 mΩ cm 2 while the conventional one exhibits 8.20 mΩ cm 2 due to the decrease of a forward voltage drop.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APExp..10a6501N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APExp..10a6501N"><span><span class="hlt">P</span>-type doping of Ga<span class="hlt">N</span>(000\\bar{1}) by magnesium ion implantation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Narita, Tetsuo; Kachi, Tetsu; Kataoka, Keita; Uesugi, Tsutomu</p> <p>2017-01-01</p> <p>Magnesium ion implantation has been performed on a Ga<span class="hlt">N</span>(000\\bar{1}) substrate, whose surface has a high thermal stability, thus allowing postimplantation annealing without the use of a protective layer. The current-voltage characteristics of <span class="hlt">p-n</span> <span class="hlt">diodes</span> fabricated on Ga<span class="hlt">N</span>(000\\bar{1}) showed distinct rectification at a turn-on voltage of about 3 V, although the leakage current varied widely among the <span class="hlt">diodes</span>. Coimplantation with magnesium and hydrogen ions effectively suppressed the leakage currents and device-to-device variations. In addition, an electroluminescence band was observed at wavelengths shorter than 450 nm for these <span class="hlt">diodes</span>. These results provide strong evidence that implanted magnesium ions create acceptors in Ga<span class="hlt">N</span>(000\\bar{1}).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820007449','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820007449"><span>Gallium phosphide high temperature <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chaffin, R. J.; Dawson, L. R.</p> <p>1981-01-01</p> <p>High temperature (300 C) <span class="hlt">diodes</span> for geothermal and other energy applications were developed. A comparison of reverse leakage currents of Si, GaAs, and Ga<span class="hlt">P</span> was made. <span class="hlt">Diodes</span> made from Ga<span class="hlt">P</span> should be usable to 500 C. A Liquid Phase Epitaxy (LPE) process for producing high quality, grown junction Ga<span class="hlt">P</span> <span class="hlt">diodes</span> is described. This process uses low vapor pressure Mg as a dopant which allows multiple boat growth in the same LPE run. These LPE wafers were cut into die and metallized to make the <span class="hlt">diodes</span>. These <span class="hlt">diodes</span> produce leakage currents below ten to the -9th power A/sq cm at 400 C while exhibiting good high temperature rectification characteristics. High temperature life test data is presented which shows exceptional stability of the V-<span class="hlt">I</span> characteristics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhD...50V5501J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhD...50V5501J"><span>Controlled carrier screening in <span class="hlt">p-n</span> NiO/Ga<span class="hlt">N</span> piezoelectric generators by an Al2O3 insertion layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Johar, Muhammad Ali; Jeong, Dae Kyung; Afifi Hassan, Mostafa; Kang, Jin-Ho; Ha, Jun-Seok; Key Lee, June; Ryu, Sang-Wan</p> <p>2017-12-01</p> <p>The performance of a piezoelectric generator (PG) depends significantly on the internal screening process inside the device. As piezoelectric charges appear on both ends of the piezoelectric crystal, internal screening starts to decrease the piezoelectric bias. Therefore, the piezoelectric energy generated by external stress is not fully utilized by external circuit, which is the most challenging aspect of high-efficiency PGs. In this work, the internal screening effect of a NiO/Ga<span class="hlt">N</span> <span class="hlt">p-n</span> PG was analyzed and controlled with an Al2O3 insertion layer. Internal screening in the <span class="hlt">p-n</span> <span class="hlt">diode</span> PG was categorized into free-carrier screening in neutral regions and junction screening due to charge drift across the junction. It was observed that junction screening could be significantly suppressed by inserting an Al2O3 layer and that effect was dominant in a leaky <span class="hlt">diode</span> PG. With this implementation, the piezoelectric bias of the NiO/Ga<span class="hlt">N</span> PG was improved by a factor of ~100 for high-leakage <span class="hlt">diodes</span> and a factor of ~1.6 for low-leakage <span class="hlt">diodes</span>. Consequently, NiO/Al2O3/Ga<span class="hlt">N</span> PGs under a stress of 5 MPa provided a piezoelectric bias of 12.1 V and a current density of 2.25 µA cm-2. The incorporation of a highly resistive Al2O3 layer between <span class="hlt">p</span>-NiO and <span class="hlt">n-GaN</span> layers in NiO/Ga<span class="hlt">N</span> heterojunctions provides an efficient means of improving the piezoelectric performance by controlling the internal screening of the piezoelectric field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JEMat..46.2379T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JEMat..46.2379T"><span>Frequency Dependent Electrical and Dielectric Properties of Au/<span class="hlt">P</span>3HT:PCBM:F4-TCNQ/<span class="hlt">n</span>-Si Schottky Barrier <span class="hlt">Diode</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Taşçıoğlu, İ.; Tüzün Özmen, Ö.; Şağban, H. M.; Yağlıoğlu, E.; Altındal, Ş.</p> <p>2017-04-01</p> <p>In this study, poly(3-hexylthiophene):[6,6]-phenyl-C61-butyric acid methyl ester: 2,3,5,6-tetrafluoro-7,7,8,8-tetracyanoquinodimethane (<span class="hlt">P</span>3HT:PCBM:F4-TCNQ) organic film was deposited on <span class="hlt">n</span>-type silicon (<span class="hlt">n</span>-Si) substrate by spin coating method. The electrical and dielectric analysis of Au/<span class="hlt">P</span>3HT:PCBM:F4-TCNQ/<span class="hlt">n</span>-Si Schottky barrier <span class="hlt">diode</span> was conducted by means of capacitance-voltage ( C- V) and conductance-voltage ( G/ ω- V) measurements in the frequency range of 10 kHz-2 MHz. The C- V- f plots exhibit fairly large frequency dispersion due to excess capacitance caused by the presence of interface states ( <span class="hlt">N</span> ss). The values of <span class="hlt">N</span> ss located in semiconductor bandgap at the organic film/semiconductor interface were calculated by Hill-Coleman method. Experimental results show that dielectric constant ( ɛ') and dielectric loss ( ɛ″) decrease with increasing frequency, whereas loss tangent (tan δ) remains nearly the same. The decrease in ɛ' and ɛ″ was interpreted by the theory of dielectric relaxation due to interfacial polarization. It is also observed that ac electrical conductivity ( σ ac) and electric modulus ( M' and M″) increase with increasing frequency.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080020434','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080020434"><span>Schottky barrier <span class="hlt">diode</span> and method thereof</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Aslam, Shahid (Inventor); Franz, David (Inventor)</p> <p>2008-01-01</p> <p>Pt/<span class="hlt">n.sup.-GaN</span> Schottky barrier <span class="hlt">diodes</span> are disclosed that are particularly suited to serve as ultra-violet sensors operating at wavelengths below 200 nm. The Pt/<span class="hlt">n.sup.-GaN</span> Schottky barrier <span class="hlt">diodes</span> have very large active areas, up to 1 cm.sup.2, which exhibit extremely low leakage current at low reverse biases. Very large area Pt/<span class="hlt">n.sup.-GaN</span> Schottky <span class="hlt">diodes</span> of sizes 0.25 cm.sup.2 and 1 cm.sup.2 have been fabricated from <span class="hlt">n.sup.-/n</span>.sup.+ Ga<span class="hlt">N</span> epitaxial layers grown by vapor phase epitaxy on single crystal c-plane sapphire, which showed leakage currents of 14 <span class="hlt">p</span>A and 2.7 <span class="hlt">n</span>A, respectively for the 0.25 cm.sup.2 and 1 cm.sup.2 <span class="hlt">diodes</span> both configured at a 0.5V reverse bias.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24922249','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24922249"><span>Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> with graphene/indium tin oxide transparent layer.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lai, Wei-Chih; Lin, Chih-Nan; Lai, Yi-Chun; Yu, Peichen; Chi, Gou Chung; Chang, Shoou-Jinn</p> <p>2014-03-10</p> <p>We have demonstrated a gallium nitride (Ga<span class="hlt">N</span>)-based green light-emitting <span class="hlt">diode</span> (LED) with graphene/indium tin oxide (ITO) transparent contact. The ohmic characteristic of the <span class="hlt">p-GaN</span> and graphene/ITO contact could be preformed by annealing at 500 °C for 5 min. The specific contact resistance of <span class="hlt">p-GaN</span>/graphene/ITO (3.72E-3 Ω·cm²) is one order less than that of <span class="hlt">p-GaN</span>/ITO. In addition, the 20-mA forward voltage of LEDs with graphene/ITO transparent (3.05 V) is 0.09 V lower than that of ITO LEDs (3.14 V). Besides, We have got an output power enhancement of 11% on LEDs with graphene/ITO transparent contact.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008SPIE.7058E..05C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008SPIE.7058E..05C"><span>On-chip very low junction temperature Ga<span class="hlt">N</span>-based light emitting <span class="hlt">diodes</span> by selective ion implantation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cheng, Yun-Wei; Chen, Hung-Hsien; Ke, Min-Yung; Chen, Cheng-Pin; Huang, JianJang</p> <p>2008-08-01</p> <p>We propose an on-wafer heat relaxation technology by selectively ion-implanted in part of the <span class="hlt">p</span>-type Ga<span class="hlt">N</span> to decrease the junction temperature in the LED structure. The Si dopant implantation energy and concentration are characterized to exhibit peak carrier density 1×1018 cm-3 at the depth of 137.6 nm after activation in nitrogen ambient at 750 °C for 30 minutes. The implantation schedule is designed to neutralize the selected region or to create a reverse <span class="hlt">p-n</span> <span class="hlt">diode</span> in the <span class="hlt">p-GaN</span> layer, which acts as the cold zone for heat dissipation. The cold zone with lower effective carrier concentration and thus higher resistance is able to divert the current path. Therefore, the electrical power consumption through the cold zone was reduced, resulting in less optical power emission from the quantum well under the cold zone. Using the <span class="hlt">diode</span> forward voltage method to extract junction temperature, when the injection current increases from 10 to 60 mA, the junction temperature of the ion-implanted LED increases from 34.3 °C to 42.3 °C, while that of the conventional one rises from 30.3 °C to 63.6 °C. At 100 mA, the output power of the ion-implanted device is 6.09 % higher than that of the conventional device. The slight increase of optical power is due to the increase of current density outside the cold zone region of the implanted device and reduced junction temperature. The result indicates that our approach improves thermal dissipation and meanwhile maintains the linearity of L-<span class="hlt">I</span> curves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22494946-physical-model-reverse-leakage-current-ga-gan-light-emitting-diodes-based-nanowires','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22494946-physical-model-reverse-leakage-current-ga-gan-light-emitting-diodes-based-nanowires"><span>A physical model for the reverse leakage current in (In,Ga)<span class="hlt">N/GaN</span> light-emitting <span class="hlt">diodes</span> based on nanowires</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Musolino, M.; Treeck, D. van, E-mail: treeck@pdi-berlin.de; Tahraoui, A.</p> <p>2016-01-28</p> <p>We investigated the origin of the high reverse leakage current in light emitting <span class="hlt">diodes</span> (LEDs) based on (In,Ga)<span class="hlt">N/GaN</span> nanowire (NW) ensembles grown by molecular beam epitaxy on Si substrates. To this end, capacitance deep level transient spectroscopy (DLTS) and temperature-dependent current-voltage (<span class="hlt">I</span>-V) measurements were performed on a fully processed NW-LED. The DLTS measurements reveal the presence of two distinct electron traps with high concentrations in the depletion region of the <span class="hlt">p-i-n</span> junction. These band gap states are located at energies of 570 ± 20 and 840 ± 30 meV below the conduction band minimum. The physical origin of these deep level states is discussed. Themore » temperature-dependent <span class="hlt">I</span>-V characteristics, acquired between 83 and 403 K, show that different conduction mechanisms cause the observed leakage current. On the basis of all these results, we developed a quantitative physical model for charge transport in the reverse bias regime. By taking into account the mutual interaction of variable range hopping and electron emission from Coulombic trap states, with the latter being described by phonon-assisted tunnelling and the Poole-Frenkel effect, we can model the experimental <span class="hlt">I</span>-V curves in the entire range of temperatures with a consistent set of parameters. Our model should be applicable to planar Ga<span class="hlt">N</span>-based LEDs as well. Furthermore, possible approaches to decrease the leakage current in NW-LEDs are proposed.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SeScT..32g5011S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SeScT..32g5011S"><span>Transistors and tunnel <span class="hlt">diodes</span> enabled by large-scale MoS2 nanosheets grown on Ga<span class="hlt">N</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>San Yip, Pak; Zou, Xinbo; Cho, Wai Ching; Wu, Kam Lam; Lau, Kei May</p> <p>2017-07-01</p> <p>We report growth, fabrication, and device results of MoS2-based transistors and <span class="hlt">diodes</span> implemented on a single 2D/3D material platform. The 2D/3D platform consists of a large-area MoS2 thin film grown on SiO2/<span class="hlt">p-GaN</span> substrates. Atomic force microscopy, scanning electron microscopy, and Raman spectroscopy were used to characterize the thickness and quality of the as-grown MoS2 film, showing that the large-area MoS2 nanosheet has a smooth surface morphology constituted by small grains. Starting from the same material, both top-gated MoS2 field effect transistors and MoS2/SiO2/<span class="hlt">p-GaN</span> heterojunction <span class="hlt">diodes</span> were fabricated. The transistors exhibited a high on/off ratio of 105, a subthreshold swing of 74 mV dec-1, field effect mobility of 0.17 cm2 V-1 s-1, and distinctive current saturation characteristics. For the heterojunction <span class="hlt">diodes</span>, current-rectifying characteristics were demonstrated with on-state current density of 29 A cm-2 and a current blocking property up to -25 V without breakdown. The reported transistors and <span class="hlt">diodes</span> enabled by the same 2D/3D material stack present promising building blocks for constructing future nanoscale electronics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24989398','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24989398"><span><span class="hlt">Detector</span> to <span class="hlt">detector</span> corrections: a comprehensive experimental study of <span class="hlt">detector</span> specific correction factors for beam output measurements for small radiotherapy beams.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Azangwe, Godfrey; Grochowska, Paulina; Georg, Dietmar; Izewska, Joanna; Hopfgartner, Johannes; Lechner, Wolfgang; Andersen, Claus E; Beierholm, Anders R; Helt-Hansen, Jakob; Mizuno, Hideyuki; Fukumura, Akifumi; Yajima, Kaori; Gouldstone, Clare; Sharpe, Peter; Meghzifene, Ahmed; Palmans, Hugo</p> <p>2014-07-01</p> <p>The aim of the present study is to provide a comprehensive set of <span class="hlt">detector</span> specific correction factors for beam output measurements for small beams, for a wide range of real time and passive <span class="hlt">detectors</span>. The <span class="hlt">detector</span> specific correction factors determined in this study may be potentially useful as a reference data set for small beam dosimetry measurements. Dose response of passive and real time <span class="hlt">detectors</span> was investigated for small field sizes shaped with a micromultileaf collimator ranging from 0.6 × 0.6 cm(2) to 4.2 × 4.2 cm(2) and the measurements were extended to larger fields of up to 10 × 10 cm(2). Measurements were performed at 5 cm depth, in a 6 MV photon beam. <span class="hlt">Detectors</span> used included alanine, thermoluminescent dosimeters (TLDs), stereotactic <span class="hlt">diode</span>, electron <span class="hlt">diode</span>, photon <span class="hlt">diode</span>, radiophotoluminescent dosimeters (RPLDs), radioluminescence <span class="hlt">detector</span> based on carbon-doped aluminium oxide (Al2O3:C), organic plastic scintillators, diamond <span class="hlt">detectors</span>, liquid filled ion chamber, and a range of small volume air filled ionization chambers (volumes ranging from 0.002 cm(3) to 0.3 cm(3)). All <span class="hlt">detector</span> measurements were corrected for volume averaging effect and compared with dose ratios determined from alanine to derive a <span class="hlt">detector</span> correction factors that account for beam perturbation related to nonwater equivalence of the <span class="hlt">detector</span> materials. For the <span class="hlt">detectors</span> used in this study, volume averaging corrections ranged from unity for the smallest <span class="hlt">detectors</span> such as the <span class="hlt">diodes</span>, 1.148 for the 0.14 cm(3) air filled ionization chamber and were as high as 1.924 for the 0.3 cm(3) ionization chamber. After applying volume averaging corrections, the <span class="hlt">detector</span> readings were consistent among themselves and with alanine measurements for several small <span class="hlt">detectors</span> but they differed for larger <span class="hlt">detectors</span>, in particular for some small ionization chambers with volumes larger than 0.1 cm(3). The results demonstrate how important it is for the appropriate corrections to be applied to give</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18778827','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18778827"><span>Separation of transition metals on a poly-iminodiacetic acid grafted polymeric resin column with post-column reaction detection utilising a paired emitter-<span class="hlt">detector</span> <span class="hlt">diode</span> system.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barron, Leon; O'Toole, Martina; Diamond, Dermot; Nesterenko, Pavel N; Paull, Brett</p> <p>2008-12-05</p> <p>The selectivity, retention and separation of transition metals on a short (2 mm x 50 mm) column packed with a poly-iminodiacetic acid functionalised polymer 10 microm resin (Dionex ProPac IMAC-10) are presented. This stationary phase, typically used for the separation of proteins, is composed of long chain poly-iminodiacetic acid groups grafted to a hydrophilic layer surrounding a 10 microm polymeric bead. Through the use of a combination of a multi-step <span class="hlt">p</span>H and picolinic acid gradient, the separation of magnesium, iron, cobalt, cadmium, zinc, lead and copper was possible, followed by post-column reaction with 4-(2-pyridylazo) resorcinol (PAR) and absorbance detection at 510 nm using a novel and inexpensive optical <span class="hlt">detector</span>, comprised of two light emitting <span class="hlt">diodes</span> with one acting as a light source and the other as a <span class="hlt">detector</span>. Column efficiency for selective transition metals was in excess of <span class="hlt">N</span>=10,000, with the baseline separation of seven metal cations in <3 min possible under optimised conditions. Detection limits of between 5 and 81 microg/L were possible based upon a 50 microL injection volume.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA625367','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA625367"><span>Effect of Defects on III-V MWIR <span class="hlt">n</span>Bn <span class="hlt">Detector</span> Performance</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2014-08-01</p> <p>SPONSORING/MONITORING AGENCY NAME(S) AND ADDRESS (ES) U.S. Army Research Office <span class="hlt">P</span>.O. Box 12211 Research Triangle Park, NC 27709-2211 infrared <span class="hlt">detectors</span> ...rather than diffusion based processes. Keywords: infrared <span class="hlt">detectors</span> , MWIR, <span class="hlt">n</span>Bn, photodiode, defects, irradiation, lattice mismatch, dark current...currents will increase noise in the <span class="hlt">detector</span> , it is important to understand the impact elevated defect concentrations will have on barrier architecture</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApPhA.122..568P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApPhA.122..568P"><span>Influence of temperature on Al/<span class="hlt">p</span>-CuInAlSe2 thin-film Schottky <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Parihar, Usha; Ray, Jaymin; Panchal, C. J.; Padha, Naresh</p> <p>2016-06-01</p> <p>Al/<span class="hlt">p</span>-CuInAlSe2 Schottky <span class="hlt">diodes</span> were fabricated using the optimized thin layers of CuInAlSe2 semiconductor. These <span class="hlt">diodes</span> were used to study their temperature-dependent current-voltage (<span class="hlt">I</span>-V) and capacitance-voltage (C-V) analysis over a wide range of 233-353 K. Based on these measurements, <span class="hlt">diode</span> parameters such as ideality factor ( η), barrier height (ϕbo) and series resistance ( R s) were determined from the downward curvature of <span class="hlt">I</span>-V characteristics using Cheung and Cheung method. The extracted parameters were found to be strongly temperature dependent; ϕbo increases, while η and R s decrease with increasing temperature. This behavior of ϕbo and η with change in temperature has been explained on the basis of barrier inhomogeneities over the MS interface by assuming a Gaussian distribution (GD) of the ϕbo at the interface. GD of barrier height (BH) was confirmed from apparent BH (ϕap) versus q/2 kT plot, and the values of the mean BH and standard deviation (σs) obtained from this plot at zero bias were found to be 1.02 and 0.14 eV, respectively. Also, a modified ln ( {J_{{s}} /T2 } ) - q2 σ_{{s}}2 /2k2 T2 versus q/ kT plot for Al/<span class="hlt">p</span>-CuInAlSe2 Schottky <span class="hlt">diodes</span> according to the GD gives ϕbo and Richardson constant ( A ** ) as 1.01 eV and 26 Acm-2 K-2, respectively. The Richardson constant value of 26 Acm-2 K-2 is very close to the theoretical value of 30 Acm-2 K-2. The discrepancy between BHs obtained from <span class="hlt">I</span>-V and C-V measurements has also been interpreted.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090011184','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090011184"><span><span class="hlt">n</span>Bn Infrared <span class="hlt">Detector</span> Containing Graded Absorption Layer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gunapala, Sarath D.; Ting, David Z.; Hill, Cory J.; Bandara, Sumith V.</p> <p>2009-01-01</p> <p>It has been proposed to modify the basic structure of an <span class="hlt">n</span>Bn infrared photodetector so that a plain electron-donor- type (<span class="hlt">n</span>-type) semiconductor contact layer would be replaced by a graded <span class="hlt">n</span>-type III V alloy semiconductor layer (<span class="hlt">i</span>.e., ternary or quarternary) with appropriate doping gradient. The abbreviation <span class="hlt">n</span>Bn refers to one aspect of the unmodified basic device structure: There is an electron-barrier ("B" ) layer between two <span class="hlt">n</span>-type ("<span class="hlt">n</span>" ) layers, as shown in the upper part of the figure. One of the <span class="hlt">n</span>-type layers is the aforementioned photon-absorption layer; the other <span class="hlt">n</span>-type layer, denoted the contact layer, collects the photocurrent. The basic unmodified device structure utilizes minority-charge-carrier conduction, such that, for reasons too complex to explain within the space available for this article, the dark current at a given temperature can be orders of magnitude lower (and, consequently, signal-to-noise ratios can be greater) than in infrared <span class="hlt">detectors</span> of other types. Thus, to obtain a given level of performance, less cooling (and, consequently, less cooling equipment and less cooling power) is needed. [In principle, one could obtain the same advantages by means of a structure that would be called <span class="hlt">p</span>Bp because it would include a barrier layer between two electron-acceptor- type (<span class="hlt">p</span>-type) layers.] The proposed modifications could make it practical to utilize <span class="hlt">n</span>Bn photodetectors in conjunction with readily available, compact thermoelectric coolers in diverse infrared- imaging applications that could include planetary exploration, industrial quality control, monitoring pollution, firefighting, law enforcement, and medical diagnosis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24387520','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24387520"><span>Application of spherical <span class="hlt">diodes</span> for megavoltage photon beams dosimetry.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barbés, Benigno; Azcona, Juan D; Burguete, Javier; Martí-Climent, Josep M</p> <p>2014-01-01</p> <p>External beam radiation therapy (EBRT) usually uses heterogeneous dose distributions in a given volume. Designing <span class="hlt">detectors</span> for quality control of these treatments is still a developing subject. The size of the <span class="hlt">detectors</span> should be small to enhance spatial resolution and ensure low perturbation of the beam. A high uniformity in angular response is also a very important feature in a <span class="hlt">detector</span>, because it has to measure radiation coming from all the directions of the space. It is also convenient that <span class="hlt">detectors</span> are inexpensive and robust, especially to perform in vivo measurements. The purpose of this work is to introduce a new <span class="hlt">detector</span> for measuring megavoltage photon beams and to assess its performance to measure relative dose in EBRT. The <span class="hlt">detector</span> studied in this work was designed as a spherical photodiode (1.8 mm in diameter). The change in response of the spherical <span class="hlt">diodes</span> is measured regarding the angle of incidence, cumulated irradiation, and instantaneous dose rate (or dose per pulse). Additionally, total scatter factors for large and small fields (between 1 × 1 cm(2) and 20 × 20 cm(2)) are evaluated and compared with the results obtained from some commercially available ionization chambers and planar <span class="hlt">diodes</span>. Additionally, the over-response to low energy scattered photons in large fields is investigated using a shielding layer. The spherical <span class="hlt">diode</span> studied in this work produces a high signal (150 <span class="hlt">n</span>C/Gy for photons of nominal energy of 15 MV and 160 for 6 MV, after 12 kGy) and its angular dependence is lower than that of planar <span class="hlt">diodes</span>: less than 5% between maximum and minimum in all directions, and 2% around one of the axis. It also has a moderated variation with accumulated dose (about 1.5%/kGy for 15 MV photons and 0.7%/kGy for 6 MV, after 12 kGy) and a low variation with dose per pulse (± 0.4%), and its behavior is similar to commercial <span class="hlt">diodes</span> in total scatter factor measurements. The measurements of relative dose using the spherical <span class="hlt">diode</span> described in this</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18371823','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18371823"><span>Quantification of residual nitrite and nitrate in ham by reverse-phase high performance liquid chromatography/<span class="hlt">diode</span> array <span class="hlt">detector</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ferreira, I M P L V O; Silva, S</p> <p>2008-02-15</p> <p>Nitrite and nitrate are used as additives in ham industry to provide colour, taste and protect against clostridia. The classical colorimetric methods widely used to determine nitrite and nitrate are laborious, suffer from matrix interferences and involve the use of toxic cadmium. The use of chromatography is potentially attractive since it is more rapid, sensitive, selective and provides reliable and accurate results. A rapid and cost-effective RP-HPLC method with <span class="hlt">diode</span> array <span class="hlt">detector</span> was optimized and validated for quantification of nitrites and nitrates in ham. The chromatographic separation was achieved using a HyPurity C18, 5 microm chromatographic column and gradient elution with 0.01 M <span class="hlt">n</span>-octylamine and 5mM tetrabutylammonium hydrogenosulphate to <span class="hlt">p</span>H 6.5. The determinations were performed in the linear range of 0.0125-10.0mg/L for nitrite and 0.0300-12.5 g/L for nitrate. The detection limits were 0.019 and 0.050 mg/kg, respectively. The reliability of the method in terms of precision and accuracy was evaluated. Coefficients of variation lower than 2.89% and 5.47% were obtained for nitrite and nitrate, respectively (<span class="hlt">n</span>=6). Recoveries of residual nitrite/nitrate ranged between 93.6% and 104.3%. Analysis of cooked and dried ham samples was performed, and the results obtained were in agreement with reference procedures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AIPC.1250..117G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AIPC.1250..117G"><span>The Influence of Geometrical Structure of AlInGa<span class="hlt">N</span> Double Quantum Well (DQWs) UV <span class="hlt">Diode</span> Laser on Its Performance and Operating Parameters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ghazai, A. J.; Thahab, S. M.; Hassan, H. Abu; Hassan, Z.</p> <p>2010-07-01</p> <p>The development of efficient MQWs active regions of quaternary InAlGa<span class="hlt">N</span> in the ultraviolet (UV) region is an engaging challenge by itself. Demonstrating lasers at such low wavelength will require resolving a number of materials, growth and device design issues. However, the quaternary AlInGa<span class="hlt">N</span> represents a more versatile material since the bandgap and lattice constant can be independently varied. We report a quaternary AlInGa<span class="hlt">N</span> double-quantum wells (DQWs) UV laser <span class="hlt">diode</span> (LDs) study by using the simulation program of Integrated System Engineering-Technical Computer Aided Design (ISE TCAD). Advanced physical models of semiconductor properties were used. In this paper, the enhancement in the performance of AlInGa<span class="hlt">N</span> laser <span class="hlt">diode</span> can be achieved by optimizing the laser structure geometry design. The AlInGa<span class="hlt">N</span> laser <span class="hlt">diodes</span> operating parameters such as internal quantum efficiency η<span class="hlt">i</span>, internal loss α<span class="hlt">i</span> and transparency threshold current density show effective improvements that contribute to a better performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA577381','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA577381"><span>Magneto-Transpots in Interband Resonant Tunneling <span class="hlt">Diodes</span> (<span class="hlt">I</span>-RTDs) and Dilute Magnetic Semiconductor (DMS) <span class="hlt">I</span>-RTDs</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2011-03-02</p> <p>Woolard, "Far- infrared and Terahertz lasing based upon resonant and interband tunneling in InAs/GaSb heterostructure," Applied Physics Letter, vol. 98...REPORT FINAL REPORT: Magneto-Transpots in interband Resonant Tunneling <span class="hlt">Diodes</span> (<span class="hlt">I</span>-RTDs) and Dilute Magnetic Semiconductor (DMS) <span class="hlt">I</span>-RTDs 14. ABSTRACT 16...<span class="hlt">diodes</span> (RTDs). This DB-BG-RTD device will utilizes two distinct innovations. First, ultra-fast heavy-hole (HH) interband tunneling is leveraged to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26852753','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26852753"><span>Enhancing UV-emissions through optical and electronic dual-function tuning of Ag nanoparticles hybridized with <span class="hlt">n</span>-ZnO nanorods/<span class="hlt">p-GaN</span> heterojunction light-emitting <span class="hlt">diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yao, Yung-Chi; Yang, Zu-Po; Hwang, Jung-Min; Chuang, Yi-Lun; Lin, Chia-Ching; Haung, Jing-Yu; Chou, Chun-Yang; Sheu, Jinn-Kong; Tsai, Meng-Tsan; Lee, Ya-Ju</p> <p>2016-02-28</p> <p>ZnO nanorods (NRs) and Ag nanoparticles (NPs) are known to enhance the luminescence of light-emitting <span class="hlt">diodes</span> (LEDs) through the high directionality of waveguide mode transmission and efficient energy transfer of localized surface plasmon (LSP) resonances, respectively. In this work, we have demonstrated Ag NP-incorporated <span class="hlt">n</span>-ZnO NRs/<span class="hlt">p-GaN</span> heterojunctions by facilely hydrothermally growing ZnO NRs on Ag NP-covered Ga<span class="hlt">N</span>, in which the Ag NPs were introduced and randomly distributed on the <span class="hlt">p-GaN</span> surface to excite the LSP resonances. Compared with the reference LED, the light-output power of the near-band-edge (NBE) emission (ZnO, λ = 380 nm) of our hybridized structure is increased almost 1.5-2 times and can be further modified in a controlled manner by varying the surface morphology of the surrounding medium of the Ag NPs. The improved light-output power is mainly attributed to the LSP resonance between the NBE emission of ZnO NRs and LSPs in Ag NPs. We also observed different behaviors in the electroluminescence (EL) spectra as the injection current increases for the treatment and reference LEDs. This observation might be attributed to the modification of the energy band diagram for introducing Ag NPs at the interface between <span class="hlt">n</span>-ZnO NRs and <span class="hlt">p-GaN</span>. Our results pave the way for developing advanced nanostructured LED devices with high luminescence efficiency in the UV emission regime.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4566124','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4566124"><span>Chemical Visualization of a Ga<span class="hlt">N</span> <span class="hlt">p-n</span> junction by XPS</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Caliskan, Deniz; Sezen, Hikmet; Ozbay, Ekmel; Suzer, Sefik</p> <p>2015-01-01</p> <p>We report on an operando XPS investigation of a Ga<span class="hlt">N</span> <span class="hlt">diode</span>, by recording the Ga2<span class="hlt">p</span>3/2 peak position under both forward and reverse bias. Areal maps of the peak positions under reverse bias are completely decoupled with respect to doped regions and allow a novel chemical visualization of the <span class="hlt">p-n</span> junction in a 2-D fashion. Other electrical properties of the device, such as leakage current, resistivity of the domains are also tapped via recording line-scan spectra. Application of a triangular voltage excitation enables probing photoresponse of the device. PMID:26359762</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1174635','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1174635"><span>Broadband visible light source based on AllnGa<span class="hlt">N</span> light emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Crawford, Mary H.; Nelson, Jeffrey S.</p> <p>2003-12-16</p> <p>A visible light source device is described based on a light emitting <span class="hlt">diode</span> and a nanocluster-based film. The light emitting <span class="hlt">diode</span> utilizes a semiconductor quantum well structure between <span class="hlt">n</span>-type and <span class="hlt">p</span>-type semiconductor materials on the top surface a substrate such as sapphire. The nanocluster-based film is deposited on the bottom surface of the substrate and can be derived from a solution of MoS.sub.2, MoSe.sub.2, WS.sub.2, and WSe.sub.2 particles of size greater than approximately 2 nm in diameter and less than approximately 15 nm in diameter, having an absorption wavelength greater than approximately 300 nm and less than approximately 650 nm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4507708','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4507708"><span>Amorphous Silicon <span class="hlt">p-i-n</span> Structure Acting as Light and Temperature Sensor</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>de Cesare, Giampiero; Nascetti, Augusto; Caputo, Domenico</p> <p>2015-01-01</p> <p>In this work, we propose a multi-parametric sensor able to measure both temperature and radiation intensity, suitable to increase the level of integration and miniaturization in Lab-on-Chip applications. The device is based on amorphous silicon <span class="hlt">p-doped/intrinsic/n</span>-doped thin film junction. The device is first characterized as radiation and temperature sensor independently. We found a maximum value of responsivity equal to 350 mA/W at 510 nm and temperature sensitivity equal to 3.2 mV/K. We then investigated the effects of the temperature variation on light intensity measurement and of the light intensity variation on the accuracy of the temperature measurement. We found that the temperature variation induces an error lower than 0.55 <span class="hlt">p</span>W/K in the light intensity measurement at 550 nm when the <span class="hlt">diode</span> is biased in short circuit condition, while an error below 1 K/µW results in the temperature measurement when a forward bias current higher than 25 µA/cm2 is applied. PMID:26016913</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22283090-selective-epitaxial-growth-monolithically-integrated-gan-based-light-emitting-diodes-algan-gan-driving-transistors','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22283090-selective-epitaxial-growth-monolithically-integrated-gan-based-light-emitting-diodes-algan-gan-driving-transistors"><span>Selective epitaxial growth of monolithically integrated Ga<span class="hlt">N</span>-based light emitting <span class="hlt">diodes</span> with AlGa<span class="hlt">N/GaN</span> driving transistors</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Liu, Zhaojun; Ma, Jun; Huang, Tongde</p> <p>2014-03-03</p> <p>In this Letter, we report selective epitaxial growth of monolithically integrated Ga<span class="hlt">N</span>-based light emitting <span class="hlt">diodes</span> (LEDs) with AlGa<span class="hlt">N/GaN</span> high-electron-mobility transistor (HEMT) drivers. A comparison of two integration schemes, selective epitaxial removal (SER), and selective epitaxial growth (SEG) was made. We found the SER resulted in serious degradation of the underlying LEDs in a HEMT-on-LED structure due to damage of the <span class="hlt">p-GaN</span> surface. The problem was circumvented using the SEG that avoided plasma etching and minimized device degradation. The integrated HEMT-LEDs by SEG exhibited comparable characteristics as unintegrated devices and emitted modulated blue light by gate biasing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22606224-development-application-inasp-inp-quantum-well-infrared-detector','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22606224-development-application-inasp-inp-quantum-well-infrared-detector"><span>Development and application of InAs<span class="hlt">P/InP</span> quantum well infrared <span class="hlt">detector</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Geetanjali,, E-mail: geetanjali@rrcat.gov.in; Porwal, S.; Kumar, R.</p> <p>2016-05-23</p> <p>InAs{sub x}<span class="hlt">P</span>{sub 1-x}/In<span class="hlt">P</span> quantum wells grown using metal organic vapor phase epitaxy are investigated for infrared <span class="hlt">detector</span> applications. The structural parameters of the QWs are evaluated from high resolution x-ray diffraction. The electronic transition energies measured from surface photo voltage and photoconductivity confirms that these QWs can be used for fabricating IR <span class="hlt">detectors</span> in the wide wavelength range, <span class="hlt">i</span>.e. 0.9–1.46 µm by inter-band transitions and 7–18 µm by inter-sub-band transitions. Subsequently the functionality of one such fabricated InAs{sub x}<span class="hlt">P</span>{sub 1-x}/InPQW <span class="hlt">detector</span> is verified by measuring the photoluminescence of suitable semiconductor quantum well structure. At the request of all authors of the paper,more » and with the agreement of the Proceedings Editor, an updated version of this article was published on 24 June 2016. The original version supplied to AIP Publishing contained an error in the Figures 1 and 2 where the right side of the images were cutoff. The error has been corrected in the updated and re-published article.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_21 --> <div id="page_22" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="421"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26726365','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26726365"><span>Highly Reflective Nonalloyed Ni/Ag/Pt Contact to Mg-Si Codoped <span class="hlt">p-GaN</span> for Enhanced Efficiency of Light-Emitting <span class="hlt">Diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Oh, Munsik; Kim, Hyunsoo</p> <p>2015-10-01</p> <p>The authors report enhanced efficiency of Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> (LEDs) fabricated with highly reflective nonalloyed Ni/Ag/Pt contact. The Ni/Ag/Pt contact formed on the Mg-Si codoped <span class="hlt">p-GaN</span> produced the low specific contact resistance of 7.9 x 10(-4) Ωcm2 under as-deposited condition, which is comparable to the reference reflector (annealed at 500 °C for 1 min in oxygen ambient). Current-voltage-temperature measurements and the secondary ion mass spectroscopy revealed that the ohmic mechanism of the nonalloyed Ni/Ag/Pt contact is due to the more generated deep-level states associated with Mg-Si codoping, which act as the efficient hopping centers for the carrier transport at the contact/<span class="hlt">p-GaN</span> interface. Due to the absence of interfacial reaction, the nonalloyed Ni/Ag/Pt contact showed much higher optical reflectivity (93.4% at 450 nm) as compared to the annealed sample (57.7%), resulting in a 40.5% brighter light output power as compared to the reference LEDs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004JPCM...16R.961P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004JPCM...16R.961P"><span>TOPICAL REVIEW: Ga<span class="hlt">N</span>-based <span class="hlt">diodes</span> and transistors for chemical, gas, biological and pressure sensing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pearton, S. J.; Kang, B. S.; Kim, Suku; Ren, F.; Gila, B. P.; Abernathy, C. R.; Lin, Jenshan; Chu, S. N. G.</p> <p>2004-07-01</p> <p>There is renewed emphasis on development of robust solid-state sensors capable of uncooled operation in harsh environments. The sensors should be capable of detecting chemical, gas, biological or radiation releases as well as sending signals to central monitoring locations. We discuss the advances in use of Ga<span class="hlt">N</span>-based solid-state sensors for these applications. AlGa<span class="hlt">N/GaN</span> high electron mobility transistors (HEMTs) show a strong dependence of source/drain current on the piezoelectric polarization-induced two-dimensional electron gas (2DEG). Furthermore, spontaneous and piezoelectric polarization-induced surface and interface charges can be used to develop very sensitive but robust sensors to detect gases, polar liquids and mechanical pressure. AlGa<span class="hlt">N/GaN</span> HEMT structures have been demonstrated to exhibit large changes in source-drain current upon exposing the gate region to various block co-polymer solutions. Pt-gated Ga<span class="hlt">N</span> Schottky <span class="hlt">diodes</span> and Sc2O3/AlGa<span class="hlt">N/GaN</span> metal-oxide semiconductor <span class="hlt">diodes</span> also show large change in forward currents upon exposure to H2. Of particular interest is detection of ethylene (C2H4), which has strong double bonds and hence is difficult to dissociate at modest temperatures. Apart from combustion gas sensing, the AlGa<span class="hlt">N/GaN</span> heterostructure devices can be used as sensitive <span class="hlt">detectors</span> of pressure changes. In addition, large changes in source-drain current of the AlGa<span class="hlt">N/GaN</span> HEMT sensors can be detected upon adsorption of biological species on the semiconductor surface. Finally, the nitrides provide an ideal platform for fabrication of surface acoustic wave (SAW) devices. The Ga<span class="hlt">N</span>-based devices thus appear promising for a wide range of chemical, biological, combustion gas, polar liquid, strain and high temperature pressure-sensing applications. In addition, the sensors are compatible with high bit-rate wireless communication systems that facilitate their use in remote arrays.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27628345','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27628345"><span>Green high-power tunable external-cavity Ga<span class="hlt">N</span> <span class="hlt">diode</span> laser at 515  nm.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chi, Mingjun; Jensen, Ole Bjarlin; Petersen, Paul Michael</p> <p>2016-09-15</p> <p>A 480 mW green tunable <span class="hlt">diode</span> laser system is demonstrated for the first time to our knowledge. The laser system is based on a Ga<span class="hlt">N</span> broad-area <span class="hlt">diode</span> laser and Littrow external-cavity feedback. The green laser system is operated in two modes by switching the polarization direction of the laser beam incident on the grating. When the laser beam is <span class="hlt">p</span>-polarized, an output power of 50 mW with a tunable range of 9.2 nm is achieved. When the laser beam is s-polarized, an output power of 480 mW with a tunable range of 2.1 nm is obtained. This constitutes the highest output power from a tunable green <span class="hlt">diode</span> laser system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22852367','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22852367"><span>Failure analysis of InGa<span class="hlt">N/GaN</span> high power light-emitting <span class="hlt">diodes</span> fabricated with ITO transparent <span class="hlt">p</span>-type electrode during accelerated electro-thermal stress.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Moon, Seong Min; Kim, Y D; Oh, S K; Park, M J; Kwak, Joon Seop</p> <p>2012-05-01</p> <p>We have investigated the high-temperature degradation of optical power as well as electrical properties of InGa<span class="hlt">N/GaN</span> light-emitting <span class="hlt">diodes</span> (LEDs) fabricated with ITO transparent <span class="hlt">p</span>-electrode during accelerated electro-thermal stress. As the thermal stress increased from 150 degrees C to 250 degrees C at a electrical stress of 200 mA, the optical power of the LEDs was significantly reduced. Degradation of the optical power was thermally activated, with the activation of 0.9 eV. In addition, the activation energy of the degradation of optical power was fairly similar to that of the degradation of series resistance of the LEDs, 1.0 eV, which implies that the increase in the series resistance may result in the severe degradation of optical power. We also showed that the increase in the series resistance of the LEDs during the accelerated electro-thermal stress can be attributed to reduction of the active acceptor concentration in the <span class="hlt">p</span>-type semiconductor layers and local joule heating due to the current crowding.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4437377','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4437377"><span>Hydrothermally Grown In-doped ZnO Nanorods on <span class="hlt">p-GaN</span> Films for Color-tunable Heterojunction Light-emitting-<span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Park, Geun Chul; Hwang, Soo Min; Lee, Seung Muk; Choi, Jun Hyuk; Song, Keun Man; Kim, Hyun You; Kim, Hyun-Suk; Eum, Sung-Jin; Jung, Seung-Boo; Lim, Jun Hyung; Joo, Jinho</p> <p>2015-01-01</p> <p>The incorporation of doping elements in ZnO nanostructures plays an important role in adjusting the optical and electrical properties in optoelectronic devices. In the present study, we fabricated 1-D ZnO nanorods (NRs) doped with different In contents (0% ~ 5%) on <span class="hlt">p-GaN</span> films using a facile hydrothermal method, and investigated the effect of the In doping on the morphology and electronic structure of the NRs and the electrical and optical performances of the <span class="hlt">n</span>-ZnO NRs/<span class="hlt">p-GaN</span> heterojunction light emitting <span class="hlt">diodes</span> (LEDs). As the In content increased, the size (diameter and length) of the NRs increased, and the electrical performance of the LEDs improved. From the electroluminescence (EL) spectra, it was found that the broad green-yellow-orange emission band significantly increased with increasing In content due to the increased defect states (oxygen vacancies) in the ZnO NRs, and consequently, the superposition of the emission bands centered at 415 nm and 570 nm led to the generation of white-light. These results suggest that In doping is an effective way to tailor the morphology and the optical, electronic, and electrical properties of ZnO NRs, as well as the EL emission property of heterojunction LEDs. PMID:25988846</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25988846','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25988846"><span>Hydrothermally Grown In-doped ZnO Nanorods on <span class="hlt">p-GaN</span> Films for Color-tunable Heterojunction Light-emitting-<span class="hlt">diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Park, Geun Chul; Hwang, Soo Min; Lee, Seung Muk; Choi, Jun Hyuk; Song, Keun Man; Kim, Hyun You; Kim, Hyun-Suk; Eum, Sung-Jin; Jung, Seung-Boo; Lim, Jun Hyung; Joo, Jinho</p> <p>2015-05-19</p> <p>The incorporation of doping elements in ZnO nanostructures plays an important role in adjusting the optical and electrical properties in optoelectronic devices. In the present study, we fabricated 1-D ZnO nanorods (NRs) doped with different In contents (0% ~ 5%) on <span class="hlt">p-GaN</span> films using a facile hydrothermal method, and investigated the effect of the In doping on the morphology and electronic structure of the NRs and the electrical and optical performances of the <span class="hlt">n</span>-ZnO NRs/<span class="hlt">p-GaN</span> heterojunction light emitting <span class="hlt">diodes</span> (LEDs). As the In content increased, the size (diameter and length) of the NRs increased, and the electrical performance of the LEDs improved. From the electroluminescence (EL) spectra, it was found that the broad green-yellow-orange emission band significantly increased with increasing In content due to the increased defect states (oxygen vacancies) in the ZnO NRs, and consequently, the superposition of the emission bands centered at 415 nm and 570 nm led to the generation of white-light. These results suggest that In doping is an effective way to tailor the morphology and the optical, electronic, and electrical properties of ZnO NRs, as well as the EL emission property of heterojunction LEDs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JSemi..35d3001S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JSemi..35d3001S"><span>Fabrication and electrical properties of <span class="hlt">p</span>-CuAlO2/(<span class="hlt">n</span>-, <span class="hlt">p</span>-)Si heterojunctions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Suzhen, Wu; Zanhong, Deng; Weiwei, Dong; Jingzhen, Shao; Xiaodong, Fang</p> <p>2014-04-01</p> <p>CuAlO2 thin films have been prepared by the chemical solution deposition method on both <span class="hlt">n</span>-Si and <span class="hlt">p</span>-Si substrates. X-ray diffraction analysis indicates that the obtained CuAlO2 films have a single delafossite structure. The current transport properties of the resultant <span class="hlt">p</span>-CuAlO2/<span class="hlt">n</span>-Si and <span class="hlt">p</span>-CuAlO2/<span class="hlt">p</span>-Si heterojunctions are investigated by current-voltage measurements. The <span class="hlt">p</span>-CuAlO2/<span class="hlt">n</span>-Si has a rectifying ratio of ~35 within the applied voltages of -3.0 to +3.0 V, while the <span class="hlt">p</span>-CuAlO2/<span class="hlt">p</span>-Si shows Schottky <span class="hlt">diode</span>-like characteristics, dominated in forward bias by the flow of space-charge-limited current.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SSCom.270..124S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SSCom.270..124S"><span>Fabrication of the heterojunction <span class="hlt">diode</span> from Y-doped ZnO thin films on <span class="hlt">p</span>-Si substrates by sol-gel method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sharma, Sanjeev K.; Singh, Satendra Pal; Kim, Deuk Young</p> <p>2018-02-01</p> <p>The heterojunction <span class="hlt">diode</span> of yttrium-doped ZnO (YZO) thin films was fabricated on <span class="hlt">p</span>-Si(100) substrates by sol-gel method. The post-annealing process was performed at 600 °C in vacuum for a short time (3 min) to prevent inter-diffusion of Zn, Y, and Si atoms. X-ray diffraction (XRD) pattern of as-grown and annealed (600 °C in vacuum) films showed the preferred orientation along the c-axis (002) regardless of dopant concentrations. The uniform surface microstructure and the absence of other metal/oxide peaks in XRD pattern confirmed the excellence of films. The increasing bandgap and carrier concentration of YZO thin films were interpreted by the BM shift, that is, the Fermi level moves towards the conduction band edge. The current-voltage characteristics of the heterojunction <span class="hlt">diode</span>, In/<span class="hlt">n-ZnO/p</span>-Si/Al, showed a rectification behavior. The turn-on voltage and ideality factor of <span class="hlt">n-ZnO/p</span>-Si and <span class="hlt">n-YZO/p</span>-Si were observed to be 3.47 V, 2.61 V, and 1.97, 1.89, respectively. Y-dopant in ZnO thin films provided more donor electrons caused the shifting of Fermi-energy level towards the conduction band and strengthen the interest for heterojunction <span class="hlt">diodes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApPhA.122.1024M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApPhA.122.1024M"><span>Tuning of optical and electrical properties of wide band gap Fe:SnO2/Li:NiO <span class="hlt">p</span>- <span class="hlt">n</span> junctions using 80 MeV oxygen ion beam</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mistry, Bhaumik V.; Avasthi, D. K.; Joshi, U. S.</p> <p>2016-12-01</p> <p>Electrical and optical properties of pristine and swift heavy ion (SHI) irradiated <span class="hlt">p</span>- <span class="hlt">n</span> junction <span class="hlt">diode</span> have been investigated for advanced electronics application. Fe:SnO2/Li:NiO <span class="hlt">p</span>- <span class="hlt">n</span> junction was fabricated by using pulsed laser deposition on c-sapphire substrate. The optical band gaps of Fe:SnO2 and Li:NiO films were obtained to be 3.88 and 3.37 eV, respectively. The current-voltage characteristics of the oxide-based <span class="hlt">p</span>- <span class="hlt">n</span> junction showed a rectifying behaviour with turn-on voltage of 0.95 V. The oxide-based <span class="hlt">p</span>- <span class="hlt">n</span> junction <span class="hlt">diode</span> was irradiated to 80 MeV O+6 ions with 1 × 1012 ions/cm2 fluence. Decrease in grain size due to SHI irradiation is confirmed by the grazing angle X-ray diffraction and atomic force microscopy. In comparison with the pristine <span class="hlt">p</span>- <span class="hlt">n</span> junction <span class="hlt">diode</span>, O+6 ion irradiated <span class="hlt">p-n</span> junction <span class="hlt">diode</span> shows the increase of surface roughness and decrease of percentage transmittance in visible region. For irradiated <span class="hlt">p</span>- <span class="hlt">n</span> junction <span class="hlt">diode</span>, current-voltage curve has still rectifying behaviour but exhibits lower turn-on voltage than that of virgin <span class="hlt">p</span>- <span class="hlt">n</span> junction <span class="hlt">diode</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23892611','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23892611"><span>Synthesis of <span class="hlt">p</span>-type Ga<span class="hlt">N</span> nanowires.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Sung Wook; Park, Youn Ho; Kim, Ilsoo; Park, Tae-Eon; Kwon, Byoung Wook; Choi, Won Kook; Choi, Heon-Jin</p> <p>2013-09-21</p> <p>Ga<span class="hlt">N</span> has been utilized in optoelectronics for two decades. However, <span class="hlt">p</span>-type doping still remains crucial for realization of high performance Ga<span class="hlt">N</span> optoelectronics. Though Mg has been used as a <span class="hlt">p</span>-dopant, its efficiency is low due to the formation of Mg-H complexes and/or structural defects in the course of doping. As a potential alternative <span class="hlt">p</span>-type dopant, Cu has been recognized as an acceptor impurity for Ga<span class="hlt">N</span>. Herein, we report the fabrication of Cu-doped Ga<span class="hlt">N</span> nanowires (Cu:Ga<span class="hlt">N</span> NWs) and their <span class="hlt">p</span>-type characteristics. The NWs were grown vertically via a vapor-liquid-solid (VLS) mechanism using a Au/Ni catalyst. Electrical characterization using a nanowire-field effect transistor (NW-FET) showed that the NWs exhibited <span class="hlt">n</span>-type characteristics. However, with further annealing, the NWs showed <span class="hlt">p</span>-type characteristics. A homo-junction structure (consisting of annealed Cu:Ga<span class="hlt">N</span> NW/<span class="hlt">n</span>-type Ga<span class="hlt">N</span> thin film) exhibited <span class="hlt">p-n</span> junction characteristics. A hybrid organic light emitting <span class="hlt">diode</span> (OLED) employing the annealed Cu:Ga<span class="hlt">N</span> NWs as a hole injection layer (HIL) also demonstrated current injected luminescence. These results suggest that Cu can be used as a <span class="hlt">p</span>-type dopant for Ga<span class="hlt">N</span> NWs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29178457','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29178457"><span>Relative dosimetry with an MR-linac: Response of ion chambers, diamond, and <span class="hlt">diode</span> <span class="hlt">detectors</span> for off-axis, depth dose, and output factor measurements.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>O'Brien, Daniel J; Dolan, James; Pencea, Stefan; Schupp, Nicholas; Sawakuchi, Gabriel O</p> <p>2018-02-01</p> <p>The purpose of this study was to acquire beam data for an MR-linac, with and without a 1.5 T magnetic field, by using a variety of commercially available <span class="hlt">detectors</span> to assess their relative response in the magnetic field. The impact of the magnetic field on the measured dose distribution was also assessed. An MR-safe 3D scanning water phantom was used to measure output factors, depth dose curves, and off-axis profiles for various depths and for field sizes between 2 × 2 cm 2 and 22 × 22 cm 2 for an Elekta MR-linac beam with the orthogonal 1.5 T magnetic field on or off. An on-board MV portal imaging system was used to ensure that the reproducibility of the <span class="hlt">detector</span> position, both with and without the magnetic field, was within 0.1 mm. The <span class="hlt">detectors</span> used included ionization chambers with large, medium, and small sensitive volumes; a diamond <span class="hlt">detector</span>; a shielded <span class="hlt">diode</span>; and an unshielded <span class="hlt">diode</span>. The offset of the effective point of measurement of the ionization chambers was found to be reduced by at least half for each chamber in the direction parallel with the beam. A lateral shift of similar magnitude was also introduced to the chambers' effective point of measurement toward the average direction of the Lorentz force. A similar lateral shift (but in the opposite direction) was also observed for the diamond and <span class="hlt">diode</span> <span class="hlt">detectors</span>. The measured lateral shift in the dose distribution was independent of depth and field size for each <span class="hlt">detector</span> for fields between 2 × 2 cm 2 and 10 × 10 cm 2 . The shielded <span class="hlt">diode</span> significantly misrepresented the dose distribution in the lateral direction perpendicular to the magnetic field, making it seem more symmetric. The percentage depth dose was generally found to be lower with the magnetic field than without, but this difference was reduced as field size increased. The depth of maximum dose showed little dependence on field size in the presence of the magnetic field, with values from 1.2 cm to 1.3 cm between the 2</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990004614','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990004614"><span>Study of Bulk and Elementary Screw Dislocation Assisted Reverse Breakdown in Low-Voltage (less than 250 V) 4H-SiC <span class="hlt">p(+)n</span> Junction <span class="hlt">diodes</span>. Part 1; DC Properties</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Neudeck, Philip G.; Huang, Wei; Dudley, Michael</p> <p>1998-01-01</p> <p>Given the high density (approx. 10(exp 4)/sq cm) of elementary screw dislocations (Burgers vector = 1c with no hollow core) in commercial SiC wafers and epilayers, all appreciable current (greater than 1 A) SiC power devices will likely contain elementary screw dislocations for the foreseeable future. It is therefore important to ascertain the electrical impact of these defects, particularly in high-field vertical power device topologies where SiC is expected to enable large performance improvements in solid-state high-power systems. This paper compares the DC-measured reverse-breakdown characteristics of low-voltage (less than 250 V) small-area (less than 5 x 10(exp -4)/sq cm) 4H-SiC <span class="hlt">p(+)n</span> <span class="hlt">diodes</span> with and without elementary screw dislocations. Compared to screw dislocation-free devices, <span class="hlt">diodes</span> containing elementary screw dislocations exhibited higher pre-breakdown reverse leakage currents, softer reverse breakdown <span class="hlt">I</span>-V knees, and highly localized microplasmic breakdown current filaments. The observed localized 4H-SiC breakdown parallels microplasmic breakdowns observed in silicon and other semiconductors, in which space-charge effects limit current conduction through the local microplasma as reverse bias is increased.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/7163590','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/7163590"><span>Fabrication of poly(<span class="hlt">p</span>-phenyleneacetylene) light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Shinar, J.; Swanson, L.S.; Lu, F.; Ding, Y.</p> <p>1994-08-02</p> <p>Acetylene-containing poly(<span class="hlt">p</span>-phenyleneacetylene) (PPA)-based light-emitting <span class="hlt">diodes</span> (LEDs) are provided. The LEDs are fabricated by coating a hole-injecting electrode, preferably an indium tin oxide (ITO) coated glass substrate, with a PPA polymer, such as a 2,5-dibutoxy or a 2,5-dihexoxy derivative of PPA, dissolved in an organic solvent. This is then followed by evaporating a layer of material capable of injecting electrons, such as Al or Al/Ca, onto the polymer to form a base electrode. This composition is then annealed to form efficient EL <span class="hlt">diodes</span>. 8 figs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/869421','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/869421"><span>Fabrication of poly(<span class="hlt">p</span>-phenyleneacetylene) light-emitting <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Shinar, Joseph; Swanson, Leland S.; Lu, Feng; Ding, Yiwei</p> <p>1994-08-02</p> <p>Acetylene containing poly(<span class="hlt">p</span>-phenyleneacetylene) (PPA) - based light-emitting <span class="hlt">diodes</span> (LEDs) are provided. The LEDs are fabricated by coating a hole-injecting electrode, preferably an indium tin oxide (ITO) coated glass substrate, with a PPA polymer, such as a 2,5-dibutoxy or a 2,5-dihexoxy derivative of PPA, dissolved in an organic solvent. This is then followed by evaporating a layer of material capable of injecting electrons, such as A1 or A1/Ca, onto the polymer to form a base electrode. This composition is then annealed to form efficient EL <span class="hlt">diodes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1042982','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1042982"><span>Axis-1 <span class="hlt">diode</span> simulations <span class="hlt">I</span>: standard 2-inch cathode</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Ekdahl, Carl</p> <p>2011-01-11</p> <p>The standard configuration of the DARHT Axis-<span class="hlt">I</span> <span class="hlt">diode</span> features a 5.08-cm diameter velvet emitter mounted in the flat surface of the cathode shroud. The surface of the velvet is slightly recessed {approx}2.5 mm. This configuration produces a 1.75 kA beam when a 3.8-MV pulse is applied to the anode-cathode (AK) gap. This note addresses some of the physics of this <span class="hlt">diode</span> through the use of finite-element simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JAP...115h4503H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JAP...115h4503H"><span>Planar micro- and nano-patterning of Ga<span class="hlt">N</span> light-emitting <span class="hlt">diodes</span>: Guidelines and limitations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Herrnsdorf, Johannes; Xie, Enyuan; Watson, Ian M.; Laurand, Nicolas; Dawson, Martin D.</p> <p>2014-02-01</p> <p>The emission area of Ga<span class="hlt">N</span> light-emitting <span class="hlt">diodes</span> can be patterned by etch-free current aperturing methods which exploit the thin and highly resistive nature of the <span class="hlt">p</span>-doped layer in these devices. Here, the fundamental underlying electrical and optical aspects of high-resolution current aperturing are investigated theoretically. The most critical parameter for the possible resolution is the thickness d of the <span class="hlt">p-GaN</span> layer, but the interplay of <span class="hlt">p-GaN</span> resistivity and electrical junction characteristics is also important. A spatial resolution of 1.59d can in principle be achieved, corresponding to about 300 nm in typical epitaxial structures. Furthermore, the emission from such a small emitter will spread by about 600 nm while propagating through the <span class="hlt">p-GaN</span>. Both values can be reduced by reducing d.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28696342','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28696342"><span>Single In x Ga1-x As nanowire/<span class="hlt">p</span>-Si heterojunction based nano-rectifier <span class="hlt">diode</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sarkar, K; Palit, M; Guhathakurata, S; Chattopadhyay, S; Banerji, P</p> <p>2017-09-20</p> <p>Nanoscale power supply units will be indispensable for fabricating next generation smart nanoelectronic integrated circuits. Fabrication of nanoscale rectifier circuits on a Si platform is required for integrating nanoelectronic devices with on-chip power supply units. In the present study, a nanorectifier <span class="hlt">diode</span> based on a single standalone In x Ga 1-x As nanowire/<span class="hlt">p</span>-Si (111) heterojunction fabricated by metal organic chemical vapor deposition technique has been studied. The nanoheterojunction <span class="hlt">diodes</span> have shown good rectification and fast switching characteristics. The rectification characteristics of the nanoheterojunction have been demonstrated by different standard waveforms of sinusoidal, square, sawtooth and triangular for two different frequencies of 1 and 0.1 Hz. Reverse recovery time of around 150 ms has been observed in all wave response. A half wave rectifier circuit with a simple capacitor filter has been assembled with this nanoheterojunction <span class="hlt">diode</span> which provides 12% output efficiency. The transport of carriers through the heterojunction is investigated. The interface states density of the nanoheterojunction has also been determined. Occurrence of output waveforms incommensurate with the input is attributed to higher series resistance of the <span class="hlt">diode</span> which is further explained considering the dimension of <span class="hlt">p</span>-side and <span class="hlt">n</span>-side of the junction. The sudden change of ideality factor after 1.7 V bias is attributed to recombination through interface states in space charge region. Low interface states density as well as high rectification ratio makes this heterojunction <span class="hlt">diode</span> a promising candidate for future nanoscale electronics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA560393','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA560393"><span>Performance Improvement of Long-Wave Infrared InAs/GaSb Strained-Layer Superlattice <span class="hlt">Detectors</span> Through Sulfur-Based Passivation</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2012-01-01</p> <p>14]. The <span class="hlt">detector</span> material was processed into a variable area <span class="hlt">diode</span> array (VADA) of square and circular mesa <span class="hlt">diodes</span> with the size of <span class="hlt">diode</span> mesa sides...processed as single element <span class="hlt">detectors</span> with 410 lm 410 lm square mesas having circular apertures ranging in diameter from 25 to 300 lm. The processing was...passivations schemes with perimeter-to-area ratio (<span class="hlt">P</span>/A) of 1600 cm1 ( mesa side size is 25 lm). Fig. 3. Inverse of the dynamic resistance area product (RdA</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28081598','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28081598"><span>An AlGa<span class="hlt">N</span> Core-Shell Tunnel Junction Nanowire Light-Emitting <span class="hlt">Diode</span> Operating in the Ultraviolet-C Band.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sadaf, S M; Zhao, S; Wu, Y; Ra, Y-H; Liu, X; Vanka, S; Mi, Z</p> <p>2017-02-08</p> <p>To date, semiconductor light emitting <span class="hlt">diodes</span> (LEDs) operating in the deep ultraviolet (UV) spectral range exhibit very low efficiency due to the presence of large densities of defects and extremely inefficient <span class="hlt">p</span>-type conduction of conventional AlGa<span class="hlt">N</span> quantum well heterostructures. We have demonstrated that such critical issues can be potentially addressed by using nearly defect-free AlGa<span class="hlt">N</span> tunnel junction core-shell nanowire heterostructures. The core-shell nanowire arrays exhibit high photoluminescence efficiency (∼80%) in the UV-C band at room temperature. With the incorporation of an epitaxial Al tunnel junction, the <span class="hlt">p-(Al)GaN</span> contact-free nanowire deep UV LEDs showed nearly one order of magnitude reduction in the device resistance, compared to the conventional nanowire <span class="hlt">p-i-n</span> device. The unpackaged Al tunnel junction deep UV LEDs exhibit an output power >8 mW and a peak external quantum efficiency ∼0.4%, which are nearly one to two orders of magnitude higher than previously reported AlGa<span class="hlt">N</span> nanowire devices. Detailed studies further suggest that the maximum achievable efficiency is limited by electron overflow and poor light extraction efficiency due to the TM polarized emission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10563E..1WB','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10563E..1WB"><span>Development and characterisation of MCT <span class="hlt">detectors</span> for space astrophysics at CEA</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boulade, O.; Baier, N.; Castelein, P.; Cervera, C.; Chorier, P.; Destefanis, G.; Fièque, B.; Gravrand, O.; Guellec, F.; Moreau, V.; Mulet, P.; Pinsard, F.; Zanatta, J.-P.</p> <p>2017-11-01</p> <p> noise, as the <span class="hlt">detector</span> operating temperature has a very strong impact at system level. A consequence of reaching low levels of dark current is the need for very low noise readout circuits. CEA and SOFRADIR are involved in a number of activities that have already started in this framework. CEA/LETI does the development of the photo-voltaic (PV) layers - MCT material growth, <span class="hlt">diode</span> technologies-, as well as some electro-optical characterisation at wafer, <span class="hlt">diode</span> and hybrid component levels, and CEA/IRFU/SAp does all the electro-optical characterisation involving very low flux measurements (mostly dark current measurements). Depending of the program, SOFRADIR can also participate in the development of the hybrid components, for instance the very low noise readout circuits (ROIC) can be developed either at SOFRADIR or at CEA/LETI. Depending of the component specifications, the MCT epitaxy can be either liquid phase (LPE, which is the standard at SOFRADIR for production purposes) or molecular beam (MBE), the <span class="hlt">diode</span> technology can be <span class="hlt">n/p</span> (standard at LETI and SOFRADIR) or <span class="hlt">p/n</span> (under development for several years now) [3], and the input stage of the ROIC can be Source Follower per <span class="hlt">Detector</span> (SFD for very low flux low noise programs) or Capacitive Trans Impedance Amplifier (CTIA for intermediate flux programs) [4]. This paper will present the different developments and results obtained so far in the two NIR-SWIR and MWIR-LWIR spectral ranges, as well as the perspectives for the near future. CEA/LETI is also involved in the development of MCT Avalanche Photo <span class="hlt">Diodes</span> (APD) that will be discussed in other papers [5,6].</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_22 --> <div id="page_23" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="441"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19420563','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19420563"><span>Amplified spontaneous emission from ZnO in <span class="hlt">n</span>-ZnO/ZnO nanodots-SiO(2) composite/<span class="hlt">p-AlGaN</span> heterojunction light-emitting <span class="hlt">diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shih, Ying Tsang; Wu, Mong Kai; Li, Wei Chih; Kuan, Hon; Yang, Jer Ren; Shiojiri, Makoto; Chen, Miin Jang</p> <p>2009-04-22</p> <p>This study demonstrates amplified spontaneous emission (ASE) of the ultraviolet (UV) electroluminescence (EL) from ZnO at lambda~380 nm in the <span class="hlt">n</span>-ZnO/ZnO nanodots-SiO(2) composite/<span class="hlt">p</span>- Al(0.12)Ga(0.88)<span class="hlt">N</span> heterojunction light-emitting <span class="hlt">diode</span>. A SiO(2) layer embedded with ZnO nanodots was prepared on the <span class="hlt">p</span>-type Al(0.12)Ga(0.88)<span class="hlt">N</span> using spin-on coating of SiO(2) nanoparticles followed by atomic layer deposition (ALD) of ZnO. An <span class="hlt">n</span>-type Al-doped ZnO layer was deposited upon the ZnO nanodots-SiO(2) composite layer also by the ALD technique. High-resolution transmission electron microscopy (HRTEM) reveals that the ZnO nanodots embedded in the SiO(2) matrix have diameters of 3-8 nm and the wurtzite crystal structure, which allows the transport of carriers through the thick ZnO nanodots-SiO(2) composite layer. The high quality of the <span class="hlt">n</span>-ZnO layer was manifested by the well crystallized lattice image in the HRTEM picture and the low-threshold optically pumped stimulated emission. The low refractive index of the ZnO nanodots-SiO(2) composite layer results in the increase in the light extraction efficiency from <span class="hlt">n</span>-ZnO and the internal optical feedback of UV EL into <span class="hlt">n</span>-ZnO layer. Consequently, significant enhancement of the UV EL intensity and super-linear increase in the EL intensity, as well as the spectral narrowing, with injection current were observed owing to ASE in the <span class="hlt">n</span>-ZnO layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhDT.......155T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhDT.......155T"><span>A method for (<span class="hlt">n</span>,alpha) and (<span class="hlt">n,p</span>) cross section measurements using a lead slowing-down spectrometer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thompson, Jason Tyler</p> <p></p> <p>The need for nuclear data comes from several sources including astrophysics, stockpile stewardship, and reactor design. Photodisintegration, neutron capture, and charged particle out reactions on stable or short-lived radioisotopes play crucial roles during stellar evolution and forming solar isotopic abundances whereas these reactions can affect the safety of our national weapons stockpile or criticality and safety calculations for reactors. Although models can be used to predict some of these values, these predictions are only as good as the experimental data that constrains them. For neutron-induced emission of α particles and protons ((<span class="hlt">n</span>,α) and (<span class="hlt">n,p</span>) reactions) at energies below 1 MeV, the experimental data is at best scarce and models must rely on extrapolations from unlike situations, (<span class="hlt">i</span>.e. different reactions, isotopes, and energies) providing ample room for uncertainty. In this work a new method of measuring energy dependent (<span class="hlt">n</span>,α) and (<span class="hlt">n,p</span>) cross sections was developed for the energy range of 0.1 eV - ˜100 keV using a lead slowing-down spectrometer (LSDS). The LSDS provides a ˜10 4 neutron flux increase over the more conventionally used time-of-flight (ToF) methods at equivalent beam conditions, allowing for the measurement of small cross sections (µb’s to mb’s) while using small sample masses (µg’s to mg’s). Several <span class="hlt">detector</span> concepts were designed and tested, including specially constructed Canberra passivated, implanted, planar silicon (PIPS) <span class="hlt">detectors</span>; and gas-electron-multiplier (GEM) foils. All designs are compensated to minimize γ-flash problems. The GEM <span class="hlt">detector</span> was found to function satisfactory for (<span class="hlt">n</span>,α) measurements, but the PIPS <span class="hlt">detectors</span> were found to be better suited for (<span class="hlt">n,p</span>) reaction measurements. A digital data acquisition (DAQ) system was programmed such that background can be measured simultaneously with the reaction cross section. Measurements of the 147Sm(<span class="hlt">n</span>,α)144Nd and 149 Sm(<span class="hlt">n</span>,α)146Nd reaction cross sections were</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApPhA.123..279V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhA.123..279V"><span>Electrical and carrier transport properties of the Au/Y2O3/<span class="hlt">n-GaN</span> metal-insulator-semiconductor (MIS) <span class="hlt">diode</span> with rare-earth oxide interlayer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Venkata Prasad, C.; Rajagopal Reddy, V.; Choi, Chel-Jong</p> <p>2017-04-01</p> <p>The electrical and transport properties of rare-earth Y2O3 on <span class="hlt">n</span>-type Ga<span class="hlt">N</span> with Au electrode have been investigated by current-voltage and capacitance-voltage techniques at room temperature. The Au/Y2O3/<span class="hlt">n-GaN</span> metal-insulator-semiconductor (MIS) <span class="hlt">diode</span> shows a good rectification behavior compared to the Au/<span class="hlt">n-GaN</span> metal-semiconductor (MS) <span class="hlt">diode</span>. Statistical analysis showed that a mean barrier height (BH) and ideality factor are 0.78 eV and 1.93, and 0.96 eV and 2.09 for the Au/<span class="hlt">n-GaN</span> MS and Au/Y2O3/<span class="hlt">n-GaN</span> MIS <span class="hlt">diodes</span>, respectively. Results indicate that the high BH is obtained for the MIS <span class="hlt">diode</span> compared to the MS <span class="hlt">diode</span>. The BH, ideality factor and series resistance are also estimated by Cheung's function and Norde method. From the forward current-voltage data, the interface state density ( <span class="hlt">N</span> SS) is estimated for both the MS and MIS Schottky <span class="hlt">diodes</span>, and found that the estimated <span class="hlt">N</span> SS is lower for the MIS <span class="hlt">diode</span> compared to the MS <span class="hlt">diode</span>. The results reveal that the introduction of Y2O3 interlayer facilitated the reduction of <span class="hlt">N</span> SS of the Au/<span class="hlt">n-GaN</span> interface. Experimental results suggest that the Poole-Frenkel emission is a dominant conduction mechanism in the reverse bias region of both Au/<span class="hlt">n-GaN</span> MS and Au/Y2O3/<span class="hlt">n-GaN</span> MIS <span class="hlt">diodes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21538104-temperature-dependent-electrical-transport-behavior-inn-gan-heterostructure-based-schottky-diodes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21538104-temperature-dependent-electrical-transport-behavior-inn-gan-heterostructure-based-schottky-diodes"><span>Temperature dependent electrical transport behavior of In<span class="hlt">N/GaN</span> heterostructure based Schottky <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Roul, Basanta; Kumar, Mahesh; Central Research Laboratory, Bharat Electronics, Bangalore 560013</p> <p></p> <p>In<span class="hlt">N/GaN</span> heterostructure based Schottky <span class="hlt">diodes</span> were fabricated by plasma-assisted molecular beam epitaxy. The temperature dependent electrical transport properties were carried out for In<span class="hlt">N/GaN</span> heterostructure. The barrier height and the ideality factor of the Schottky <span class="hlt">diodes</span> were found to be temperature dependent. The temperature dependence of the barrier height indicates that the Schottky barrier height is inhomogeneous in nature at the heterostructure interface. The higher value of the ideality factor and its temperature dependence suggest that the current transport is primarily dominated by thermionic field emission (TFE) other than thermionic emission (TE). The room temperature barrier height obtained by using TEmore » and TFE models were 1.08 and 1.43 eV, respectively.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29328213','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29328213"><span>Iodine-stabilized single-frequency green InGa<span class="hlt">N</span> <span class="hlt">diode</span> laser.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Yi-Hsi; Lin, Wei-Chen; Shy, Jow-Tsong; Chui, Hsiang-Chen</p> <p>2018-01-01</p> <p>A 520-nm InGa<span class="hlt">N</span> <span class="hlt">diode</span> laser can emit a milliwatt-level, single-frequency laser beam when the applied current slightly exceeds the lasing threshold. The laser frequency was less sensitive to <span class="hlt">diode</span> temperature and could be finely tuned by adjusting the applied current. Laser frequency was stabilized onto a hyperfine component in an iodine transition through the saturated absorption spectroscopy. The uncertainty of frequency stabilization was approximately 8×10 -9 at a 10-s integration time. This compact laser system can replace the conventional green <span class="hlt">diode</span>-pumped solid-state laser and applied as a frequency reference. A single longitudinal mode operational region with <span class="hlt">diode</span> temperature, current, and output power was investigated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27052973','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27052973"><span>Giant spin-torque <span class="hlt">diode</span> sensitivity in the absence of bias magnetic field.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fang, Bin; Carpentieri, Mario; Hao, Xiaojie; Jiang, Hongwen; Katine, Jordan A; Krivorotov, Ilya N; Ocker, Berthold; Langer, Juergen; Wang, Kang L; Zhang, Baoshun; Azzerboni, Bruno; Amiri, Pedram Khalili; Finocchio, Giovanni; Zeng, Zhongming</p> <p>2016-04-07</p> <p>Microwave <span class="hlt">detectors</span> based on the spin-torque <span class="hlt">diode</span> effect are among the key emerging spintronic devices. By utilizing the spin of electrons in addition to charge, they have the potential to overcome the theoretical performance limits of their semiconductor (Schottky) counterparts. However, so far, practical implementations of spin-<span class="hlt">diode</span> microwave <span class="hlt">detectors</span> have been limited by the necessity to apply a magnetic field. Here, we demonstrate nanoscale magnetic tunnel junction microwave <span class="hlt">detectors</span>, exhibiting high-detection sensitivity of 75,400 mV mW(-1) at room temperature without any external bias fields, and for low-input power (micro-Watts or lower). This sensitivity is significantly larger than both state-of-the-art Schottky <span class="hlt">diode</span> <span class="hlt">detectors</span> and existing spintronic <span class="hlt">diodes</span>. Micromagnetic simulations and measurements reveal the essential role of injection locking to achieve this sensitivity performance. This mechanism may provide a pathway to enable further performance improvement of spin-torque <span class="hlt">diode</span> microwave <span class="hlt">detectors</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4829691','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4829691"><span>Giant spin-torque <span class="hlt">diode</span> sensitivity in the absence of bias magnetic field</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Fang, Bin; Carpentieri, Mario; Hao, Xiaojie; Jiang, Hongwen; Katine, Jordan A.; Krivorotov, Ilya N.; Ocker, Berthold; Langer, Juergen; Wang, Kang L.; Zhang, Baoshun; Azzerboni, Bruno; Amiri, Pedram Khalili; Finocchio, Giovanni; Zeng, Zhongming</p> <p>2016-01-01</p> <p>Microwave <span class="hlt">detectors</span> based on the spin-torque <span class="hlt">diode</span> effect are among the key emerging spintronic devices. By utilizing the spin of electrons in addition to charge, they have the potential to overcome the theoretical performance limits of their semiconductor (Schottky) counterparts. However, so far, practical implementations of spin-<span class="hlt">diode</span> microwave <span class="hlt">detectors</span> have been limited by the necessity to apply a magnetic field. Here, we demonstrate nanoscale magnetic tunnel junction microwave <span class="hlt">detectors</span>, exhibiting high-detection sensitivity of 75,400 mV mW−1 at room temperature without any external bias fields, and for low-input power (micro-Watts or lower). This sensitivity is significantly larger than both state-of-the-art Schottky <span class="hlt">diode</span> <span class="hlt">detectors</span> and existing spintronic <span class="hlt">diodes</span>. Micromagnetic simulations and measurements reveal the essential role of injection locking to achieve this sensitivity performance. This mechanism may provide a pathway to enable further performance improvement of spin-torque <span class="hlt">diode</span> microwave <span class="hlt">detectors</span>. PMID:27052973</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22311141-doping-free-iii-nitride-high-electron-mobility-light-emitting-diodes-transistors','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22311141-doping-free-iii-nitride-high-electron-mobility-light-emitting-diodes-transistors"><span><span class="hlt">P</span>-doping-free III-nitride high electron mobility light-emitting <span class="hlt">diodes</span> and transistors</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Li, Baikui; Tang, Xi; Chen, Kevin J., E-mail: eekjchen@ust.hk</p> <p>2014-07-21</p> <p>We report that a simple metal-AlGa<span class="hlt">N/GaN</span> Schottky <span class="hlt">diode</span> is capable of producing Ga<span class="hlt">N</span> band-edge ultraviolet emission at 3.4 eV at a small forward bias larger than ∼2 V at room temperature. Based on the surface states distribution of AlGa<span class="hlt">N</span>, a mature impact-ionization-induced Fermi-level de-pinning model is proposed to explain the underlying mechanism of the electroluminescence (EL) process. By experimenting with different Schottky metals, Ni/Au and Pt/Au, we demonstrated that this EL phenomenon is a “universal” property of metal-AlGa<span class="hlt">N/GaN</span> Schottky <span class="hlt">diodes</span>. Since this light-emitting Schottky <span class="hlt">diode</span> shares the same active structure and fabrication processes as the AlGa<span class="hlt">N/GaN</span> high electron mobility transistors, straight-forward andmore » seamless integration of photonic and electronic functional devices has been demonstrated on doping-free III-nitride heterostructures. Using a semitransparent Schottky drain electrode, an AlGa<span class="hlt">N/GaN</span> high electron mobility light-emitting transistor is demonstrated.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJP..132..178M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJP..132..178M"><span>Electrical characterization of ZnO/NiO <span class="hlt">p-n</span> junction prepared by the sol-gel method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Merih Akyuzlu, A.; Dagdelen, Fethi; Gultek, Ahmet; Hendi, A. A.; Yakuphanoglu, Fahrettin</p> <p>2017-04-01</p> <p>ZnO and NiO films were synthesized on fluourine-doped tin oxide (FTO) glass substrate by the sol-gel method. The surface morphology of the films was investigated by atomic force microscopy. The optical band gaps of the ZnO and NiO films were found to be 3.198 and 3.827eV, respectively. A ZnO/NiO <span class="hlt">p-n</span> junction <span class="hlt">diode</span> was prepared and electrical charge transport mechanism of the <span class="hlt">diode</span> was analyzed using thermionic emission and Norde functions. The ideality factor, barrier height and series resistance of the <span class="hlt">diode</span> were determined to be 6.46, 1.036eV and 39.1 M {Ω} , respectively. The obtained results indicate that ZnO/NiO <span class="hlt">p-n</span> junction can be used as transparent <span class="hlt">diode</span> for optic communications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28438176','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28438176"><span>The PINK1 <span class="hlt">p.I</span>368<span class="hlt">N</span> mutation affects protein stability and ubiquitin kinase activity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ando, Maya; Fiesel, Fabienne C; Hudec, Roman; Caulfield, Thomas R; Ogaki, Kotaro; Górka-Skoczylas, Paulina; Koziorowski, Dariusz; Friedman, Andrzej; Chen, Li; Dawson, Valina L; Dawson, Ted M; Bu, Guojun; Ross, Owen A; Wszolek, Zbigniew K; Springer, Wolfdieter</p> <p>2017-04-24</p> <p>Mutations in PINK1 and PARKIN are the most common causes of recessive early-onset Parkinson's disease (EOPD). Together, the mitochondrial ubiquitin (Ub) kinase PINK1 and the cytosolic E3 Ub ligase PARKIN direct a complex regulated, sequential mitochondrial quality control. Thereby, damaged mitochondria are identified and targeted to degradation in order to prevent their accumulation and eventually cell death. Homozygous or compound heterozygous loss of either gene function disrupts this protective pathway, though at different steps and by distinct mechanisms. While structure and function of PARKIN variants have been well studied, PINK1 mutations remain poorly characterized, in particular under endogenous conditions. A better understanding of the exact molecular pathogenic mechanisms underlying the pathogenicity is crucial for rational drug design in the future. Here, we characterized the pathogenicity of the PINK1 <span class="hlt">p.I</span>368<span class="hlt">N</span> mutation on the clinical and genetic as well as on the structural and functional level in patients' fibroblasts and in cell-based, biochemical assays. Under endogenous conditions, PINK1 <span class="hlt">p.I</span>368<span class="hlt">N</span> is expressed, imported, and <span class="hlt">N</span>-terminally processed in healthy mitochondria similar to PINK1 wild type (WT). Upon mitochondrial damage, however, full-length PINK1 <span class="hlt">p.I</span>368<span class="hlt">N</span> is not sufficiently stabilized on the outer mitochondrial membrane (OMM) resulting in loss of mitochondrial quality control. We found that binding of PINK1 <span class="hlt">p.I</span>368<span class="hlt">N</span> to the co-chaperone complex HSP90/CDC37 is reduced and stress-induced interaction with TOM40 of the mitochondrial protein import machinery is abolished. Analysis of a structural PINK1 <span class="hlt">p.I</span>368<span class="hlt">N</span> model additionally suggested impairments of Ub kinase activity as the ATP-binding pocket was found deformed and the substrate Ub was slightly misaligned within the active site of the kinase. Functional assays confirmed the lack of Ub kinase activity. Here we demonstrated that mutant PINK1 <span class="hlt">p.I</span>368<span class="hlt">N</span> can not be stabilized on the OMM upon</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NatSR...745143Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NatSR...745143Z"><span>Resistive switching mechanism in the one <span class="hlt">diode</span>-one resistor memory based on <span class="hlt">p+-Si/n</span>-ZnO heterostructure revealed by in-situ TEM</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Lei; Zhu, Liang; Li, Xiaomei; Xu, Zhi; Wang, Wenlong; Bai, Xuedong</p> <p>2017-03-01</p> <p>One <span class="hlt">diode</span>-one resistor (1D1R) memory is an effective architecture to suppress the crosstalk interference, realizing the crossbar network integration of resistive random access memory (RRAM). Herein, we designed a <span class="hlt">p+-Si/n</span>-ZnO heterostructure with 1D1R function. Compared with the conventional multilayer 1D1R devices, the structure and fabrication technique can be largely simplified. The real-time imaging of formation/rupture process of conductive filament (CF) process demonstrated the RS mechanism by in-situ transmission electron microscopy (TEM). Meanwhile, we observed that the formed CF is only confined to the outside of depletion region of Si/ZnO pn junction, and the formation of CF does not degrade the <span class="hlt">diode</span> performance, which allows the coexistence of RS and rectifying behaviors, revealing the 1D1R switching model. Furthermore, it has been confirmed that the CF is consisting of the oxygen vacancy by in-situ TEM characterization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhRvB..93i4302M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhRvB..93i4302M"><span>Phonovoltaic. <span class="hlt">I</span>. Harvesting hot optical phonons in a nanoscale <span class="hlt">p</span> -<span class="hlt">n</span> junction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Melnick, Corey; Kaviany, Massoud</p> <p>2016-03-01</p> <p>The phonovoltaic (<span class="hlt">p</span>V) cell is similar to the photovoltaic. It harvests nonequilibrium (hot) optical phonons (Ep ,O) more energetic than the band gap (Δ Ee ,g) to generate power in a <span class="hlt">p-n</span> junction. We examine the theoretical electron-phonon and phonon-phonon scattering rates, the Boltzmann transport of electrons, and the <span class="hlt">diode</span> equation and hydrodynamic simulations to describe the operation of a <span class="hlt">p</span>V cell and develop an analytic model predicting its efficiency. Our findings indicate that a <span class="hlt">p</span>V material with Ep ,O≃Δ Ee ,g≫kBT , where kBT is the thermal energy, and a strong interband electron-phonon coupling surpasses the thermoelectric limit, provided the optical phonon population is excited in a nanoscale cell, enabling the ensuing local nonequilibrium. Finding and tuning a material with these properties is challenging. In Paper II [C. Melnick and M. Kaviany, Phys. Rev. B 93, 125203 (2016), 10.1103/PhysRevB.93.125203], we tune the band gap of graphite within density functional theory through hydrogenation and the application of isotropic strains. The band gap is tuned to resonate with its energetic optical phonon modes and calculate the ab initio electron-phonon and phonon-phonon scattering rates. While hydrogenation degrades the strong electron-phonon coupling in graphene such that the figure of merit vanishes, we outline the methodology for a continued material search.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22591439-improved-performance-vertical-gan-schottky-diode-assisted-algan-tunneling-barrier','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22591439-improved-performance-vertical-gan-schottky-diode-assisted-algan-tunneling-barrier"><span>Improved performance in vertical Ga<span class="hlt">N</span> Schottky <span class="hlt">diode</span> assisted by AlGa<span class="hlt">N</span> tunneling barrier</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Cao, Y.; Chu, R.; Li, R.</p> <p>2016-03-14</p> <p>In a vertical Ga<span class="hlt">N</span> Schottky barrier <span class="hlt">diode</span>, the free electron concentration <span class="hlt">n</span> in the 6-μm-thick drift layer was found to greatly impact the <span class="hlt">diode</span> reverse leakage current, which increased from 2.1 × 10{sup −7} A to 3.9 × 10{sup −4} A as <span class="hlt">n</span> increased from 7.5 × 10{sup 14 }cm{sup −3} to 6.3 × 10{sup 15 }cm{sup −3} at a reverse bias of 100 V. By capping the drift layer with an ultrathin 5-nm graded AlGa<span class="hlt">N</span> layer, reverse leakage was reduced by more than three orders of magnitude with the same <span class="hlt">n</span> in the drift layer. We attribute this to the increased Schottky barrier height with the AlGa<span class="hlt">N</span> at the surface. Meanwhile, themore » polarization field within the graded AlGa<span class="hlt">N</span> effectively shortened the depletion depth, which led to the formation of tunneling current at a relatively small forward bias. The turn-on voltage in the vertical Schottky <span class="hlt">diodes</span> was reduced from 0.77 V to 0.67 V—an advantage in reducing conduction loss in power switching applications.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9466E..04N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9466E..04N"><span>AlGaIn<span class="hlt">N</span> laser <span class="hlt">diode</span> technology and systems for defence and security applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Najda, Stephen P.; Perlin, Piotr; Suski, Tadek; Marona, Lucja; Boćkowski, Mike; Leszczyński, Mike; Wisniewski, Przemek; Czernecki, Robert; Kucharski, Robert; Targowski, Grzegorz; Watson, Scott; Kelly, Antony E.</p> <p>2015-05-01</p> <p>The latest developments in AlGaIn<span class="hlt">N</span> laser <span class="hlt">diode</span> technology are reviewed for defence and security applications such as underwater communications. The AlGaIn<span class="hlt">N</span> material system allows for laser <span class="hlt">diodes</span> to be fabricated over a very wide range of wavelengths from u.v., ~380nm, to the visible ~530nm, by tuning the indium content of the laser GaIn<span class="hlt">N</span> quantum well. Thus AlGaIn<span class="hlt">N</span> laser <span class="hlt">diode</span> technology is a key enabler for the development of new disruptive system level applications in displays, telecom, defence and other industries.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010NIMPA.624..295W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010NIMPA.624..295W"><span>Results from a 64-pixel PIN-<span class="hlt">diode</span> <span class="hlt">detector</span> system for low-energy beta-electrons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wuestling, Sascha; Fraenkle, F.; Habermehl, F.; Renschler, P.; Steidl, M.</p> <p>2010-12-01</p> <p>The KATRIN neutrino mass experiment is based on a precise energy measurement (Δ E/ E=5×10 -5) of electrons emerging from tritium beta decay ( Emax=18.6 keV). This is done by a large electrostatic retarding spectrometer (MAC-E Filter), which is followed by an electron <span class="hlt">detector</span>. Key requirements for this <span class="hlt">detector</span> are a large sensitive area (˜80 cm 2), a certain energy resolution (Δ E=600 eV @ 18.6 keV) but also a certain spatial resolution (˜3 mm), which leads to a multi-pixel design. As a tentative design on the way to the final <span class="hlt">detector</span>, but also for operational service on the so-called pre-spectrometer experiment, a <span class="hlt">detector</span> system with a reduced size (16 cm 2) and a reduced pixel number (64), making use of a monolithic segmented silicon PIN <span class="hlt">diode</span>, was designed and built. While the design and very first measurements have been presented in Wuestling et al. [6], this publication shows the operational performance of the <span class="hlt">detector</span> system. The robust concept of the electronics allowed adaptation to mechanically different experimental setups. The spacial resolution of the <span class="hlt">detector</span> system proved to be essential in examining Penning trap induced background and other effects in the pre-spectrometer experiment. The <span class="hlt">detector</span> performance test runs include energy resolution and calibration, background rates, correlation between pixels (crosstalk), spatially resolved rate analysis, and a dead-layer measurement [7]. The <span class="hlt">detector</span> allows for background searches with a sensitivity as low as 1.3×10 -3 cps/cm 2 in the energy range of 20 keV. This allows the pre-spectrometer to be characterized with e-gun illumination with a signal to background ratio of better than 10 5 and the search for ultra low Penning discharge emissions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/870409','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/870409"><span>Fast Cs<span class="hlt">I</span>-phoswich <span class="hlt">detector</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Langenbrunner, James R.</p> <p>1996-01-01</p> <p>An improved phoswich radiation <span class="hlt">detector</span> used pure Cs<span class="hlt">I</span> crystal and a fast plastic scintillator and a single photomultiplier tube. The plastic is arranged to receive incident radiation, and that which passed through then strikes the Cs<span class="hlt">I</span> crystal. Scintillation light from both the plastic and Cs<span class="hlt">I</span> crystal are applied to the photomultiplier tube, with the light from the plastic passing through the crystal without absorption therein. Electronics are provided for analyzing the output of the photomultiplier tube to discriminate responses due to the plastic and the Cs<span class="hlt">I</span> crystal, through short gate and long gate integration, to produce results which are indicative of the characteristics of the different types of incident radiation, even in the presence of large amounts of radiation. The phoswich <span class="hlt">detector</span> has excellent timing resolution. The scintillators of the Cs<span class="hlt">I</span>- phoswich were chosen for their fast risetimes, of about 3 ns for NE102A, and 30 ns for the pure Cs<span class="hlt">I</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/228060','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/228060"><span>Fast Cs<span class="hlt">I</span>-phoswich <span class="hlt">detector</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Langenbrunner, J.R.</p> <p>1996-05-07</p> <p>An improved phoswich radiation <span class="hlt">detector</span> used pure Cs<span class="hlt">I</span> crystal and a fast plastic scintillator and a single photomultiplier tube. The plastic is arranged to receive incident radiation, and that which passed through then strikes the Cs<span class="hlt">I</span> crystal. Scintillation light from both the plastic and Cs<span class="hlt">I</span> crystal are applied to the photomultiplier tube, with the light from the plastic passing through the crystal without absorption therein. Electronics are provided for analyzing the output of the photomultiplier tube to discriminate responses due to the plastic and the Cs<span class="hlt">I</span> crystal, through short gate and long gate integration, to produce results which are indicative of the characteristics of the different types of incident radiation, even in the presence of large amounts of radiation. The phoswich <span class="hlt">detector</span> has excellent timing resolution. The scintillators of the Cs<span class="hlt">I</span>- phoswich were chosen for their fast risetimes, of about 3 ns for NE102A, and 30 ns for the pure Cs<span class="hlt">I</span>. 5 figs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SeScT..33e5006P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SeScT..33e5006P"><span>Current Transport Properties of Monolayer Graphene/<span class="hlt">n</span>-Si Schottky <span class="hlt">Diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pathak, C. S.; Garg, Manjari; Singh, J. P.; Singh, R.</p> <p>2018-05-01</p> <p>The present work reports on the fabrication and the detailed macroscopic and nanoscale electrical characteristics of monolayer graphene/<span class="hlt">n</span>-Si Schottky <span class="hlt">diodes</span>. The temperature dependent electrical transport properties of monolayer graphene/<span class="hlt">n</span>-Si Schottky <span class="hlt">diodes</span> were investigated. Nanoscale electrical characterizations were carried out using Kelvin probe force microscopy and conducting atomic force microscopy. Most the values of ideality factor and barrier height are found to be in the range of 2.0–4.4 and 0.50–0.70 eV for monolayer graphene/<span class="hlt">n</span>-Si nanoscale Schottky contacts. The tunneling of electrons is found to be responsible for the high value of ideality factor for nanoscale Schottky contacts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22648932-su-diode-array-transmission-detector-systems-evaluation','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22648932-su-diode-array-transmission-detector-systems-evaluation"><span>SU-F-T-326: <span class="hlt">Diode</span> Array Transmission <span class="hlt">Detector</span> Systems Evaluation</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Hoffman, D; Dyer, B; Kumaran Nair, C</p> <p>2016-06-15</p> <p>Purpose: A new transmission <span class="hlt">detector</span>, Delta4 Discover, developed by Scandidos (Uppsala, Sweden) was evaluated for external photon beam verification and quality assurance. The device is an array of 4040 <span class="hlt">diodes</span> designed to be mounted on the linac accessory tray to measure photon field shape, position and fluence during patient treatment. Interfractional measurements are compared to a baseline measurement made during delivery quality assurance. The aim of this work is to evaluate the stability of the device and its effect on the shape and magnitude of the treatment beam. Methods: Beam profiles, percent depth dose, and beam attenuation was measured formore » 6, 10, and 15 MV photon beams with and without the device in place for 1×1 and 30×30 cm2 fields. Changes in profile and percent depth dose was quantified to evaluate the need to recommission the treatment beam, or account for the device with a tray factor. The stability of the radiation measurements was evaluated by measuring the deviation of each <span class="hlt">diode</span> measurement during repeated prostate VMAT treatment delivery. Results: Photon beam profiles changed by < 1.25% in the nonpenumbra regions of the 30×30 cm2 beam. Percent depth dose curves show a 5–7% increased dose at depths < 2.5cm, but agreed within 1% at depths > 2.5cm. This indicates increased skin dose, similar to the use of a physical beam wedge. The device attenuated 6, 10, and 15 MV photon beams by 1.71±0.02%, 1.36±0.03%, and 1.17±0.03%, respectively. The <span class="hlt">diode</span> array reproduced dosimetric measurements within 0.5% standard deviation for repeated prostate VMAT measurement. Conclusion: The device demonstrated stabile radiation measurements, while not changing the treatment beam shape in a clinically significantly manner. Use of this device can be accounted for with a tray factor, as opposed to recommissioning the treatment beam.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9833E..09N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9833E..09N"><span>Free-space and underwater GHz data transmission using AlGaIn<span class="hlt">N</span> laser <span class="hlt">diode</span> technology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Najda, S. P.; Perlin, P.; Suski, T.; Marona, L.; Boćkowski, M.; Leszczyński, M.; Wisniewski, P.; Czernecki, R.; Kucharski, R.; Targowski, G.; Watson, S.; Kelly, A. E.</p> <p>2016-05-01</p> <p>Laser <span class="hlt">diodes</span> fabricated from the AlGaIn<span class="hlt">N</span> material system is an emerging technology for defence and security applications; in particular for free space laser communication. Conventional underwater communication is done acoustically with very slow data rates, short reach, and vulnurable for interception. AlGaIn<span class="hlt">N</span> blue-green laser <span class="hlt">diode</span> technology allows the possibility of both airbourne links and underwater telecom that operate at very fast data rates (GHz), long reach (100's of metres underwater) and can also be quantum encrypted. The latest developments in AlGaIn<span class="hlt">N</span> laser <span class="hlt">diode</span> technology are reviewed for defence and security applications. The AlGaIn<span class="hlt">N</span> material system allows for laser <span class="hlt">diodes</span> to be fabricated over a very wide range of wavelengths from u.v., ~380nm, to the visible ~530nm, by tuning the indium content of the laser GaIn<span class="hlt">N</span> quantum well. Ridge waveguide laser <span class="hlt">diode</span> structures are fabricated to achieve single mode operation with optical powers of <100mW. Visible light communications at high frequency (up to 2.5 Gbit/s) using a directly modulated 422nm Galliumnitride (Ga<span class="hlt">N</span>) blue laser <span class="hlt">diode</span> is reported in free-space and underwater.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_23 --> <div id="page_24" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="461"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19485230','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19485230"><span>Single-laboratory validation of a high-performance liquid chromatographic-<span class="hlt">diode</span> array <span class="hlt">detector</span>-fluorescence <span class="hlt">detector</span>/mass spectrometric method for simultaneous determination of water-soluble vitamins in multivitamin dietary tablets.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Pei; Atkinson, Renata; Wolf, Wayne R</p> <p>2009-01-01</p> <p>The purpose of this study was to develop a single-laboratory validated (SLV) method using high-performance liquid chromatography with different <span class="hlt">detectors</span> [<span class="hlt">diode</span> array <span class="hlt">detector</span> (DAD); fluorescence <span class="hlt">detector</span> (FLD); and mass spectrometry (MS)] for determination of 7 B-complex vitamins (B1-thiamin, B2-riboflavin, B3-nicotinamide, B6-pyridoxine, B9-folic acid, pantothenic acid, and biotin) and vitamin C in multivitamin/multimineral dietary supplements. The method involves the use of a reversed-phase octadecylsilyl column (4 microm, 250 x 2.0 mm id) and a gradient mobile phase profile. Gradient elution was performed at a flow rate of 0.25 mL/min. After a 5 min isocratic elution at 100% A (0.1% formic acid in water), a linear gradient to 50% A and 50% B (0.1% formic acid in acetonitrile) at 15 min was employed. Detection was performed with a DAD as well as either an FLD or a triple-quadrupole MS <span class="hlt">detector</span> in the multiple reaction monitoring mode. SLV was performed using Standard Reference Material (SRM) 3280 Multivitamin/Multimineral Tablets, being developed by the National Institute of Standards and Technology, with support by the Office of Dietary Supplements of the National Institutes of Health. Phosphate buffer (10 mM, <span class="hlt">p</span>H 2.0) extracts of the NIST SRM 3280 were analyzed by the liquid chromatographic (LC)-DAD-FLDIMS method. Following extraction, the method does not require any sample cleanup/preconcentration steps except centrifugation and filtration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4159756','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4159756"><span>Single-Laboratory Validation of a High-Performance Liquid Chromatographic-<span class="hlt">Diode</span> Array <span class="hlt">Detector</span>-Fluorescence <span class="hlt">Detector</span>/Mass Spectrometric Method for Simultaneous Determination of Water-Soluble Vitamins in Multivitamin Dietary Tablets</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Chen, Pei; Atkinson, Renata; Wolf, Wayne R.</p> <p>2014-01-01</p> <p>The purpose of this study was to develop a single-laboratory validated (SLV) method using high-performance liquid chromatography with different <span class="hlt">detectors</span> [<span class="hlt">diode</span> array <span class="hlt">detector</span> (DAD); fluorescence <span class="hlt">detector</span> (FLD); and mass spectrometry (MS)] for determination of 7 B-complex vitamins (B1-thiamin, B2-riboflavin, B3-nicotinamide, B6-pyridoxine, B9-folic acid, pantothenic acid, and biotin) and vitamin C in multivitamin/multimineral dietary supplements. The method involves the use of a reversed-phase octadecylsilyl column (4 µm, 250 × 2.0 mm id) and a gradient mobile phase profile. Gradient elution was performed at a flow rate of 0.25 mL/min. After a 5 min isocratic elution at 100% A (0.1% formic acid in water), a linear gradient to 50% A and 50% B (0.1% formic acid in acetonitrile) at 15 min was employed. Detection was performed with a DAD as well as either an FLD or a triple-quadrupole MS <span class="hlt">detector</span> in the multiple reaction monitoring mode. SLV was performed using Standard Reference Material (SRM) 3280 Multivitamin/Multimineral Tablets, being developed by the National Institute of Standards and Technology, with support by the Office of Dietary Supplements of the National Institutes of Health. Phosphate buffer (10 mM, <span class="hlt">p</span>H 2.0) extracts of the NIST SRM 3280 were analyzed by the liquid chromatographic (LC)-DAD-FLD/MS method. Following extraction, the method does not require any sample cleanup/preconcentration steps except centrifugation and filtration. PMID:19485230</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/692523-electrical-effects-plasma-damage-gan','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/692523-electrical-effects-plasma-damage-gan"><span>Electrical effects of plasma damage in <span class="hlt">p-GaN</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Cao, X.A.; Pearton, S.J.; Zhang, A.P.</p> <p>1999-10-01</p> <p>The reverse breakdown voltage of <span class="hlt">p-GaN</span> Schottky <span class="hlt">diodes</span> was used to measure the electrical effects of high density Ar or H{sub 2} plasma exposure. The near surface of the <span class="hlt">p-GaN</span> became more compensated through introduction of shallow donor states whose concentration depended on ion flux, ion energy, and ion mass. At high fluxes or energies, the donor concentration exceeded 10{sup 19}&hthinsp;cm{sup {minus}3} and produced {ital <span class="hlt">p</span>}-to-{ital <span class="hlt">n</span>} surface conversion. The damage depth was established as {approximately}400 {Angstrom} based on electrical and wet etch rate measurements. Rapid thermal annealing at 900&hthinsp;{degree}C under a <span class="hlt">N</span>{sub 2} ambient restored the initial electrical propertiesmore » of the <span class="hlt">p-GaN</span>. {copyright} {ital 1999 American Institute of Physics.}« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JPhCS.643a2068U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JPhCS.643a2068U"><span>Spectral sensitivity characteristics simulation for silicon <span class="hlt">p-i-n</span> photodiode</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Urchuk, S. U.; Legotin, S. A.; Osipov, U. V.; Elnikov, D. S.; Didenko, S. I.; Astahov, V. P.; Rabinovich, O. I.; Yaromskiy, V. P.; Kuzmina, K. A.</p> <p>2015-11-01</p> <p>In this paper the simulation results of the spectral sensitivity characteristics of silicon <span class="hlt">p-i-n</span>-photodiodes are presented. The analysis of the characteristics of the semiconductor material (the doping level, lifetime, surface recombination velocity), the construction and operation modes on the characteristics of photosensitive structures in order to optimize them was carried out.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003RScI...74.4352B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003RScI...74.4352B"><span>Laser induced fluorescence in Ar and He plasmas with a tunable <span class="hlt">diode</span> laser</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boivin, R. F.; Scime, E. E.</p> <p>2003-10-01</p> <p>A <span class="hlt">diode</span> laser based laser induced fluorescence (LIF) diagnostic that uses an inexpensive <span class="hlt">diode</span> laser system is described. This LIF diagnostic has been developed on the hot helicon experiment (HELIX) plasma device. The same <span class="hlt">diode</span> laser is used to alternatively pump Ar II and He <span class="hlt">I</span> transitions to obtain argon ion and atomic helium temperatures, respectively. The 1.5 MHz bandwidth <span class="hlt">diode</span> laser has a Littrow external cavity with a mode-hop free tuning range up to 14 GHz (≈0.021 nm) and a total power output of about 12 mW. Wavelength scanning is achieved by varying the voltage on a piezoelectric controlled grating located within the laser cavity. The fluorescence radiation is monitored with a photomultiplier <span class="hlt">detector</span>. A narrow band interference filter is used to eliminate all but the plasma radiation in the immediate vicinity of the fluorescence wavelength. Lock-in amplification is used to isolate the fluorescence signal from noise and electron-impact induced radiation. For the Ar ion, the laser tuned at 668.43 nm is used to pump the 3d 4F7/2 Ar II metastable level to the 4<span class="hlt">p</span> 4D5/2 level. The 442.60 nm fluorescence radiation between the 4<span class="hlt">p</span> 4D5/2 and the 4s 4<span class="hlt">P</span>3/2 levels is captured by the photomultiplier tube. For atomic He, the laser is tuned at 667.82 nm to pump a fraction of the electron population from the 21<span class="hlt">P</span> state to the 31D upper level. Although the 21<span class="hlt">P</span> level is not a metastable, the close proximity of 21S metastable makes this new He <span class="hlt">I</span> LIF scheme possible. In this scheme, a fraction of the laser-excited electrons undergo collisional excitation transfer from the 31D to the 31<span class="hlt">P</span> level. In turn, the 31<span class="hlt">P</span> state decays to the metastable 21S by emitting 501.57 nm fluorescence photons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013SPIE.8626E..0LB','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013SPIE.8626E..0LB"><span>Engineering future light emitting <span class="hlt">diodes</span> and photovoltaics with inexpensive materials: Integrating ZnO and Si into Ga<span class="hlt">N</span>-based devices</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bayram, C.; Shiu, K. T.; Zhu, Y.; Cheng, C. W.; Sadana, D. K.; Teherani, F. H.; Rogers, D. J.; Sandana, V. E.; Bove, P.; Zhang, Y.; Gautier, S.; Cho, C.-Y.; Cicek, E.; Vashaei, Z.; McClintock, R.; Razeghi, M.</p> <p>2013-03-01</p> <p>Indium Gallium Nitride (InGa<span class="hlt">N</span>) based PV have the best fit to the solar spectrum of any alloy system and emerging LED lighting based on InGa<span class="hlt">N</span> technology and has the potential to reduce energy consumption by nearly one half while enabling significant carbon emission reduction. However, getting the maximum benefit from Ga<span class="hlt">N</span> <span class="hlt">diode</span> -based PV and LEDs will require wide-scale adoption. A key bottleneck for this is the device cost, which is currently dominated by the substrate (<span class="hlt">i</span>.e. sapphire) and the epitaxy (<span class="hlt">i</span>.e. Ga<span class="hlt">N</span>). This work investigates two schemes for reducing such costs. First, we investigated the integration of Zinc Oxide (ZnO) in InGa<span class="hlt">N</span>-based <span class="hlt">diodes</span>. (Successful growth of Ga<span class="hlt">N</span> on ZnO template layers (on sapphire) was illustrated. These templates can then be used as sacrificial release layers for chemical lift-off. Such an approach provides an alternative to laser lift-off for the transfer of Ga<span class="hlt">N</span> to substrates with a superior cost-performance profile, plus an added advantage of reclaiming the expensive single-crystal sapphire. It was also illustrated that substitution of low temperature <span class="hlt">n</span>-type ZnO for <span class="hlt">n-GaN</span> layers can combat indium leakage from InGa<span class="hlt">N</span> quantum well active layers in inverted <span class="hlt">p-n</span> junction structures. The ZnO overlayers can also double as transparent contacts with a nanostructured surface which enhances light in/out coupling. Thus ZnO was confirmed to be an effective Ga<span class="hlt">N</span> substitute which offers added flexibility in device design and can be used in order to simultaneously reduce the epitaxial cost and boost the device performance. Second, we investigated the use of Ga<span class="hlt">N</span> templates on patterned Silicon (100) substrates for reduced substrate cost LED applications. Controlled local metal organic chemical vapor deposition epitaxy of cubic phase Ga<span class="hlt">N</span> with on-axis Si(100) substrates was illustrated. Scanning electron microscopy and transmission electron microscopy techniques were used to investigate uniformity and examine the defect structure in the Ga<span class="hlt">N</span>. Our</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22164066','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22164066"><span>Dual-functional on-chip AlGaAs/GaAs Schottky <span class="hlt">diode</span> for RF power detection and low-power rectenna applications.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hashim, Abdul Manaf; Mustafa, Farahiyah; Rahman, Shaharin Fadzli Abd; Rahman, Abdul Rahim Abdul</p> <p>2011-01-01</p> <p>A Schottky <span class="hlt">diode</span> has been designed and fabricated on an <span class="hlt">n</span>-AlGaAs/GaAs high-electron-mobility-transistor (HEMT) structure. Current-voltage (<span class="hlt">I</span>-V) measurements show good device rectification, with a Schottky barrier height of 0.4349 eV for Ni/Au metallization. The differences between the Schottky barrier height and the theoretical value (1.443 eV) are due to the fabrication process and smaller contact area. The RF signals up to 1 GHz are rectified well by the fabricated Schottky <span class="hlt">diode</span> and a stable DC output voltage is obtained. The increment ratio of output voltage vs input power is 0.2 V/dBm for all tested frequencies, which is considered good enough for RF power detection. Power conversion efficiency up to 50% is obtained at frequency of 1 GHz and input power of 20 dBm with series connection between <span class="hlt">diode</span> and load, which also shows the device's good potential as a rectenna device with further improvement. The fabricated <span class="hlt">n</span>-AlGaAs/GaAs Schottky <span class="hlt">diode</span> thus provides a conduit for breakthrough designs for RF power <span class="hlt">detectors</span>, as well as ultra-low power on-chip rectenna device technology to be integrated in nanosystems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28789045','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28789045"><span>Fully integrated free-running InGaAs/In<span class="hlt">P</span> single-photon <span class="hlt">detector</span> for accurate lidar applications.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yu, Chao; Shangguan, Mingjia; Xia, Haiyun; Zhang, Jun; Dou, Xiankang; Pan, Jian-Wei</p> <p>2017-06-26</p> <p>We present a fully integrated InGaAs/In<span class="hlt">P</span> negative feedback avalanche <span class="hlt">diode</span> (NFAD) based free-running single-photon <span class="hlt">detector</span> (SPD) designed for accurate lidar applications. A free-piston Stirling cooler is used to cool down the NFAD with a large temperature range, and an active hold-off circuit implemented in a field programmable gate array is applied to further suppress the afterpulsing contribution. The key parameters of the free-running SPD including photon detection efficiency (PDE), dark count rate (DCR), afterpulse probability, and maximum count rate (MCR) are dedicatedly optimized for lidar application in practice. We then perform a field experiment using a Mie lidar system with 20 kHz pulse repetition frequency to compare the performance between the free-running InGaAs/In<span class="hlt">P</span> SPD and a commercial superconducting nanowire single-photon <span class="hlt">detector</span> (SNSPD). Our <span class="hlt">detector</span> exhibits good performance with 1.6 Mcps MCR (0.6 μs hold-off time), 10% PDE, 950 cps DCR, and 18% afterpulse probability over 50 μs period. Such performance is worse than the SNSPD with 60% PDE and 300 cps DCR. However, after performing a specific algorithm that we have developed for afterpulse and count rate corrections, the lidar system performance in terms of range-corrected signal (Pr 2 ) distribution using our SPD agrees very well with the result using the SNSPD, with only a relative error of ∼2%. Due to the advantages of low-cost and small size of InGaAs/In<span class="hlt">P</span> NFADs, such <span class="hlt">detector</span> provides a practical solution for accurate lidar applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27929510','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27929510"><span>Deriving <span class="hlt">detector</span>-specific correction factors for rectangular small fields using a scintillator <span class="hlt">detector</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Qin, Yujiao; Zhong, Hualiang; Wen, Ning; Snyder, Karen; Huang, Yimei; Chetty, Indrin J</p> <p>2016-11-08</p> <p>The goal of this study was to investigate small field output factors (OFs) for flat-tening filter-free (FFF) beams on a dedicated stereotactic linear accelerator-based system. From this data, the collimator exchange effect was quantified, and <span class="hlt">detector</span>-specific correction factors were generated. Output factors for 16 jaw-collimated small fields (from 0.5 to 2 cm) were measured using five different <span class="hlt">detectors</span> including an ion chamber (CC01), a stereotactic field <span class="hlt">diode</span> (SFD), a <span class="hlt">diode</span> <span class="hlt">detector</span> (Edge), Gafchromic film (EBT3), and a plastic scintillator <span class="hlt">detector</span> (PSD, W1). Chamber, <span class="hlt">diodes</span>, and PSD measurements were performed in a Wellhofer water tank, while films were irradiated in solid water at 100 cm source-to-surface distance and 10 cm depth. The collimator exchange effect was quantified for rectangular fields. Monte Carlo (MC) simulations of the measured configurations were also performed using the EGSnrc/DOSXYZnrc code. Output factors measured by the PSD and verified against film and MC calculations were chosen as the benchmark measurements. Compared with plastic scintillator <span class="hlt">detector</span> (PSD), the small volume ion chamber (CC01) underestimated output factors by an average of -1.0% ± 4.9% (max. = -11.7% for 0.5 × 0.5 cm2 square field). The stereotactic <span class="hlt">diode</span> (SFD) overestimated output factors by 2.5% ± 0.4% (max. = 3.3% for 0.5 × 1 cm2 rectangular field). The other <span class="hlt">diode</span> <span class="hlt">detector</span> (Edge) also overestimated the OFs by an average of 4.2% ± 0.9% (max. = 6.0% for 1 × 1 cm2 square field). Gafchromic film (EBT3) measure-ments and MC calculations agreed with the scintillator <span class="hlt">detector</span> measurements within 0.6% ± 1.8% and 1.2% ± 1.5%, respectively. Across all the X and Y jaw combinations, the average collimator exchange effect was computed: 1.4% ± 1.1% (CC01), 5.8% ± 5.4% (SFD), 5.1% ± 4.8% (Edge <span class="hlt">diode</span>), 3.5% ± 5.0% (Monte Carlo), 3.8% ± 4.7% (film), and 5.5% ± 5.1% (PSD). Small field <span class="hlt">detectors</span> should be used with caution with a clear understanding of their</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16633580','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16633580"><span>Low-picomolar limits of detection using high-power light-emitting <span class="hlt">diodes</span> for fluorescence.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>de Jong, Ebbing P; Lucy, Charles A</p> <p>2006-05-01</p> <p>Fluorescence <span class="hlt">detectors</span> are ever more frequently being used with light-emitting <span class="hlt">diodes</span> (LEDs) as the light source. Technological advances in the solid-state lighting industry have produced LEDs which are also suitable tools in analytical measurements. LEDs are now available which deliver 700 mW of radiometric power. While this greater light power can increase the fluorescence signal, it is not trivial to make proper use of this light. This new generation of LEDs has a large emitting area and a highly divergent beam. This presents a classic problem in optics where one must choose between either a small focused light spot, or high light collection efficiency. We have selected for light collection efficiency, which yields a light spot somewhat larger than the emitting area of the LED. This light is focused onto a flow cell. Increasing the <span class="hlt">detector</span> cell internal diameter (<span class="hlt">i</span>.d.) produces gains in (sensitivity)3. However, since the <span class="hlt">detector</span> cell <span class="hlt">i</span>.d. is smaller than the LED spot size, scattering of excitation light towards the <span class="hlt">detector</span> remains a significant source of background signal. This can be minimized through the use of spectral filters and spatial filters in the form of pinholes. The <span class="hlt">detector</span> produced a limit of detection (LOD) of 3 <span class="hlt">p</span>M, which is roughly three orders of magnitude lower than other reports of LED-based fluorescence <span class="hlt">detectors</span>. Furthermore, this LOD comes within a factor of six of much more expensive laser-based fluorescence systems. This <span class="hlt">detector</span> has been used to monitor a separation from a gel filtration column of fluorescently labeled BSA from residual labeling reagent. The LOD of fluorescently labeled BSA is 25 <span class="hlt">p</span>M.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19800011329','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19800011329"><span>Studies of silicon <span class="hlt">p-n</span> junction solar cells</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Neugroschel, A.; Lindholm, F. A.</p> <p>1979-01-01</p> <p>To provide theoretical support for investigating different ways to obtain high open-circuit voltages in <span class="hlt">p-n</span> junction silicon solar cells, an analytical treatment of heavily doped transparent-emitter devices is presented that includes the effects of bandgap narrowing, Fermi-Dirac statistics, a doping concentration gradient, and a finite surface recombination velocity at the emitter surface. Topics covered include: (1) experimental determination of bandgap narrowing in the emitter of silicon <span class="hlt">p-n</span> junction devices; (2) heavily doped transparent regions in junction solar cells, <span class="hlt">diodes</span>, and transistors; (3) high-low-emitter solar cell; (4) determination of lifetimes and recombination currents in <span class="hlt">p-n</span> junction solar cells; (5) MOS and oxide-charged-induced BSF solar cells; and (6) design of high efficiency solar cells for space and terrestrial applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JAP...111i4513F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JAP...111i4513F"><span>Thermal characterization of Ga<span class="hlt">N</span>-based laser <span class="hlt">diodes</span> by forward-voltage method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Feng, M. X.; Zhang, S. M.; Jiang, D. S.; Liu, J. P.; Wang, H.; Zeng, C.; Li, Z. C.; Wang, H. B.; Wang, F.; Yang, H.</p> <p>2012-05-01</p> <p>An expression of the relation between junction temperature and forward voltage common for both Ga<span class="hlt">N</span>-based laser <span class="hlt">diodes</span> (LDs) and light emitting <span class="hlt">diodes</span> is derived. By the expression, the junction temperature of Ga<span class="hlt">N</span>-based LDs emitting at 405 nm was measured at different injection current and compared with the result of micro-Raman spectroscopy, showing that the expression is reasonable. In addition, the activation energy of Mg in AlGa<span class="hlt">N/GaN</span> superlattice layers is obtained based on the temperature dependence of forward voltage.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820010124','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820010124"><span>Moderate temperature <span class="hlt">detector</span> development</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Marciniec, J. W.; Briggs, R. J.; Sood, A. K.</p> <p>1981-01-01</p> <p><span class="hlt">P</span>-side backside reflecting constant, photodiode characterization, and photodiode diffusion and G-R currents were investigated in an effort to develop an 8 m to 12 m infrared quantum <span class="hlt">detector</span> using mercury cadmium telluride. Anodization, phosphorus implantation, and the graded band gap concept were approaches considered for backside formation. Variable thickness <span class="hlt">diodes</span> were fabricated with a back surface anodic oxide to investigate the effect of this surface preparation on the diffusion limited zero bias impedance. A modeling technique was refined to thoroughly model <span class="hlt">diode</span> characteristics. Values for the surface recombination velocity in the depletion region were obtained. These values were improved by implementing better surface damage removal techniques.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9354E..0QN','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9354E..0QN"><span>AlGaIn<span class="hlt">N</span> laser <span class="hlt">diode</span> technology for free-space telecom applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Najda, S. P.; Perlin, P.; Suski, T.; Marona, L.; Boćkowski, M.; Leszczyński, M.; Wisniewski, P.; Czernecki, R.; Kucharski, R.; Targowski, G.; Watson, S.; Kelly, A. E.; Watson, M. A.; Blanchard, P.; White, H.</p> <p>2015-03-01</p> <p>The AlGaIn<span class="hlt">N</span> material system allows for laser <span class="hlt">diodes</span> to be fabricated over a very wide range of wavelengths from u.v., ~380nm, to the visible ~530nm, by tuning the indium content of the laser GaIn<span class="hlt">N</span> quantum well. We consider the suitability of AlGaIn<span class="hlt">N</span> laser <span class="hlt">diode</span> technology for free space laser communication, both airborne links and underwater telecom applications, mainly for defense and oil and gas industries.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011InPhT..54..252P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011InPhT..54..252P"><span>Passivation of long-wave infrared InAs/GaSb strained layer superlattice <span class="hlt">detectors</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Plis, E.; Kutty, M. N.; Myers, S.; Kim, H. S.; Gautam, N.; Dawson, L. R.; Krishna, S.</p> <p>2011-05-01</p> <p>We have investigated various passivation techniques for type-II InAs/GaSb strained layer superlattice (SLS) <span class="hlt">detectors</span> with <span class="hlt">p-i-n</span> and PbIb<span class="hlt">N</span> designs with a 100%-cut-off wavelength of ˜12 μm at 77 K. The passivation schemes include dielectric deposition (silicon nitride (Si<span class="hlt">N</span> x), silicon dioxide (SiO 2), photoresist (SU-8)), chalcogenide treatments (zinc sulfide (ZnS), ammonium sulfide [(NH 4) 2S]), and electrochemical sulphur deposition. [(NH 4) 2S] passivation and electrochemical sulphur passivation (ECP) showed the better performances, improving the dark current density by factors of 200 and 25 (<span class="hlt">p-i-n</span> <span class="hlt">detector</span>) and ˜3 and 54 (PbIb<span class="hlt">N</span> <span class="hlt">detector</span>), respectively ( T = 77 K, -0.1 V of applied bias). The specific detectivity D* was improved by a factor of 2 and by an order of magnitude for (NH 4) 2S and ECP passivated PbIb<span class="hlt">N</span> <span class="hlt">detectors</span>, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10121E..09T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10121E..09T"><span>Intracavity double <span class="hlt">diode</span> structures with GaIn<span class="hlt">P</span> barrier layers for thermophotonic cooling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tiira, Jonna; Radevici, Ivan; Haggren, Tuomas; Hakkarainen, Teemu; Kivisaari, Pyry; Lyytikäinen, Jari; Aho, Arto; Tukiainen, Antti; Guina, Mircea; Oksanen, Jani</p> <p>2017-02-01</p> <p>Optical cooling of semiconductors has recently been demonstrated both for optically pumped CdS nanobelts and for electrically injected GaInAsSb LEDs at very low powers. To enable cooling at larger power and to understand and overcome the main obstacles in optical cooling of conventional semiconductor structures, we study thermophotonic (TPX) heat transport in cavity coupled light emitters. Our structures consist of a double heterojunction (DHJ) LED with a GaAs active layer and a corresponding DHJ or a <span class="hlt">p-n</span>-homojunction photodiode, enclosed within a single semiconductor cavity to eliminate the light extraction challenges. Our presently studied double <span class="hlt">diode</span> structures (DDS) use GaIn<span class="hlt">P</span> barriers around the GaAs active layer instead of the AlGaAs barriers used in our previous structures. We characterize our updated double <span class="hlt">diode</span> structures by four point probe IV- measurements and measure how the material modifications affect the recombination parameters and coupling quantum efficiencies in the structures. The coupling quantum efficiency of the new devices with InGa<span class="hlt">P</span> barrier layers is found to be approximately 10 % larger than for the structures with AlGaAs barriers at the point of maximum efficiency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19720009509','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19720009509"><span>Development of reverse biased <span class="hlt">p-n</span> junction electron emission</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fowler, P.; Muly, E. C.</p> <p>1971-01-01</p> <p>A cold cathode emitter of hot electrons for use as a source of electrons in vacuum gauges and mass spectrometers was developed using standard Norton electroluminescent silicon carbide <span class="hlt">p-n</span> <span class="hlt">diodes</span> operated under reverse bias conditions. Continued development including variations in the geometry of these emitters was carried out such that emitters with an emission efficiency (emitted current/junction current) as high as 3 x 10-0.00001 were obtained. Pulse measurements of the <span class="hlt">diode</span> characteristics were made and showed that higher efficiency can be attained under pulse conditions probably due to the resulting lower temperatures resulting from such operation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920041397&hterms=tunnel+diodes&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dtunnel%2Bdiodes','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920041397&hterms=tunnel+diodes&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dtunnel%2Bdiodes"><span>Characterization of resonant tunneling <span class="hlt">diodes</span> for microwave and millimeter-wave detection</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mehdi, I.; East, J. R.; Haddad, G. I.</p> <p>1991-01-01</p> <p>The authors report on the direct detection capabilities of resonant tunneling <span class="hlt">diodes</span> in the 10-100 GHz range. An open circuit voltage sensitivity of 1750 mV/mW (in Ka-band) was measured. This is higher than the sensitivity of comparatively based commercially available solid-state <span class="hlt">detectors</span>. The <span class="hlt">detector</span> properties are a strong function of <span class="hlt">diode</span> bias and the measured tangential signal sensitivity (-32 dBm at Ka-band with 1-MHz bandwidth) and the dynamic range (25 dB) of the <span class="hlt">diode</span> are smaller compared to other solid-state <span class="hlt">detectors</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ChPhB..25h8505Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ChPhB..25h8505Q"><span>Improved performance of near UV light-emitting <span class="hlt">diodes</span> with a composition-graded <span class="hlt">p-AlGaN</span> irregular sawtooth electron-blocking layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Qin, Ping; Song, Wei-Dong; Hu, Wen-Xiao; Zhang, Yuan-Wen; Zhang, Chong-Zhen; Wang, Ru-Peng; Zhao, Liang-Liang; Xia, Chao; Yuan, Song-Yang; Yin, Yi-an; Li, Shu-Ti; Su, Shi-Chen</p> <p>2016-08-01</p> <p>We investigate the performances of the near-ultraviolet (about 350 nm-360 nm) light-emitting <span class="hlt">diodes</span> (LEDs) each with specifically designed irregular sawtooth electron blocking layer (EBL) by using the APSYS simulation program. The internal quantum efficiencies (IQEs), light output powers, carrier concentrations in the quantum wells, energy-band diagrams, and electrostatic fields are analyzed carefully. The results indicate that the LEDs with composition-graded <span class="hlt">p</span>-Al x Ga1-x <span class="hlt">N</span> irregular sawtooth EBLs have better performances than their counterparts with stationary component <span class="hlt">p-AlGaN</span> EBLs. The improvements can be attributed to the improved polarization field in EBL and active region as well as the alleviation of band bending in the EBL/<span class="hlt">p-AlGaN</span> interface, which results in less electron leakage and better hole injection efficiency, thus reducing efficiency droop and enhancing the radiative recombination rate. Project supported by the National Natural Science Foundation of China (Grant Nos. 11474105 and 51172079), the Science and Technology Program of Guangdong Province, China (Grant Nos. 2015B090903078 and 2015B010105011), the Program for Changjiang Scholars and Innovative Research Team in University, China (Grant No. IRT13064), the Science and Technology Project of Guangzhou City, China (Grant No. 201607010246), and the Science and Technology Planning Project of Guangdong Province, China (Grant No. 2015A010105025).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28489398','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28489398"><span>Simultaneously Enhancing Light Emission and Suppressing Efficiency Droop in Ga<span class="hlt">N</span> Microwire-Based Ultraviolet Light-Emitting <span class="hlt">Diode</span> by the Piezo-Phototronic Effect.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Xingfu; Peng, Wenbo; Yu, Ruomeng; Zou, Haiyang; Dai, Yejing; Zi, Yunlong; Wu, Changsheng; Li, Shuti; Wang, Zhong Lin</p> <p>2017-06-14</p> <p>Achievement of <span class="hlt">p-n</span> homojuncted Ga<span class="hlt">N</span> enables the birth of III-nitride light emitters. Owing to the wurtzite-structure of Ga<span class="hlt">N</span>, piezoelectric polarization charges present at the interface can effectively control/tune the optoelectric behaviors of local charge-carriers (<span class="hlt">i</span>.e., the piezo-phototronic effect). Here, we demonstrate the significantly enhanced light-output efficiency and suppressed efficiency droop in Ga<span class="hlt">N</span> microwire (MW)-based <span class="hlt">p-n</span> junction ultraviolet light-emitting <span class="hlt">diode</span> (UV LED) by the piezo-phototronic effect. By applying a -0.12% static compressive strain perpendicular to the <span class="hlt">p-n</span> junction interface, the relative external quantum efficiency of the LED is enhanced by over 600%. Furthermore, efficiency droop is markedly reduced from 46.6% to 7.5% and corresponding droop onset current density shifts from 10 to 26.7 A cm -2 . Enhanced electrons confinement and improved holes injection efficiency by the piezo-phototronic effect are revealed and theoretically confirmed as the physical mechanisms. This study offers an unconventional path to develop high efficiency, strong brightness and high power III-nitride light sources.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SuScT..31c5011S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SuScT..31c5011S"><span>Nb<span class="hlt">N</span> single-photon <span class="hlt">detectors</span> with saturated dependence of quantum efficiency</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smirnov, Konstantin; Divochiy, Alexander; Vakhtomin, Yury; Morozov, Pavel; Zolotov, Philipp; Antipov, Andrey; Seleznev, Vitaliy</p> <p>2018-07-01</p> <p>The possibility of creating Nb<span class="hlt">N</span> superconducting single-photon <span class="hlt">detectors</span> with saturated dependence of quantum efficiency (QE) versus normalized bias current was investigated. It was shown that the saturation increases for the <span class="hlt">detectors</span> based on finer films with a lower value of R s300/R s20. The decreasing of R s300/R s20 was related to the increasing influence of quantum corrections to conductivity of superconductors and, in turn, to the decrease of the electron diffusion coefficient. The best samples have a constant value of system QE 94% at <span class="hlt">I</span> b /<span class="hlt">I</span> c ∼ 0.8 and wavelength 1310 nm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5458876','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5458876"><span>Origin of the Electroluminescence from Annealed-ZnO/Ga<span class="hlt">N</span> Heterojunction Light-Emitting <span class="hlt">Diodes</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Hsu, Kai-Chiang; Hsiao, Wei-Hua; Lee, Ching-Ting; Chen, Yan-Ting; Liu, Day-Shan</p> <p>2015-01-01</p> <p>This paper addressed the effect of post-annealed treatment on the electroluminescence (EL) of an <span class="hlt">n-ZnO/p-GaN</span> heterojunction light-emitting <span class="hlt">diode</span> (LED). The bluish light emitted from the 450 °C-annealed LED became reddish as the LED annealed at a temperature of 800 °C under vacuum atmosphere. The origins of the light emission for these LEDs annealed at various temperatures were studied using measurements of electrical property, photoluminescence, and Auger electron spectroscopy (AES) depth profiles. A blue-violet emission located at 430 nm was associated with intrinsic transitions between the bandgap of <span class="hlt">n</span>-ZnO and <span class="hlt">p-GaN</span>, the green-yellow emission at 550 nm mainly originating from the deep-level transitions of native defects in the <span class="hlt">n</span>-ZnO and <span class="hlt">p-GaN</span> surfaces, and the red emission at 610 nm emerging from the Ga-O interlayer due to interdiffusion at the <span class="hlt">n-ZnO/p-GaN</span> interface. The above-mentioned emissions also supported the EL spectra of LEDs annealed at 700 °C under air, nitrogen, and oxygen atmospheres, respectively. PMID:28793675</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28793675','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28793675"><span>Origin of the Electroluminescence from Annealed-ZnO/Ga<span class="hlt">N</span> Heterojunction Light-Emitting <span class="hlt">Diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hsu, Kai-Chiang; Hsiao, Wei-Hua; Lee, Ching-Ting; Chen, Yan-Ting; Liu, Day-Shan</p> <p>2015-11-16</p> <p>This paper addressed the effect of post-annealed treatment on the electroluminescence (EL) of an <span class="hlt">n</span> -ZnO/ <span class="hlt">p</span> -Ga<span class="hlt">N</span> heterojunction light-emitting <span class="hlt">diode</span> (LED). The bluish light emitted from the 450 °C-annealed LED became reddish as the LED annealed at a temperature of 800 °C under vacuum atmosphere. The origins of the light emission for these LEDs annealed at various temperatures were studied using measurements of electrical property, photoluminescence, and Auger electron spectroscopy (AES) depth profiles. A blue-violet emission located at 430 nm was associated with intrinsic transitions between the bandgap of <span class="hlt">n</span> -ZnO and <span class="hlt">p</span> -Ga<span class="hlt">N</span>, the green-yellow emission at 550 nm mainly originating from the deep-level transitions of native defects in the <span class="hlt">n</span> -ZnO and <span class="hlt">p</span> -Ga<span class="hlt">N</span> surfaces, and the red emission at 610 nm emerging from the Ga-O interlayer due to interdiffusion at the <span class="hlt">n</span> -ZnO/ <span class="hlt">p</span> -Ga<span class="hlt">N</span> interface. The above-mentioned emissions also supported the EL spectra of LEDs annealed at 700 °C under air, nitrogen, and oxygen atmospheres, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22611717-enhancement-performance-gan-impatt-diodes-negative-differential-mobility','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22611717-enhancement-performance-gan-impatt-diodes-negative-differential-mobility"><span>Enhancement of the performance of Ga<span class="hlt">N</span> IMPATT <span class="hlt">diodes</span> by negative differential mobility</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Dai, Yang; Yang, Lin’an, E-mail: layang@xidian.edu.cn; Chen, Qing</p> <p>2016-05-15</p> <p>A theoretical analysis of high-efficiency punch-through operation Ga<span class="hlt">N</span>-based terahertz IMPATT <span class="hlt">diodes</span> has been carried out in this paper. It is shown that the negative differential mobility (NDM) characteristics of Ga<span class="hlt">N</span> coupled with the space charge effect acting as a self-feedback system can markedly increase the drift velocity of injection carriers, and thereby enhance <span class="hlt">diode</span> performance under appropriate external RF voltage. The behavior of traveling electrons in the transit zone is investigated in detail. It is found that the IMPATT <span class="hlt">diode</span> with a punch-through structure operating in the NDM mode exhibits superior characteristics compared with the equivalent <span class="hlt">diode</span> operating in themore » Si-like constant mobility mode. In particular, the NDM-mode <span class="hlt">diode</span> can tolerate a larger RF voltage swing than that operating in constant mobility mode. Numerical simulation results reveal that the highest efficiency of 26.6% and maximum RF power of 2.29 W can be achieved for the NDM-mode <span class="hlt">diode</span> at a frequency of 225 GHz. A highest efficiency of 19.0% and maximum RF power of 1.58 W are obtained for the <span class="hlt">diode</span> with constant mobility.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27891634','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27891634"><span>Sensitive determination of sulfonamides in environmental water by capillary electrophoresis coupled with both silvering detection window and in-capillary optical fiber light-emitting <span class="hlt">diode</span>-induced fluorescence <span class="hlt">detector</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ji, Hongyun; Wu, Yu; Duan, Zhijuan; Yang, Feng; Yuan, Hongyan; Xiao, Dan</p> <p>2017-02-01</p> <p>A new <span class="hlt">detector</span>, silvering detection window and in-capillary optical fiber light-emitting <span class="hlt">diode</span>-induced fluorescence <span class="hlt">detector</span> (SDW-ICOF-LED-IFD), is introduced for capillary electrophoresis (CE). The strategy of the work was that half surface of the detection window was coated with silver mirror, which could reflect the undetected fluorescence to the photomultiplier tube to be detected, consequently enhancing the detection sensitivity. Sulfonamides (SAs) are important antibiotics that achieved great applications in many fields. However, they pose a serious threat on the environment and human health when they enter into the environment. The SDW-ICOF-LED-IFD-CE system was used to determine fluorescein isothiocyanate (FITC)-labeled sulfadoxine (SDM), sulfaguanidine (SGD) and sulfamonomethoxine sodium (SMM-Na) in environmental water. The detection results obtained by the SDW-ICOF-LED-IFD-CE system were compared to those acquired by the CE with in-capillary optical fiber light-emitting <span class="hlt">diode</span>-induced fluorescence detection (ICOF-LED-IFD-CE). The limits of detection (LODs) of SDW-ICOF-LED-IFD-CE and ICOF-LED-IFD-CE were 1.0-2.0 <span class="hlt">n</span>M and 2.5-7.7 <span class="hlt">n</span>M (S/<span class="hlt">N</span> = 3), respectively. The intraday (<span class="hlt">n</span> = 6) and interday (<span class="hlt">n</span> = 6) precision of migration time and corresponding peak area for both types of CE were all less than 0.86% and 3.68%, respectively. The accuracy of the proposed method was judged by employing standard addition method, and recoveries obtained were in the range of 92.5-102.9%. The results indicated that the sensitivity of the SDW-ICOF-LED-IFD-CE system was improved, and that its reproducibility and accuracy were satisfactory. It was successfully applied to analyze SAs in environmental water. © 2016 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ChPhB..22h6803W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ChPhB..22h6803W"><span>Light-extraction efficiency and forward voltage in Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> with different patterns of V-shaped pits</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Min-Shuai; Huang, Xiao-Jing</p> <p>2013-08-01</p> <p>We present a new method of making a textured V-pit surface for improving the light extraction efficiency in Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> and compare it with the usual low-temperature method for <span class="hlt">p-GaN</span> V-pits. Three types of Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> (LEDs) with surface V-pits in different densities and regions were grown by metal—organic chemical vapor deposition. We achieved the highest output power and lowest forward voltage values with the <span class="hlt">p-InGaN</span> V-pit LED. The V-pits enhanced the light output power values by 1.45 times the values of the conventional LED owing to an enhancement of the light scattering probability and an effective reduction of Mg-acceptor activation energy. Moreover, this new technique effectively solved the higher forward voltage problem of the usual V-pit LED.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018OptMa..81..109L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018OptMa..81..109L"><span>Surface morphological, structural, electrical and optical properties of Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> using submicron-scaled Ag islands and ITO thin films</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, Young-Woong; Reddy, M. Siva Pratap; Kim, Bo-Myung; Park, Chinho</p> <p>2018-07-01</p> <p>An ITO-Ag islands complex as a new transparent conducting electrode (TCE) structure (on the 5 nm-thick <span class="hlt">p-InGaN</span>/90 nm-thick <span class="hlt">p-GaN</span>) for achieving high-performance and more reliable Ga<span class="hlt">N</span>-based LEDs were fabricated. A normal LED with a conventional ITO TCE was also compared. The surface morphological, structural, electrical and optical properties of fabricated Ga<span class="hlt">N</span>-based light-emitting <span class="hlt">diodes</span> using a complex electrode of submicron-scaled Ag islands and ITO thin films are explored by X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), current-voltage (<span class="hlt">I</span>-V) and output power-current (L-<span class="hlt">I</span>) techniques. Surface morphology investigations revealed Ag islands formed uniformly on the <span class="hlt">p-InGaN/p-GaN</span> surface during rapid thermal annealing at 400 °C for 1 min in <span class="hlt">N</span>2 ambient. The ohmic properties and overall device-performance of the suggested contact and device structures were superior to those in the conventional ITO contact and normal ITO LED structures. Based on the results of XRD and XPS measurements, the formation of the intermetallic gallide phases (AgGa) is responsible for better performance characteristics of the ITO-Ag islands device. The significant improvements are described in terms of the conducting bridge influence, highly effective micro-mirror effect, and wider photon window via the roughened structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApPhL.109r3505K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApPhL.109r3505K"><span>High current density 2D/3D MoS2/Ga<span class="hlt">N</span> Esaki tunnel <span class="hlt">diodes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krishnamoorthy, Sriram; Lee, Edwin W.; Lee, Choong Hee; Zhang, Yuewei; McCulloch, William D.; Johnson, Jared M.; Hwang, Jinwoo; Wu, Yiying; Rajan, Siddharth</p> <p>2016-10-01</p> <p>The integration of two-dimensional materials such as transition metal dichalcogenides with bulk semiconductors offer interesting opportunities for 2D/3D heterojunction-based device structures without any constraints of lattice matching. By exploiting the favorable band alignment at the Ga<span class="hlt">N</span>/MoS2 heterojunction, an Esaki interband tunnel <span class="hlt">diode</span> is demonstrated by transferring large area Nb-doped, <span class="hlt">p</span>-type MoS2 onto heavily <span class="hlt">n</span>-doped Ga<span class="hlt">N</span>. A peak current density of 446 A/cm2 with repeatable room temperature negative differential resistance, peak to valley current ratio of 1.2, and minimal hysteresis was measured in the MoS2/Ga<span class="hlt">N</span> non-epitaxial tunnel <span class="hlt">diode</span>. A high current density of 1 kA/cm2 was measured in the Zener mode (reverse bias) at -1 V bias. The Ga<span class="hlt">N</span>/MoS2 tunnel junction was also modeled by treating MoS2 as a bulk semiconductor, and the electrostatics at the 2D/3D interface was found to be crucial in explaining the experimentally observed device characteristics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920063383&hterms=tunneling+current&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dtunneling%2Bcurrent','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920063383&hterms=tunneling+current&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dtunneling%2Bcurrent"><span>A model for the trap-assisted tunneling mechanism in diffused <span class="hlt">n-p</span> and implanted <span class="hlt">n(+)-p</span> HgCdTe photodiodes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rosenfeld, David; Bahir, Gad</p> <p>1992-01-01</p> <p>This paper presents a theoretical model for the trap-assisted tunneling process in diffused <span class="hlt">n-on-p</span> and implanted <span class="hlt">n(+)-on-p</span> HgCdTe photodiodes. The model describes the connection between the leakage current associated with the traps and the trap characteristics: concentration, energy level, and capture cross sections. It is observed that the above two types of <span class="hlt">diodes</span> differ the voltage dependence of the trap-assisted tunneling current and dynamic resistance. The model takes this difference into account and offers an explanation of the phenomenon. The good fit between measured and calculated dc characteristics of the photodiodes supports the validity of the model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920023735&hterms=tunneling+current&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dtunneling%2Bcurrent','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920023735&hterms=tunneling+current&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dtunneling%2Bcurrent"><span>A model for the trap-assisted tunneling mechanism in diffused <span class="hlt">n-p</span> and implanted <span class="hlt">n(+)-p</span> HgCdTe photodiodes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rosenfeld, David; Bahir, Gad</p> <p>1992-01-01</p> <p>A theoretical model for the trap-assisted tunneling process in diffused <span class="hlt">n-on-p</span> and implanted <span class="hlt">n(+)-on-p</span> HgCdTe photodiodes is presented. The model describes the traps and the trap characteristics: concentration, energy level, and capture cross sections. We have observed that the above two types of <span class="hlt">diodes</span> differ in the voltage dependence of the trap-assisted tunneling current and dynamic resistance. Our model takes this difference into account and offers an explanation of the phenomenon. The good fit between measured and calculated DC characteristics of the photodiodes (for medium and high reverse bias and for temperatures from 65 to 140 K) supports the validity of the model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=%22light-emitting+diode%22+OR+lighting&pg=5&id=EJ536669','ERIC'); return false;" href="https://eric.ed.gov/?q=%22light-emitting+diode%22+OR+lighting&pg=5&id=EJ536669"><span>Demonstrating the Light-Emitting <span class="hlt">Diode</span>.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Johnson, David A.</p> <p>1995-01-01</p> <p>Describes a simple inexpensive circuit which can be used to quickly demonstrate the basic function and versatility of the solid state <span class="hlt">diode</span>. Can be used to demonstrate the light-emitting <span class="hlt">diode</span> (LED) as a light emitter, temperature sensor, light <span class="hlt">detector</span> with both a linear and logarithmic response, and charge storage device. (JRH)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9649E..0PN','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9649E..0PN"><span>AlGaIn<span class="hlt">N</span> laser <span class="hlt">diode</span> technology and systems for defence and security applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Najda, Stephen P.; Perlin, Piotr; Suski, Tadek; Marona, Lujca; Boćkowski, Mike; Leszczyński, Mike; Wisniewski, Przemek; Czernecki, Robert; Kucharski, Robert; Targowski, Grzegorz; Watson, Scott; Kelly, Antony E.</p> <p>2015-10-01</p> <p>AlGaIn<span class="hlt">N</span> laser <span class="hlt">diodes</span> is an emerging technology for defence and security applications such as underwater communications and sensing, atomic clocks and quantum information. The AlGaIn<span class="hlt">N</span> material system allows for laser <span class="hlt">diodes</span> to be fabricated over a very wide range of wavelengths from u.v., ~380nm, to the visible ~530nm, by tuning the indium content of the laser GaIn<span class="hlt">N</span> quantum well. Thus AlGaIn<span class="hlt">N</span> laser <span class="hlt">diode</span> technology is a key enabler for the development of new disruptive system level applications in displays, telecom, defence and other industries. Ridge waveguide laser <span class="hlt">diodes</span> are fabricated to achieve single mode operation with optical powers up to 100mW with the 400-440nm wavelength range with high reliability. Visible free-space and underwater communication at frequencies up to 2.5GHz is reported using a directly modulated 422nm Ga<span class="hlt">N</span> laser <span class="hlt">diode</span>. Low defectivity and highly uniform Ga<span class="hlt">N</span> substrates allow arrays and bars to be fabricated. High power operation operation of AlGaIn<span class="hlt">N</span> laser bars with up to 20 emitters have been demonstrated at optical powers up to 4W in a CS package with common contact configuration. An alternative package configuration for AlGaIn<span class="hlt">N</span> laser arrays allows for each individual laser to be individually addressable allowing complex free-space or optical fibre system integration with a very small form-factor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009SPIE.7325E..0TP','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009SPIE.7325E..0TP"><span>High brightness <span class="hlt">diode</span> laser module development at <span class="hlt">n</span>LIGHT Photonics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Price, Kirk; Karlsen, Scott; Brown, Aaron; Reynolds, Mitch; Mehl, Ron; Leisher, Paul; Patterson, Steve; Bell, Jake; Martinsen, Rob</p> <p>2009-05-01</p> <p>We report on the development of ultra-high brightness laser <span class="hlt">diode</span> modules at <span class="hlt">n</span>LIGHT Photonics. This paper demonstrates a laser <span class="hlt">diode</span> module capable of coupling over 100W at 976 nm into a 105 μm, 0.15 NA fiber with fiber coupling efficiency greater than 85%. The high brightness module has an optical excitation under 0.13 NA, is virtually free of cladding modes, and has been wavelength stabilized with the use of volume holographic gratings for narrow-band operation. Utilizing <span class="hlt">n</span>LIGHT's Pearl product architecture, these modules are based on hard soldered single emitters packaged into a compact and passively-cooled package. These modules are designed to be compatible with high power 7:1 fused fiber combiners, enabling over 500W power coupled into a 220 μm, 0.22 NA fiber. These modules address the need in the market for high brightness and wavelength stabilized <span class="hlt">diode</span> lasers for pumping fiber lasers and solid-state laser systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23070147','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23070147"><span>Optical sensing system based on wireless paired emitter <span class="hlt">detector</span> <span class="hlt">diode</span> device and ionogels for lab-on-a-disc water quality analysis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Czugala, Monika; Gorkin, Robert; Phelan, Thomas; Gaughran, Jennifer; Curto, Vincenzo Fabio; Ducrée, Jens; Diamond, Dermot; Benito-Lopez, Fernando</p> <p>2012-12-07</p> <p>This work describes the first use of a wireless paired emitter <span class="hlt">detector</span> <span class="hlt">diode</span> device (PEDD) as an optical sensor for water quality monitoring in a lab-on-a-disc device. The microfluidic platform, based on an ionogel sensing area combined with a low-cost optical sensor, is applied for quantitative <span class="hlt">p</span>H and qualitative turbidity monitoring of water samples at point-of-need. The autonomous capabilities of the PEDD system, combined with the portability and wireless communication of the full device, provide the flexibility needed for on-site water testing. Water samples from local fresh and brackish sources were successfully analysed using the device, showing very good correlation with standard bench-top systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25281940','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25281940"><span>Design and experimental testing of air slab caps which convert commercial electron <span class="hlt">diodes</span> into dual purpose, correction-free <span class="hlt">diodes</span> for small field dosimetry.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Charles, P H; Cranmer-Sargison, G; Thwaites, D I; Kairn, T; Crowe, S B; Pedrazzini, G; Aland, T; Kenny, J; Langton, C M; Trapp, J V</p> <p>2014-10-01</p> <p>Two <span class="hlt">diodes</span> which do not require correction factors for small field relative output measurements are designed and validated using experimental methodology. This was achieved by adding an air layer above the active volume of the <span class="hlt">diode</span> <span class="hlt">detectors</span>, which canceled out the increase in response of the <span class="hlt">diodes</span> in small fields relative to standard field sizes. Due to the increased density of silicon and other components within a <span class="hlt">diode</span>, additional electrons are created. In very small fields, a very small air gap acts as an effective filter of electrons with a high angle of incidence. The aim was to design a <span class="hlt">diode</span> that balanced these perturbations to give a response similar to a water-only geometry. Three thicknesses of air were placed at the proximal end of a PTW 60017 electron <span class="hlt">diode</span> (PTWe) using an adjustable "air cap". A set of output ratios (ORDet (fclin) ) for square field sizes of side length down to 5 mm was measured using each air thickness and compared to ORDet (fclin) measured using an IBA stereotactic field <span class="hlt">diode</span> (SFD). kQclin,Qmsr (fclin,fmsr) was transferred from the SFD to the PTWe <span class="hlt">diode</span> and plotted as a function of air gap thickness for each field size. This enabled the optimal air gap thickness to be obtained by observing which thickness of air was required such that kQclin,Qmsr (fclin,fmsr) was equal to 1.00 at all field sizes. A similar procedure was used to find the optimal air thickness required to make a modified Sun Nuclear EDGE <span class="hlt">detector</span> (EDGEe) which is "correction-free" in small field relative dosimetry. In addition, the feasibility of experimentally transferring kQclin,Qmsr (fclin,fmsr) values from the SFD to unknown <span class="hlt">diodes</span> was tested by comparing the experimentally transferred kQclin,Qmsr (fclin,fmsr) values for unmodified PTWe and EDGEe <span class="hlt">diodes</span> to Monte Carlo simulated values. 1.0 mm of air was required to make the PTWe <span class="hlt">diode</span> correction-free. This modified <span class="hlt">diode</span> (PTWeair) produced output factors equivalent to those in water at all field sizes (5-50 mm</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4154899','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4154899"><span>Ultraviolet/blue light-emitting <span class="hlt">diodes</span> based on single horizontal ZnO microrod/Ga<span class="hlt">N</span> heterojunction</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2014-01-01</p> <p>We report electroluminescence (EL) from single horizontal ZnO microrod (MR) and <span class="hlt">p-GaN</span> heterojunction light-emitting <span class="hlt">diodes</span> under forward and reverse bias. EL spectra were composed of two blue emissions centered at 431 and 490 nm under forward biases, but were dominated by a ultraviolet (UV) emission located at 380 nm from <span class="hlt">n</span>-ZnO MR under high reverse biases. Light-output-current characteristic of the UV emission reveals that the rate of radiative recombination is faster than that of the nonradiative recombination. Highly efficient ZnO excitonic recombination at reverse bias is caused by electrons tunneling from deep-level states near the <span class="hlt">n-ZnO/p-GaN</span> interface to the conduction band in <span class="hlt">n</span>-ZnO. PMID:25232299</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25232299','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25232299"><span>Ultraviolet/blue light-emitting <span class="hlt">diodes</span> based on single horizontal ZnO microrod/Ga<span class="hlt">N</span> heterojunction.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Du, Chia-Fong; Lee, Chen-Hui; Cheng, Chao-Tsung; Lin, Kai-Hsiang; Sheu, Jin-Kong; Hsu, Hsu-Cheng</p> <p>2014-01-01</p> <p>We report electroluminescence (EL) from single horizontal ZnO microrod (MR) and <span class="hlt">p-GaN</span> heterojunction light-emitting <span class="hlt">diodes</span> under forward and reverse bias. EL spectra were composed of two blue emissions centered at 431 and 490 nm under forward biases, but were dominated by a ultraviolet (UV) emission located at 380 nm from <span class="hlt">n</span>-ZnO MR under high reverse biases. Light-output-current characteristic of the UV emission reveals that the rate of radiative recombination is faster than that of the nonradiative recombination. Highly efficient ZnO excitonic recombination at reverse bias is caused by electrons tunneling from deep-level states near the <span class="hlt">n-ZnO/p-GaN</span> interface to the conduction band in <span class="hlt">n</span>-ZnO.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21499630-sup-gamma-sup-reaction-studied-composite-germanium-detector','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21499630-sup-gamma-sup-reaction-studied-composite-germanium-detector"><span>The {sup 14}<span class="hlt">N(p</span>,{gamma}){sup 15}O reaction studied with a composite germanium <span class="hlt">detector</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Marta, M.; Bemmerer, D.; Formicola, A.</p> <p>2011-04-15</p> <p>The rate of the carbon-nitrogen-oxygen (CNO) cycle of hydrogen burning is controlled by the {sup 14}<span class="hlt">N(p</span>,{gamma}){sup 15}O reaction. The reaction proceeds by capture to the ground states and several excited states in {sup 15}O. In order to obtain a reliable extrapolation of the excitation curve to astrophysical energy, fits in the R-matrix framework are needed. In an energy range that sensitively tests such fits, new cross-section data are reported here for the four major transitions in the {sup 14}<span class="hlt">N(p</span>,{gamma}){sup 15}O reaction. The experiment has been performed at the Laboratory for Underground Nuclear Astrophysics (LUNA) 400-kV accelerator placed deep underground inmore » the Gran Sasso facility in Italy. Using a composite germanium <span class="hlt">detector</span>, summing corrections have been considerably reduced with respect to previous studies. The cross sections for capture to the ground state and to the 5181, 6172, and 6792 keV excited states in {sup 15}O have been determined at 359, 380, and 399 keV beam energy. In addition, the branching ratios for the decay of the 278-keV resonance have been remeasured.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21121615','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21121615"><span>Rectifying properties of <span class="hlt">p-GaN</span> nanowires and an <span class="hlt">n</span>-silicon heterojunction vertical <span class="hlt">diode</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Manna, Sujit; Ashok, Vishal D; De, S K</p> <p>2010-12-01</p> <p>The heterojunction of a Pd-doped <span class="hlt">p-GaN</span> nanowire and <span class="hlt">n</span>-Si (100) is fabricated vertically by the vapor-liquid-solid method. The average diameter of the nanowire is 40 nm. The vertical junction reveals a significantly high rectification ratio of 10(3) at 5 V, a moderate ideality factor of ∼2, and a high breakdown voltage of ∼40 V. The charge transport across the <span class="hlt">p-n</span> junction is dominated by the electron-hole recombination process. The voltage dependence of capacitance indicates a graded-type junction. The resistance of the junction decreases with an increase in the bias voltage confirmed by impedance measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17840057','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17840057"><span>High-luminosity blue and blue-green gallium nitride light-emitting <span class="hlt">diodes</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Morkoç, H; Mohammad, S N</p> <p>1995-01-06</p> <p>Compact and efficient sources of blue light for full color display applications and lighting eluded and tantalized researchers for many years. Semiconductor light sources are attractive owing to their reliability and amenability to mass manufacture. However, large band gaps are required to achieve blue color. A class of compound semiconductors formed by metal nitrides, Ga<span class="hlt">N</span> and its allied compounds AIGa<span class="hlt">N</span> and InGa<span class="hlt">N</span>, exhibits properties well suited for not only blue and blue-green emitters, but also for ultraviolet emitters and <span class="hlt">detectors</span>. What thwarted engineers and scientists from fabricating useful devices from these materials in the past was the poor quality of material and lack of <span class="hlt">p</span>-type doping. Both of these obstacles have recently been overcome to the point where highluminosity blue and blue-green light-emitting <span class="hlt">diodes</span> are now available in the marketplace.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_25 --> <div class="footer-extlink text-muted" style="margin-bottom:1rem; text-align:center;">Some links on this page may take you to non-federal websites. 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