Sample records for local electronic structure

  1. Local-structure change rendered by electronic localization-delocalization transition in cerium-based metallic glasses

    NASA Astrophysics Data System (ADS)

    Luo, Qiang; Schwarz, Björn; Swarbrick, Janine C.; Bednarčik, Jozef; Zhu, Yingcai; Tang, Meibo; Zheng, Lirong; Li, Ran; Shen, Jun; Eckert, Jürgen

    2018-02-01

    With increasing temperature, metallic glasses (MGs) undergo first glass transition without pronounced structural change and then crystallization with distinct variation in structure and properties. The present study shows a structural change of short-range order induced by an electron-delocalization transition, along with an unusual large-volume shrinkage in Ce-based MGs. An f -electron localization-delocalization transition with thermal hysteresis is observed from the temperature dependence of x-ray absorption spectroscopy and resonant inelastic x-ray scattering spectra, indicating an inheritance of the 4 f configuration of pure Ce. However, the delocalization transition becomes broadened due to the local structural heterogeneity and related fluctuation of 4 f levels in the Ce-based MGs. The amorphous structure regulated 4 f delocalization of Ce leads to bond shortening and abnormal structure change of the topological and chemical short-range orders. Due to the hierarchical bonding nature, the structure should change in a similar manner on different length scales (but not isostructurally like the Ce metal) in Ce-based MGs.

  2. How localized is ``local?'' Efficiency vs. accuracy of O(N) domain decomposition in local orbital based all-electron electronic structure theory

    NASA Astrophysics Data System (ADS)

    Havu, Vile; Blum, Volker; Scheffler, Matthias

    2007-03-01

    Numeric atom-centered local orbitals (NAO) are efficient basis sets for all-electron electronic structure theory. The locality of NAO's can be exploited to render (in principle) all operations of the self-consistency cycle O(N). This is straightforward for 3D integrals using domain decomposition into spatially close subsets of integration points, enabling critical computational savings that are effective from ˜tens of atoms (no significant overhead for smaller systems) and make large systems (100s of atoms) computationally feasible. Using a new all-electron NAO-based code,^1 we investigate the quantitative impact of exploiting this locality on two distinct classes of systems: Large light-element molecules [Alanine-based polypeptide chains (Ala)n], and compact transition metal clusters. Strict NAO locality is achieved by imposing a cutoff potential with an onset radius rc, and exploited by appropriately shaped integration domains (subsets of integration points). Conventional tight rc<= 3å have no measurable accuracy impact in (Ala)n, but introduce inaccuracies of 20-30 meV/atom in Cun. The domain shape impacts the computational effort by only 10-20 % for reasonable rc. ^1 V. Blum, R. Gehrke, P. Havu, V. Havu, M. Scheffler, The FHI Ab Initio Molecular Simulations (aims) Project, Fritz-Haber-Institut, Berlin (2006).

  3. Probing the band structure and local electronic properties of low-dimensional semiconductor structures

    NASA Astrophysics Data System (ADS)

    Walrath, Jenna Cherie

    Low-dimensional semiconductor structures are important for a wide variety of applications, and recent advances in nanoscale fabrication are paving the way for increasingly precise nano-engineering of a wide range of materials. It is therefore essential that the physics of materials at the nanoscale are thoroughly understood to unleash the full potential of nanotechnology, requiring the development of increasingly sophisticated instrumentation and modeling. Of particular interest is the relationship between the local density of states (LDOS) of low-dimensional structures and the band structure and local electronic properties. This dissertation presents the investigation of the band structure, LDOS, and local electronic properties of nanostructures ranging from zero-dimensional (0D) quantum dots (QDs) to two-dimensional (2D) thin films, synthesizing computational and experimental approaches including Poisson-Schrodinger band structure calculations, scanning tunneling microscopy (STM), scanning tunneling spectroscopy (STS), and scanning thermoelectric microscopy (SThEM). A method is presented for quantifying the local Seebeck coefficient (S) with SThEM, using a quasi-3D conversion matrix approach to directly convert temperature gradient-induced voltages S. For a GaAs p-n junction, the resulting S-profile is consistent with that computed using the free carrier concentration profile. This combined computational-experimental approach is expected to enable nanoscale measurements of S across a wide variety of heterostructure interfaces. The local carrier concentration, n, is profiled across epitaxial InAs/GaAs QDs, where SThEM is used to profile the temperature gradient-induced voltage, which is converted to a profile of the local S and finally to an n profile. The S profile is converted to a conduction band-edge profile and compared with Poisson-Schrodinger band-edge simulations. The combined computational-experimental approach suggests a reduced n in the QD center in

  4. Direct Visualization of Local Electromagnetic Field Structures by Scanning Transmission Electron Microscopy.

    PubMed

    Shibata, Naoya; Findlay, Scott D; Matsumoto, Takao; Kohno, Yuji; Seki, Takehito; Sánchez-Santolino, Gabriel; Ikuhara, Yuichi

    2017-07-18

    The functional properties of materials and devices are critically determined by the electromagnetic field structures formed inside them, especially at nanointerface and surface regions, because such structures are strongly associated with the dynamics of electrons, holes and ions. To understand the fundamental origin of many exotic properties in modern materials and devices, it is essential to directly characterize local electromagnetic field structures at such defect regions, even down to atomic dimensions. In recent years, rapid progress in the development of high-speed area detectors for aberration-corrected scanning transmission electron microscopy (STEM) with sub-angstrom spatial resolution has opened new possibilities to directly image such electromagnetic field structures at very high-resolution. In this Account, we give an overview of our recent development of differential phase contrast (DPC) microscopy for aberration-corrected STEM and its application to many materials problems. In recent years, we have developed segmented-type STEM detectors which divide the detector plane into 16 segments and enable simultaneous imaging of 16 STEM images which are sensitive to the positions and angles of transmitted/scattered electrons on the detector plane. These detectors also have atomic-resolution imaging capability. Using these segmented-type STEM detectors, we show DPC STEM imaging to be a very powerful tool for directly imaging local electromagnetic field structures in materials and devices in real space. For example, DPC STEM can clearly visualize the local electric field variation due to the abrupt potential change across a p-n junction in a GaAs semiconductor, which cannot be observed by normal in-focus bright-field or annular type dark-field STEM imaging modes. DPC STEM is also very effective for imaging magnetic field structures in magnetic materials, such as magnetic domains and skyrmions. Moreover, real-time imaging of electromagnetic field structures can

  5. Localized variations in electronic structure of AlGaN/GaN heterostructures grown by molecular-beam epitaxy

    NASA Astrophysics Data System (ADS)

    Smith, K. V.; Yu, E. T.; Elsass, C. R.; Heying, B.; Speck, J. S.

    2001-10-01

    Local electronic properties in a molecular-beam-epitaxy-grown AlxGa1-xN/GaN heterostructure field-effect transistor epitaxial layer structure are probed using depth-resolved scanning capacitance microscopy. Theoretical analysis of contrast observed in scanning capacitance images acquired over a range of bias voltages is used to assess the possible structural origins of local inhomogeneities in electronic structure, which are shown to be concentrated in areas where Ga droplets had formed on the surface during growth. Within these regions, there are significant variations in the local electronic structure that are attributed to variations in both AlxGa1-xN layer thickness and Al composition. Increased charge trapping is also observed in these regions.

  6. Structural phase transition and 5f-electrons localization of PuSe explored by ab initio calculations

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

    Cui Shouxin, E-mail: shouxincui@yahoo.co; Feng Wenxia; Hu Haiquan

    2010-04-15

    An investigation into the structural phase transformation, electronic and optical properties of PuSe under high pressure was conducted by using the full potential linearized augmented plane wave plus local orbitals (FP-LAPW+lo) method, in the presence and in the absence of spin-orbit coupling (SOC). Our results demonstrate that there exists a structural phase transition from rocksalt (B 1) structure to CsCl-type (B 2) structure at the transition pressure of 36.3 GPa (without SOC) and 51.3 GPa (with SOC). The electronic density of states (DOS) for PuSe show that the f-electrons of Pu are more localized and concentrated in a narrow peakmore » near the Fermi level, which is consistent with the experimental studies. The band structure shows that B 1-PuSe is metallic. A pseudogap appears around the Fermi level of the total density of states of B 1 phase PuSe, which may contribute to its stability. The calculated reflectivity R(omega) shows agreement with the available experimental results. Furthermore, the absorption spectrum, refractive index, extinction coefficient, energy-loss spectrum and dielectric function were calculated. The origin of the spectral peaks was interpreted based on the electronic structures. - Abstract: Graphical Abstract Legend (TOC Figure): 5f-electrons are more localized by the analysis of the density of states (SOC). The origin spectra peaks was interpreted based on electronic structures.« less

  7. On the electron density localization in elemental cubic ceramic and FCC transition metals by means of a localized electrons detector.

    PubMed

    Aray, Yosslen; Paredes, Ricardo; Álvarez, Luis Javier; Martiz, Alejandro

    2017-06-14

    The electron density localization in insulator and semiconductor elemental cubic materials with diamond structure, carbon, silicon, germanium, and tin, and good metallic conductors with face centered cubic structure such as α-Co, Ni, Cu, Rh, Pd, Ag, Ir, Pt, and Au, was studied using a localized electrons detector defined in the local moment representation. Our results clearly show an opposite pattern of the electron density localization for the cubic ceramic and transition metal materials. It was found that, for the elemental ceramic materials, the zone of low electron localization is very small and is mainly localized on the atomic basin edges. On the contrary, for the transition metals, there are low-valued localized electrons detector isocontours defining a zone of highly delocalized electrons that extends throughout the material. We have found that the best conductors are those in which the electron density at this low-value zone is the lowest.

  8. Effect of local atomic and electronic structures on thermoelectric properties of chemically substituted CoSi

    NASA Astrophysics Data System (ADS)

    Hsu, C. C.; Pao, C. W.; Chen, J. L.; Chen, C. L.; Dong, C. L.; Liu, Y. S.; Lee, J. F.; Chan, T. S.; Chang, C. L.; Kuo, Y. K.; Lue, C. S.

    2014-05-01

    We report the effects of Ge partial substitution for Si on local atomic and electronic structures of thermoelectric materials in binary compound cobalt monosilicides (\\text{CoSi}_{1-x}\\text{Ge}_{x}\\text{:}\\ 0 \\le x \\le 0.15 ). Correlations between local atomic/electronic structure and thermoelectric properties are investigated by means of X-ray absorption spectroscopy. The spectroscopic results indicate that as Ge is partially substituted onto Si sites at x \\le 0.05 , Co in CoSi1-xGex gains a certain amount of charge in its 3d orbitals. Contrarily, upon further replacing Si with Ge at x \\ge 0.05 , the Co 3d orbitals start to lose some of their charge. Notably, thermopower is strongly correlated with charge redistribution in the Co 3d orbital, and the observed charge transfer between Ge and Co is responsible for the variation of Co 3d occupancy number. In addition to Seebeck coefficient, which can be modified by tailoring the Co 3d states, local lattice disorder may also be beneficial in enhancing the thermoelectric properties. Extended X-ray absorption fine structure spectrum results further demonstrate that the lattice phonons can be enhanced by Ge doping, which results in the formation of the disordered Co-Co pair. Improvements in the thermoelectric properties are interpreted based on the variation of local atomic and electronic structure induced by lattice distortion through chemical substitution.

  9. Propagation of localized structures in relativistic magnetized electron-positron plasmas using particle-in-cell simulations

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

    López, Rodrigo A.; Muñoz, Víctor; Viñas, Adolfo F.

    2015-09-15

    We use a particle-in-cell simulation to study the propagation of localized structures in a magnetized electron-positron plasma with relativistic finite temperature. We use as initial condition for the simulation an envelope soliton solution of the nonlinear Schrödinger equation, derived from the relativistic two fluid equations in the strongly magnetized limit. This envelope soliton turns out not to be a stable solution for the simulation and splits in two localized structures propagating in opposite directions. However, these two localized structures exhibit a soliton-like behavior, as they keep their profile after they collide with each other due to the periodic boundary conditions.more » We also observe the formation of localized structures in the evolution of a spatially uniform circularly polarized Alfvén wave. In both cases, the localized structures propagate with an amplitude independent velocity.« less

  10. TiO 2 nanotube arrays for photocatalysis: Effects of crystallinity, local order, and electronic structure

    DOE PAGES

    Liu, Jing; Hosseinpour, Pegah M.; Luo, Si; ...

    2014-11-19

    To furnish insight into correlations of electronic and local structure and photoactivity, arrays of short and long TiO₂ nanotubes were synthesized by electrochemical anodization of Ti foil, followed by thermal treatment in O₂ (oxidizing), Ar (inert), and H₂ (reducing) environments. The physical and electronic structures of these nanotubes were probed with x-ray diffraction, scanning electron microscopy, and synchrotron-based x-ray absorption spectroscopy, and correlated with their photocatalytic properties. The photocatalytic activity of the nanotubes was evaluated by monitoring the degradation of methyl orange under UV-VIS light irradiation. Results show that upon annealing at 350 °C all as-anodized amorphous TiO₂ nanotube samplesmore » partially transform to the anatase structure, with variations in the degree of crystallinity and in the concentration of local defects near the nanotubes' surface (~5 nm) depending on the annealing conditions. Degradation of methyl orange was not detectable for the as-anodized TiO₂ nanotubes regardless of their length. The annealed long nanotubes demonstrated detectable catalytic activity, which was more significant with the H₂-annealed nanotubes than with the Ar- and O₂-annealed nanotube samples. This enhanced photocatalytic response of the H₂-annealed long nanotubes relative to the other samples is positively correlated with the presence of a larger concentration of lattice defects (such as Ti 3+ and anticipated oxygen vacancies) and a slightly lower degree of crystallinity near the nanotube surface. These physical and electronic structural attributes impact the efficacy of visible light absorption; moreover, the increased concentration of surface defects is postulated to promote the generation of hydroxyl radicals and thus accelerate the photodegradation of the methyl orange. The information obtained from this study provides unique insight into the role of the near-surface electronic and defect structure

  11. Localized electronic structures of graphene oxide studied using scanning tunneling microscopy and spectroscopy.

    PubMed

    Katano, Satoshi; Wei, Tao; Sasajima, Takumi; Kasama, Ryuhei; Uehara, Yoichi

    2018-06-21

    We have used scanning tunneling microscopy (STM) to elucidate the nanoscale electronic structures of graphene oxide (GO). The unreduced GO layer was imaged using STM without reduction processes when deposited on a Au(111) surface covered with an octanethiolate self-assembled monolayer (C8S-SAM). The STM image of the GO sheet exhibits a grainy structure having a thickness of about 1 nm, which is in good agreement with the previous results obtained using atomic force microscopy (AFM). We found that the C8S-SAM suppresses the adsorption of water remaining on the substrate, which would be important to accomplish the nanoscale imaging of the unreduced GO by STM. Furthermore, we successfully detected the π and π* states localized in the GO sheet using scanning tunneling spectroscopy (STS). The π-π* gap energy and the gap center are not uniform within the GO sheet, indicating the existence of various sizes of the sp2 domain and evidence for the local electronic doping by the substituents.

  12. Electron solvation and localization at interfaces

    NASA Astrophysics Data System (ADS)

    Harris, Charles B.; Szymanski, Paul; Garrett-Roe, Sean; Miller, Andre D.; Gaffney, Kelly J.; Liu, Simon H.; Bezel, Ilya

    2003-12-01

    Two-photon photoemission of thiolate/Ag(111), nitrile/Ag(111), and alcohol/Ag(111) interfaces elucidates electron solvation and localization in two dimensions. For low coverages of thiolates on Ag(111), the occupied (HOMO) and unoccupied (LUMO) electronic states of the sulfer-silver bond are localized due to the lattice gas structure of the adsorbate. As the coverage saturates and the adsorbate-adsorbate nearest neighbor distance decreases, the HOMO and LUMO delocalize across many adsorbate molecules. Alcohol- and nitrile-covered Ag(111) surfaces solvate excess image potential state (IPS) electrons. In the case of alcohol-covered surfaces, this solvation is due to a shift in the local workfunction of the surface. For two-monolayer coverages of nitriles/Ag(111), localization accompanies solvation of the IPS. The size of the localized electron can be estimated by Fourier transformation of the wavefunction from momentum- to position-space. The IPS electron localizes to 15 +/- 4 angstroms full-width at half maximum in the plane of the surface, i.e., to a single lattice site.

  13. Effect of oxygen deficiency on electronic properties and local structure of amorphous tantalum oxide thin films

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

    Denny, Yus Rama; Firmansyah, Teguh; Oh, Suhk Kun

    2016-10-15

    Highlights: • The effect of oxygen flow rate on electronic properties and local structure of tantalum oxide thin films was studied. • The oxygen deficiency induced the nonstoichiometric state a-TaOx. • A small peak at 1.97 eV above the valence band side appeared on nonstoichiometric Ta{sub 2}O{sub 5} thin films. • The oxygen flow rate can change the local electronic structure of tantalum oxide thin films. - Abstract: The dependence of electronic properties and local structure of tantalum oxide thin film on oxygen deficiency have been investigated by means of X-ray photoelectron spectroscopy (XPS), Reflection Electron Energy Loss Spectroscopy (REELS),more » and X-ray absorption spectroscopy (XAS). The XPS results showed that the oxygen flow rate change results in the appearance of features in the Ta 4f at the binding energies of 23.2 eV, 24.4 eV, 25.8, and 27.3 eV whose peaks are attributed to Ta{sup 1+}, Ta{sup 2+}, Ta{sup 3+}/Ta{sup 4+}, and Ta{sup 5+}, respectively. The presence of nonstoichiometric state from tantalum oxide (TaOx) thin films could be generated by the oxygen vacancies. In addition, XAS spectra manifested both the increase of coordination number of the first Ta-O shell and a considerable reduction of the Ta-O bond distance with the decrease of oxygen deficiency.« less

  14. Probing the electronic and local structural changes across the pressure-induced insulator-to-metal transition in VO2

    NASA Astrophysics Data System (ADS)

    Marini, C.; Bendele, M.; Joseph, B.; Kantor, I.; Mitrano, M.; Mathon, O.; Baldini, M.; Malavasi, L.; Pascarelli, S.; Postorino, P.

    2014-11-01

    Local and electronic structures of vanadium in \\text{VO}2 are studied across the high-pressure insulator-to-metal (IMT) transition using V K-edge x-ray absorption spectroscopy. Unlike the temperature-induced IMT, pressure-induced metallization leads to only subtle changes in the V K-edge prepeak structure, indicating a different mechanism involving smaller electronic spectral weight transfer close to the chemical potential. Intriguingly, upon application of the hydrostatic pressure, the electronic structure begins to show substantial changes well before the occurrence of the IMT and the associated structural transition to an anisotropic compression of the monoclinic metallic phase.

  15. Communication: Recovering the flat-plane condition in electronic structure theory at semi-local DFT cost

    NASA Astrophysics Data System (ADS)

    Bajaj, Akash; Janet, Jon Paul; Kulik, Heather J.

    2017-11-01

    The flat-plane condition is the union of two exact constraints in electronic structure theory: (i) energetic piecewise linearity with fractional electron removal or addition and (ii) invariant energetics with change in electron spin in a half filled orbital. Semi-local density functional theory (DFT) fails to recover the flat plane, exhibiting convex fractional charge errors (FCE) and concave fractional spin errors (FSE) that are related to delocalization and static correlation errors. We previously showed that DFT+U eliminates FCE but now demonstrate that, like other widely employed corrections (i.e., Hartree-Fock exchange), it worsens FSE. To find an alternative strategy, we examine the shape of semi-local DFT deviations from the exact flat plane and we find this shape to be remarkably consistent across ions and molecules. We introduce the judiciously modified DFT (jmDFT) approach, wherein corrections are constructed from few-parameter, low-order functional forms that fit the shape of semi-local DFT errors. We select one such physically intuitive form and incorporate it self-consistently to correct semi-local DFT. We demonstrate on model systems that jmDFT represents the first easy-to-implement, no-overhead approach to recovering the flat plane from semi-local DFT.

  16. Probing the structural and dynamical properties of liquid water with models including non-local electron correlation

    NASA Astrophysics Data System (ADS)

    Del Ben, Mauro; Hutter, Jürg; VandeVondele, Joost

    2015-08-01

    Water is a ubiquitous liquid that displays a wide range of anomalous properties and has a delicate structure that challenges experiment and simulation alike. The various intermolecular interactions that play an important role, such as repulsion, polarization, hydrogen bonding, and van der Waals interactions, are often difficult to reproduce faithfully in atomistic models. Here, electronic structure theories including all these interactions at equal footing, which requires the inclusion of non-local electron correlation, are used to describe structure and dynamics of bulk liquid water. Isobaric-isothermal (NpT) ensemble simulations based on the Random Phase Approximation (RPA) yield excellent density (0.994 g/ml) and fair radial distribution functions, while various other density functional approximations produce scattered results (0.8-1.2 g/ml). Molecular dynamics simulation in the microcanonical (NVE) ensemble based on Møller-Plesset perturbation theory (MP2) yields dynamical properties in the condensed phase, namely, the infrared spectrum and diffusion constant. At the MP2 and RPA levels of theory, ice is correctly predicted to float on water, resolving one of the anomalies as resulting from a delicate balance between van der Waals and hydrogen bonding interactions. For several properties, obtaining quantitative agreement with experiment requires correction for nuclear quantum effects (NQEs), highlighting their importance, for structure, dynamics, and electronic properties. A computed NQE shift of 0.6 eV for the band gap and absorption spectrum illustrates the latter. Giving access to both structure and dynamics of condensed phase systems, non-local electron correlation will increasingly be used to study systems where weak interactions are of paramount importance.

  17. Role of defects in BiFeO₃ multiferroic films and their local electronic structure by x-ray absorption spectroscopy

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

    Ravalia, Ashish; Vagadia, Megha; Solanki, P. S.

    2014-10-21

    Present study reports the role of defects in the electrical transport in BiFeO₃ (BFO) multiferroic films and its local electronic structure investigated by near-edge X-ray absorption fine structure. Defects created by high energy 200 MeV Ag⁺¹⁵ ion irradiation with a fluence of ∼5 × 10¹¹ ions/cm² results in the increase in structural strain and reduction in the mobility of charge carriers and enhancement in resistive (I-V) and polarization (P-E) switching behaviour. At higher fluence of ∼5 × 10¹² ions/cm², there is a release in the structural strain due to local annealing effect, resulting in an increase in the mobility of charge carriers, which are releasedmore » from oxygen vacancies and hence suppression in resistive and polarization switching. Near-edge X-ray absorption fine structure studies at Fe L₃,₂- and O K-edges show a significant change in the spectral features suggesting the modifications in the local electronic structure responsible for changes in the intrinsic magnetic moment and electrical transport properties of BFO.« less

  18. Local electronic structure and nanolevel hierarchical organization of bone tissue: theory and NEXAFS study

    NASA Astrophysics Data System (ADS)

    Pavlychev, A. A.; Avrunin, A. S.; Vinogradov, A. S.; Filatova, E. O.; Doctorov, A. A.; Krivosenko, Yu S.; Samoilenko, D. O.; Svirskiy, G. I.; Konashuk, A. S.; Rostov, D. A.

    2016-12-01

    Theoretical and experimental investigations of native bone are carried out to understand relationships between its hierarchical organization and local electronic and atomic structure of the mineralized phase. The 3D superlattice model of a coplanar assembly of the hydroxyapatite (HAP) nanocrystallites separated by the hydrated nanolayers is introduced to account the interplay of short-, long- and super-range order parameters in bone tissue. The model is applied to (i) predict and rationalize the HAP-to-bone spectral changes in the electronic structure and (ii) describe the mechanisms ensuring the link of the hierarchical organization with the electronic structure of the mineralized phase in bone. To check the predictions the near-edge x-ray absorption fine structure (NEXAFS) at the Ca 2p, P 2p and O 1s thresholds is measured for native bone and compared with NEXAFS for reference compounds. The NEXAFS analysis has demonstrated the essential hierarchy induced HAP-to-bone red shifts of the Ca and P 2p-to-valence transitions. The lowest O 1s excitation line at 532.2 eV in bone is assigned with superposition of core transitions in the hydroxide OH-(H2O) m anions, Ca2+(H2O) n cations, the carboxyl groups inside the collagen and [PO4]2- and [PO4]- anions with unsaturated P-O bonds.

  19. Electronic structure, local magnetism, and spin-orbit effects of Ir(IV)-, Ir(V)-, and Ir(VI)-based compounds

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

    Laguna-Marco, M. A.; Kayser, P.; Alonso, J. A.

    2015-06-01

    Element- and orbital-selective x-ray absorption and magnetic circular dichroism measurements are carried out to probe the electronic structure and magnetism of Ir 5d electronic states in double perovskite Sr2MIrO6 (M = Mg, Ca, Sc, Ti, Ni, Fe, Zn, In) and La2NiIrO6 compounds. All the studied systems present a significant influence of spin-orbit interactions in the electronic ground state. In addition, we find that the Ir 5d local magnetic moment shows different character depending on the oxidation state despite the net magnetization being similar for all the compounds. Ir carries an orbital contribution comparable to the spin contribution for Ir4+ (5d(5))more » and Ir5+ (5d(4)) oxides, whereas the orbital contribution is quenched for Ir6+ (5d(3)) samples. Incorporation of a magnetic 3d atom allows getting insight into the magnetic coupling between 5d and 3d transition metals. Together with previous susceptibility and neutron diffractionmeasurements, the results indicate that Ir carries a significant local magnetic moment even in samples without a 3d metal. The size of the (small) net magnetization of these compounds is a result of predominant antiferromagnetic interactions between local moments coupled with structural details of each perovskite structure« less

  20. Local Atomic Arrangements and Band Structure of Boron Carbide.

    PubMed

    Rasim, Karsten; Ramlau, Reiner; Leithe-Jasper, Andreas; Mori, Takao; Burkhardt, Ulrich; Borrmann, Horst; Schnelle, Walter; Carbogno, Christian; Scheffler, Matthias; Grin, Yuri

    2018-05-22

    Boron carbide, the simple chemical combination of boron and carbon, is one of the best-known binary ceramic materials. Despite that, a coherent description of its crystal structure and physical properties resembles one of the most challenging problems in materials science. By combining ab initio computational studies, precise crystal structure determination from diffraction experiments, and state-of-the-art high-resolution transmission electron microscopy imaging, this concerted investigation reveals hitherto unknown local structure modifications together with the known structural alterations. The mixture of different local atomic arrangements within the real crystal structure reduces the electron deficiency of the pristine structure CBC+B 12 , answering the question about electron precise character of boron carbide and introducing new electronic states within the band gap, which allow a better understanding of physical properties. © 2018 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim.

  1. Wavelets in electronic structure calculations

    NASA Astrophysics Data System (ADS)

    Modisette, Jason Perry

    1997-09-01

    Ab initio calculations of the electronic structure of bulk materials and large clusters are not possible on today's computers using current techniques. The storage and diagonalization of the Hamiltonian matrix are the limiting factors in both memory and execution time. The scaling of both quantities with problem size can be reduced by using approximate diagonalization or direct minimization of the total energy with respect to the density matrix in conjunction with a localized basis. Wavelet basis members are much more localized than conventional bases such as Gaussians or numerical atomic orbitals. This localization leads to sparse matrices of the operators that arise in SCF multi-electron calculations. We have investigated the construction of the one-electron Hamiltonian, and also the effective one- electron Hamiltonians that appear in density-functional and Hartree-Fock theories. We develop efficient methods for the generation of the kinetic energy and potential matrices, the Hartree and exchange potentials, and the local exchange-correlation potential of the LDA. Test calculations are performed on one-electron problems with a variety of potentials in one and three dimensions.

  2. AB INITIO Molecular Dynamics Simulations on Local Structure and Electronic Properties in Liquid MgxBi1-x Alloys

    NASA Astrophysics Data System (ADS)

    Hao, Qing-Hai; You, Yu-Wei; Kong, Xiang-Shan; Liu, C. S.

    2013-03-01

    The microscopic structure and dynamics of liquid MgxBi1-x(x = 0.5, 0.6, 0.7) alloys together with pure liquid Mg and Bi metals were investigated by means of ab initio molecular dynamics simulations. We present results of structure properties including pair correlation function, structural factor, bond-angle distribution function and bond order parameter, and their composition dependence. The dynamical and electronic properties have also been studied. The structure factor and pair correlation function are in agreement with the available experimental data. The calculated bond-angle distribution function and bond order parameter suggest that the stoichiometric composition Mg3Bi2 exhibits a different local structure order compared with other concentrations, which help us understand the appearance of the minimum electronic conductivity at this composition observed in previous experiments.

  3. Local 3d Electronic Structures of Co-Based Complexes with Medicinal Molecules Probed by Soft X-ray Absorption

    NASA Astrophysics Data System (ADS)

    Yamagami, Kohei; Fujiwara, Hidenori; Imada, Shin; Kadono, Toshiharu; Yamanaka, Keisuke; Muro, Takayuki; Tanaka, Arata; Itai, Takuma; Yoshinari, Nobuto; Konno, Takumi; Sekiyama, Akira

    2017-07-01

    We have examined the local 3d electronic structures of Co-Au multinuclear complexes with the medicinal molecules d-penicillaminate (d-pen) [Co{Au(PPh3)(d-pen)}2]ClO4 and [Co3{Au3(tdme)(d-pen)3}2] by Co L2,3-edge soft X-ray absorption (XAS) spectroscopy, where PPh3 denotes triphenylphosphine and tdme stands for 1,1,1-tris[(diphenylphosphino)methyl]ethane. The Co L2,3-edge XAS spectra indicate the localized ionic 3d electronic states in both materials. The experimental spectra are well explained by spectral simulation for a localized Co ion under ligand fields with the full multiplet theory, which verifies that the ions are in the low-spin Co3+ state in the former compound and in the high-spin Co2+ state in the latter.

  4. Electron localization of anions probed by nitrile vibrations

    DOE PAGES

    Mani, Tomoyasu; Grills, David C.; Newton, Marshall D.; ...

    2015-08-02

    Localization and delocalization of electrons is a key concept in chemistry, and is one of the important factors determining the efficiency of electron transport through organic conjugated molecules, which have potential to act as “molecular wires”. This, in turn, substantially influences the efficiencies of organic solar cells and other molecular electronic devices. It is also necessary to understand the electronic energy landscape and the dynamics of electrons through molecular chain that govern their transport capabilities in one-dimensional conjugated chains so that we can better define the design principles of conjugated molecules for their applications. We show that nitrile ν(C≡N) vibrationsmore » respond to the degree of electron localization in nitrile-substituted organic anions by utilizing time-resolved infrared (TRIR) detection combined with pulse radiolysis. Measurements of a series of aryl nitrile anions allow us to construct a semi-empirical calibration curve between the changes in the ν(C≡N) IR shifts and the changes in the electronic charges from the neutral to the anion states in the nitriles; more electron localization in the nitrile anion results in larger IR shifts. Furthermore, the IR linewidth in anions can report a structural change accompanying changes in the electronic density distribution. Probing the shift of the nitrile ν(C≡N) IR vibrational bands enables us to determine how the electron is localized in anions of nitrile-functionalized oligofluorenes, considered as organic mixed-valence compounds. We estimate the diabatic electron transfer distance, electronic coupling strengths, and energy barriers in these organic mixed-valence compounds. The analysis reveals a dynamic picture, showing that the electron is moving back and forth within the oligomers with a small activation energy of ≤ k BT, likely controlled by the movement of dihedral angles between monomer units. Thus, implications for the electron transport capability

  5. Theoretical Studies of the Electron Paramagnetic Resonance Parameters and Local Structure for VO2+ in Oxyfluoroborate Glasses

    NASA Astrophysics Data System (ADS)

    Zhang, Huaming; Yu, Xiaopeng; Xiao, Wenbo

    2017-12-01

    The electron paramagnetic resonance parameters (g factors g ‖, g ⊥ and hyperfine structure constants A ‖, A ⊥) of a tetragonal V4+ center in oxyfluoroborate glasses (20Li2O-10Li2F2-70B2O3) are theoretically investigated by using the perturbation formulas for a 3d1 ion in tetragonally compressed octahedra. The calculated results are in good agreement with the experimental data. Local structure parameters of [VO6]8- clusters are obtained from the calculation (i.e., R‖ ≈ 1.74 Å and R⊥ ≈ 1.985 Å for the metal-ligand distances parallel and perpendicular to the C4 axis, respectively). It is shown that the local structure around the V4+ ion possesses a compressed tetragonal distortion along C 4 axis. The signs of the hyperfine structure constants A‖ and A ⊥ for V4+ centers in oxyfluoroborate glasses were also suggested in the discussion.

  6. Nano-fEM: protein localization using photo-activated localization microscopy and electron microscopy.

    PubMed

    Watanabe, Shigeki; Richards, Jackson; Hollopeter, Gunther; Hobson, Robert J; Davis, Wayne M; Jorgensen, Erik M

    2012-12-03

    Mapping the distribution of proteins is essential for understanding the function of proteins in a cell. Fluorescence microscopy is extensively used for protein localization, but subcellular context is often absent in fluorescence images. Immuno-electron microscopy, on the other hand, can localize proteins, but the technique is limited by a lack of compatible antibodies, poor preservation of morphology and because most antigens are not exposed to the specimen surface. Correlative approaches can acquire the fluorescence image from a whole cell first, either from immuno-fluorescence or genetically tagged proteins. The sample is then fixed and embedded for electron microscopy, and the images are correlated (1-3). However, the low-resolution fluorescence image and the lack of fiducial markers preclude the precise localization of proteins. Alternatively, fluorescence imaging can be done after preserving the specimen in plastic. In this approach, the block is sectioned, and fluorescence images and electron micrographs of the same section are correlated (4-7). However, the diffraction limit of light in the correlated image obscures the locations of individual molecules, and the fluorescence often extends beyond the boundary of the cell. Nano-resolution fluorescence electron microscopy (nano-fEM) is designed to localize proteins at nano-scale by imaging the same sections using photo-activated localization microscopy (PALM) and electron microscopy. PALM overcomes the diffraction limit by imaging individual fluorescent proteins and subsequently mapping the centroid of each fluorescent spot (8-10). We outline the nano-fEM technique in five steps. First, the sample is fixed and embedded using conditions that preserve the fluorescence of tagged proteins. Second, the resin blocks are sectioned into ultrathin segments (70-80 nm) that are mounted on a cover glass. Third, fluorescence is imaged in these sections using the Zeiss PALM microscope. Fourth, electron dense structures are

  7. Electron localization in rod-shaped triicosahedral gold nanocluster

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

    Zhou, Meng; Jin, Renxi; Sfeir, Matthew Y.

    Atomically precise gold nanocluster based on linear assembly of repeating icosahedrons (clusters of clusters) is a unique type of linear nanostructure, which exhibits strong near-infrared absorption as their free electrons are confined in a one-dimensional quantum box. There is little known about the carrier dynamics in these nanoclusters, which limit their energy-related applications. We reported the observation of exciton localization in triicosahedral Au37 nanoclusters (0.5 nm in diameter and 1.6 nm in length) by measuring femtosecond and nanosecond carrier dynamics. Upon photoexcitation to S1 electronic state, electrons in Au37 undergo ~100-ps localization from the two vertexes of three icosahedrons tomore » one vertex, forming a long-lived S1* state. Such phenomenon is not observed in Au25 (dimer) and Au13 (monomer) consisting of two and one icosahedrons, respectively. We have further observed temperature dependence on the localization process, which proves it is thermally driven. Two excited-state vibration modes with frequencies of 20 and 70 cm -1 observed in the kinetic traces are assigned to the axial and radial breathing modes, respectively. The electron localization is ascribed to the structural distortion of Au37 in the excited state induced by the strong coherent vibrations. The electron localization phenomenon we observed provides unique physical insight into one-dimensional gold nanoclusters and other nanostructures, which will advance their applications in solar-energy storage and conversion.« less

  8. Electron localization in rod-shaped triicosahedral gold nanocluster

    DOE PAGES

    Zhou, Meng; Jin, Renxi; Sfeir, Matthew Y.; ...

    2017-05-30

    Atomically precise gold nanocluster based on linear assembly of repeating icosahedrons (clusters of clusters) is a unique type of linear nanostructure, which exhibits strong near-infrared absorption as their free electrons are confined in a one-dimensional quantum box. There is little known about the carrier dynamics in these nanoclusters, which limit their energy-related applications. We reported the observation of exciton localization in triicosahedral Au37 nanoclusters (0.5 nm in diameter and 1.6 nm in length) by measuring femtosecond and nanosecond carrier dynamics. Upon photoexcitation to S1 electronic state, electrons in Au37 undergo ~100-ps localization from the two vertexes of three icosahedrons tomore » one vertex, forming a long-lived S1* state. Such phenomenon is not observed in Au25 (dimer) and Au13 (monomer) consisting of two and one icosahedrons, respectively. We have further observed temperature dependence on the localization process, which proves it is thermally driven. Two excited-state vibration modes with frequencies of 20 and 70 cm -1 observed in the kinetic traces are assigned to the axial and radial breathing modes, respectively. The electron localization is ascribed to the structural distortion of Au37 in the excited state induced by the strong coherent vibrations. The electron localization phenomenon we observed provides unique physical insight into one-dimensional gold nanoclusters and other nanostructures, which will advance their applications in solar-energy storage and conversion.« less

  9. Role of non-local exchange in the electronic structure of correlated oxides

    NASA Astrophysics Data System (ADS)

    Iori, Federico; Gatti, Matteo; Rubio Secades, Angel

    Transition-metal oxides (TMO) with partially filled d or f shells are a prototype of correlated materials. They exhibit very interesting properties, like metal-insulator phase transitions (MIT). In this work we consider several TMO insulators in which Kohn-Sham LDA band structures are metallic: VO2, V2O3, Ti2O3, LaTiO3 and YTiO3. In the past, this failure of LDA has been explained in terms of its inadequacy to capture the strong interactions taking place between correlated electrons. In the spirit of the Hubbard model, possible corrections to improve onsite correlation are the LDA +U and LDA +DMFT approaches. Here we make use of the HSE06 hybrid functional. We show that, without invoking strong-correlation effects, the contribution of the non-local Fock exchange is essential to correct the LDA results, by curing its delocalization error. In fact, HSE06 provides insulating band structures and correctly describes the MIT in all the considered compounds. We further discuss the advantages and the limitations of the HSE06 hybrid functional in correlated TMO

  10. CoCrMo cellular structures made by Electron Beam Melting studied by local tomography and finite element modelling

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

    Petit, Clémence; Maire, Eric, E-mail: eric.maire@insa-lyon.fr; Meille, Sylvain

    The work focuses on the structural and mechanical characterization of Co-Cr-Mo cellular samples with cubic pore structure made by Electron Beam Melting (EBM). X-ray tomography was used to characterize the architecture of the sample. High resolution images were also obtained thanks to local tomography in which the specimen is placed close to the X-ray source. These images enabled to observe some defects due to the fabrication process: small pores in the solid phase, partially melted particles attached to the surface. Then, in situ compression tests were performed in the tomograph. The images of the deformed sample show a progressive bucklingmore » of the vertical struts leading to final fracture. The deformation initiated where the defects were present in the strut i.e. in regions with reduced local thickness. The finite element modelling confirmed the high stress concentrations of these weak points leading to the fracture of the sample. - Highlights: • CoCrMo samples fabricated by Electron Beam Melting (EBM) process are considered. • X-ray Computed Tomography is used to observe the structure of the sample. • The mechanical properties are tested thanks to an in situ test in the tomograph. • A finite element model is developed to model the mechanical behaviour.« less

  11. Surface and local electronic structure modification of MgO film using Zn and Fe ion implantation

    NASA Astrophysics Data System (ADS)

    Singh, Jitendra Pal; Lim, Weon Cheol; Lee, Jihye; Song, Jonghan; Lee, Ik-Jae; Chae, Keun Hwa

    2018-02-01

    Present work is motivated to investigate the surface and local electronic structure modifications of MgO films implanted with Zn and Fe ions. MgO film was deposited using radio frequency sputtering method. Atomic force microscopy measurements exhibit morphological changes associated with implantation. Implantation of Fe and Zn ions leads to the reduction of co-ordination geometry of Mg2+ ions in host lattice. The effect is dominant at bulk of film rather than surface as the large concentration of implanted ions resides inside bulk. Moreover, the evidences of interaction among implanted ions and oxygen are not being observed using near edge fine structure measurements.

  12. Forging Fast Ion Conducting Nanochannels with Swift Heavy Ions: The Correlated Role of Local Electronic and Atomic Structure

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

    Sachan, Ritesh; Cooper, Valentino R.; Liu, Bin

    2016-12-19

    Atomically disordered oxides have attracted significant attention in recent years due to the possibility of enhanced ionic conductivity. However, the correlation between atomic disorder, corresponding electronic structure, and the resulting oxygen diffusivity is not well understood. The disordered variants of the ordered pyrochlore structure in gadolinium titanate (Gd 2Ti 2O 7) are seen as a particularly interesting prospect due to intrinsic presence of a vacant oxygen site in the unit atomic structure, which could provide a channel for fast oxygen conduction. In this paper, we provide insights into the subangstrom scale on the disordering-induced variations in the local atomic environmentmore » and its effect on the electronic structure in high-energy ion irradiation-induced disordered nanochannels, which can be utilized as pathways for fast oxygen ion transport. With the help of an atomic plane-by-plane-resolved analyses, the work shows how the presence of various types of TiO x polyhedral that exist in the amorphous and disordered crystalline phase modify the electronic structures relative to the ordered pyrochlore phase in Gd 2Ti 2O 7. Finally, the correlated molecular dynamics simulations on the disordered structures show a remarkable enhancement in oxygen diffusivity as compared with ordered pyrochlore lattice and make that a suitable candidate for applications requiring fast oxygen conduction.« less

  13. Modification of electronic structure, magnetic structure, and topological phase of bismuthene by point defects

    NASA Astrophysics Data System (ADS)

    Kadioglu, Yelda; Kilic, Sevket Berkay; Demirci, Salih; Aktürk, O. Üzengi; Aktürk, Ethem; Ciraci, Salim

    2017-12-01

    This paper reveals how the electronic structure, magnetic structure, and topological phase of two-dimensional (2D), single-layer structures of bismuth are modified by point defects. We first showed that a free-standing, single-layer, hexagonal structure of bismuth, named h-bismuthene, exhibits nontrivial band topology. We then investigated interactions between single foreign adatoms and bismuthene structures, which comprise stability, bonding, electronic structure, and magnetic structures. Localized states in diverse locations of the band gap and resonant states in band continua of bismuthene are induced upon the adsorption of different adatoms, which modify electronic and magnetic properties. Specific adatoms result in reconstruction around the adsorption site. Single vacancies and divacancies can form readily in bismuthene structures and remain stable at high temperatures. Through rebondings, Stone-Whales-type defects are constructed by divacancies, which transform into a large hole at high temperature. Like adsorbed adatoms, vacancies induce also localized gap states, which can be eliminated through rebondings in divacancies. We also showed that not only the optical and magnetic properties, but also the topological features of pristine h-bismuthene can be modified by point defects. The modification of the topological features depends on the energies of localized states and also on the strength of coupling between point defects.

  14. Identifying local structural states in atomic imaging by computer vision

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

    Laanait, Nouamane; Ziatdinov, Maxim; He, Qian

    The availability of atomically resolved imaging modalities enables an unprecedented view into the local structural states of materials, which manifest themselves by deviations from the fundamental assumptions of periodicity and symmetry. Consequently, approaches that aim to extract these local structural states from atomic imaging data with minimal assumptions regarding the average crystallographic configuration of a material are indispensable to advances in structural and chemical investigations of materials. Here, we present an approach to identify and classify local structural states that is rooted in computer vision. This approach introduces a definition of a structural state that is composed of both localmore » and non-local information extracted from atomically resolved images, and is wholly untethered from the familiar concepts of symmetry and periodicity. Instead, this approach relies on computer vision techniques such as feature detection, and concepts such as scale-invariance. We present the fundamental aspects of local structural state extraction and classification by application to simulated scanning transmission electron microscopy images, and analyze the robustness of this approach in the presence of common instrumental factors such as noise, limited spatial resolution, and weak contrast. Finally, we apply this computer vision-based approach for the unsupervised detection and classification of local structural states in an experimental electron micrograph of a complex oxides interface, and a scanning tunneling micrograph of a defect engineered multilayer graphene surface.« less

  15. Identifying local structural states in atomic imaging by computer vision

    DOE PAGES

    Laanait, Nouamane; Ziatdinov, Maxim; He, Qian; ...

    2016-11-02

    The availability of atomically resolved imaging modalities enables an unprecedented view into the local structural states of materials, which manifest themselves by deviations from the fundamental assumptions of periodicity and symmetry. Consequently, approaches that aim to extract these local structural states from atomic imaging data with minimal assumptions regarding the average crystallographic configuration of a material are indispensable to advances in structural and chemical investigations of materials. Here, we present an approach to identify and classify local structural states that is rooted in computer vision. This approach introduces a definition of a structural state that is composed of both localmore » and non-local information extracted from atomically resolved images, and is wholly untethered from the familiar concepts of symmetry and periodicity. Instead, this approach relies on computer vision techniques such as feature detection, and concepts such as scale-invariance. We present the fundamental aspects of local structural state extraction and classification by application to simulated scanning transmission electron microscopy images, and analyze the robustness of this approach in the presence of common instrumental factors such as noise, limited spatial resolution, and weak contrast. Finally, we apply this computer vision-based approach for the unsupervised detection and classification of local structural states in an experimental electron micrograph of a complex oxides interface, and a scanning tunneling micrograph of a defect engineered multilayer graphene surface.« less

  16. Magnetic field effects on the local electronic structure near a single impurity in Graphene

    NASA Astrophysics Data System (ADS)

    Yang, Ling; Zhu, Jian-Xin; Tsai, Shan-Wen

    2011-03-01

    Impurities in graphene can have a significant effect on the local electronic structure of graphene when the Fermi level is near the Dirac point. We study the problem of an isolated impurity in a single layer graphene in the presence of a perpendicular magnetic field. We use a linearization approximation for the energy dispersion and employ a T-matrix formalism to calculate the Green's function. We investigate the effect of an external magnetic field on the Friedel oscillations and impurity-induced resonant states. Different types of impurities, such as vacancies, substitutional impurities, and adatoms, are also considered. LY and SWT acknowledge financial support from NSF(DMR-0847801)and from the UC Lab Fees Research Program.

  17. First-principle simulations of electronic structure in semicrystalline polyethylene

    NASA Astrophysics Data System (ADS)

    Moyassari, A.; Unge, M.; Hedenqvist, M. S.; Gedde, U. W.; Nilsson, F.

    2017-05-01

    In order to increase our fundamental knowledge about high-voltage cable insulation materials, realistic polyethylene (PE) structures, generated with a novel molecular modeling strategy, have been analyzed using first principle electronic structure simulations. The PE structures were constructed by first generating atomistic PE configurations with an off-lattice Monte Carlo method and then equilibrating the structures at the desired temperature and pressure using molecular dynamics simulations. Semicrystalline, fully crystalline and fully amorphous PE, in some cases including crosslinks and short-chain branches, were analyzed. The modeled PE had a structure in agreement with established experimental data. Linear-scaling density functional theory (LS-DFT) was used to examine the electronic structure (e.g., spatial distribution of molecular orbitals, bandgaps and mobility edges) on all the materials, whereas conventional DFT was used to validate the LS-DFT results on small systems. When hybrid functionals were used, the simulated bandgaps were close to the experimental values. The localization of valence and conduction band states was demonstrated. The localized states in the conduction band were primarily found in the free volume (result of gauche conformations) present in the amorphous regions. For branched and crosslinked structures, the localized electronic states closest to the valence band edge were positioned at branches and crosslinks, respectively. At 0 K, the activation energy for transport was lower for holes than for electrons. However, at room temperature, the effective activation energy was very low (˜0.1 eV) for both holes and electrons, which indicates that the mobility will be relatively high even below the mobility edges and suggests that charge carriers can be hot carriers above the mobility edges in the presence of a high electrical field.

  18. The electron localization as the information content of the conditional pair density

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

    Urbina, Andres S.; Torres, F. Javier; Universidad San Francisco de Quito

    2016-06-28

    In the present work, the information gained by an electron for “knowing” about the position of another electron with the same spin is calculated using the Kullback-Leibler divergence (D{sub KL}) between the same-spin conditional pair probability density and the marginal probability. D{sub KL} is proposed as an electron localization measurement, based on the observation that regions of the space with high information gain can be associated with strong correlated localized electrons. Taking into consideration the scaling of D{sub KL} with the number of σ-spin electrons of a system (N{sup σ}), the quantity χ = (N{sup σ} − 1) D{sub KL}f{submore » cut} is introduced as a general descriptor that allows the quantification of the electron localization in the space. f{sub cut} is defined such that it goes smoothly to zero for negligible densities. χ is computed for a selection of atomic and molecular systems in order to test its capability to determine the region in space where electrons are localized. As a general conclusion, χ is able to explain the electron structure of molecules on the basis of chemical grounds with a high degree of success and to produce a clear differentiation of the localization of electrons that can be traced to the fluctuation in the average number of electrons in these regions.« less

  19. Effect of the lattice dynamics on the electronic structure of paramagnetic NiO within the disordered local moment picture

    NASA Astrophysics Data System (ADS)

    Mozafari, Elham; Alling, Björn; Belov, Maxim P.; Abrikosov, Igor A.

    2018-01-01

    Using the disordered local moments approach in combination with the ab initio molecular dynamics method, we simulate the behavior of a paramagnetic phase of NiO at finite temperatures to investigate the effect of magnetic disorder, thermal expansion, and lattice vibrations on its electronic structure. In addition, we study its lattice dynamics. We verify the reliability of our theoretical scheme via comparison of our results with available experiment and earlier theoretical studies carried out within static approximations. We present the phonon dispersion relations for the paramagnetic rock-salt (B1) phase of NiO and demonstrate that it is dynamically stable. We observe that including the magnetic disorder to simulate the paramagnetic phase has a small yet visible effect on the band gap. The amplitude of the local magnetic moment of Ni ions from our calculations for both antiferromagnetic and paramagnetic phases agree well with other theoretical and experimental values. We demonstrate that the increase of temperature up to 1000 K does not affect the electronic structure strongly. Taking into account the lattice vibrations and thermal expansion at higher temperatures have a major impact on the electronic structure, reducing the band gap from ˜3.5 eV at 600 K to ˜2.5 eV at 2000 K. We conclude that static lattice approximations can be safely employed in simulations of the paramagnetic state of NiO up to relatively high temperatures (˜1000 K), but as we get closer to the melting temperature vibrational effects become quite large and therefore should be included in the calculations.

  20. Holographic Reconstruction of Photoelectron Diffraction and Its Circular Dichroism for Local Structure Probing

    NASA Astrophysics Data System (ADS)

    Matsui, Fumihiko; Matsushita, Tomohiro; Daimon, Hiroshi

    2018-06-01

    The local atomic structure around a specific element atom can be recorded as a photoelectron diffraction pattern. Forward focusing peaks and diffraction rings around them indicate the directions and distances from the photoelectron emitting atom to the surrounding atoms. The state-of-the-art holography reconstruction algorithm enables us to image the local atomic arrangement around the excited atom in a real space. By using circularly polarized light as an excitation source, the angular momentum transfer from the light to the photoelectron induces parallax shifts in these diffraction patterns. As a result, stereographic images of atomic arrangements are obtained. These diffraction patterns can be used as atomic-site-resolved probes for local electronic structure investigation in combination with spectroscopy techniques. Direct three-dimensional atomic structure visualization and site-specific electronic property analysis methods are reviewed. Furthermore, circular dichroism was also found in valence photoelectron and Auger electron diffraction patterns. The investigation of these new phenomena provides hints for the development of new techniques for local structure probing.

  1. Correlation of Calculated Halonium Ion Structures with Experimental Product Distributions from Terminal Alkenes: The Effect of Electron-Withdrawing Fluorine Substituents on the Structure and Charge Localization of Halonium Ions (PREPRINT)

    DTIC Science & Technology

    2006-04-03

    2) Substituting a vinyl hydrogen with a fluorine presents an interesting situation for electrophilic reactions. The π-bond is less...reactive toward electrophiles due to the electron-withdrawing effect of the vinyl fluorine . Therefore, carbocations or radical cations are destabilized...NUMBER Distributions from Terminal Alkenes: The Effect of Electron-Withdrawing Fluorine Substituents on the Structure and Charge Localization of

  2. Structure and Electronic Properties of Interface-Confined Oxide Nanostructures

    DOE PAGES

    Liu, Yun; Ning, Yanxiao; Yu, Liang; ...

    2017-09-16

    The controlled fabrication of nanostructures has often made use of a substrate template to mediate and control the growth kinetics. Electronic substrate-mediated interactions have been demonstrated to guide the assembly of organic molecules or the nucleation of metal atoms but usually at cryogenic temperatures, where the diffusion has been limited. Combining STM, STS, and DFT studies, we report that the strong electronic interaction between transition metals and oxides could indeed govern the growth of low-dimensional oxide nanostructures. As a demonstration, a series of FeO triangles, which are of the same structure and electronic properties but with different sizes (side lengthmore » >3 nm), are synthesized on Pt(111). The strong interfacial interaction confines the growth of FeO nanostructures, leading to a discrete size distribution and a uniform step structure. Given the same interfacial configuration, as-grown FeO nanostructures not only expose identical edge/surface structure but also exhibit the same electronic properties, as manifested by the local density of states and local work functions. We expect the interfacial confinement effect can be generally applied to control the growth of oxide nanostructures on transition metal surfaces. These oxide nanostructures of the same structure and electronic properties are excellent models for studies of nanoscale effects and applications.« less

  3. Structure and Electronic Properties of Interface-Confined Oxide Nanostructures

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

    Liu, Yun; Ning, Yanxiao; Yu, Liang

    The controlled fabrication of nanostructures has often made use of a substrate template to mediate and control the growth kinetics. Electronic substrate-mediated interactions have been demonstrated to guide the assembly of organic molecules or the nucleation of metal atoms but usually at cryogenic temperatures, where the diffusion has been limited. Combining STM, STS, and DFT studies, we report that the strong electronic interaction between transition metals and oxides could indeed govern the growth of low-dimensional oxide nanostructures. As a demonstration, a series of FeO triangles, which are of the same structure and electronic properties but with different sizes (side lengthmore » >3 nm), are synthesized on Pt(111). The strong interfacial interaction confines the growth of FeO nanostructures, leading to a discrete size distribution and a uniform step structure. Given the same interfacial configuration, as-grown FeO nanostructures not only expose identical edge/surface structure but also exhibit the same electronic properties, as manifested by the local density of states and local work functions. We expect the interfacial confinement effect can be generally applied to control the growth of oxide nanostructures on transition metal surfaces. These oxide nanostructures of the same structure and electronic properties are excellent models for studies of nanoscale effects and applications.« less

  4. Fast probe of local electronic states in nanostructures utilizing a single-lead quantum dot

    PubMed Central

    Otsuka, Tomohiro; Amaha, Shinichi; Nakajima, Takashi; Delbecq, Matthieu R.; Yoneda, Jun; Takeda, Kenta; Sugawara, Retsu; Allison, Giles; Ludwig, Arne; Wieck, Andreas D.; Tarucha, Seigo

    2015-01-01

    Transport measurements are powerful tools to probe electronic properties of solid-state materials. To access properties of local electronic states in nanostructures, such as local density of states, electronic distribution and so on, micro-probes utilizing artificial nanostructures have been invented to perform measurements in addition to those with conventional macroscopic electronic reservoirs. Here we demonstrate a new kind of micro-probe: a fast single-lead quantum dot probe, which utilizes a quantum dot coupled only to the target structure through a tunneling barrier and fast charge readout by RF reflectometry. The probe can directly access the local electronic states with wide bandwidth. The probe can also access more electronic states, not just those around the Fermi level, and the operations are robust against bias voltages and temperatures. PMID:26416582

  5. Local electronic structure and ferromagnetic interaction in La(Co,Ni)O3

    NASA Astrophysics Data System (ADS)

    Schuppler, S.; Nagel, P.; Fuchs, D.; Löhneysen, H. V.; Merz, M.; Huang, M.-J.

    Perovskite-related transition-metal oxides exhibit properties ranging from insulating to superconducting as well as unusual magnetic phases, and cobaltates, in particular, have been known for their propensity for spin-state transitions. Nonmagnetic LaCoO3 and paramagnetic LaNiO3 are parent compounds for the La(Co1-xNix) O3 (LCNO) family, which, for intermediate Ni content x, exhibits ferromagnetism. The local electronic structure and the ferromagnetic interaction in LCNO have been studied by x-ray absorption (XAS) and x-ray magnetic circular dichroism (XMCD). XAS indicates a mixed-valence state for both Co and Ni, with both valences changing systematically with increasing x. Simultaneously, a spin-state redistribution towards HS (Co site) and LS (Ni site) occurs, and temperature-dependent spin-state transitions are increasingly suppressed. XMCD identifies the element-specific contributions to the magnetic moment and interactions. A simple model based on a double-exchange-like mechanism between Co3+ HS and Ni3+HS can qualitatively account for the evolution of ferromagnetism in the LCNO series.

  6. Virtual scanning tunneling microscopy: A local spectroscopic probe of two-dimensional electron systems

    NASA Astrophysics Data System (ADS)

    Sciambi, A.; Pelliccione, M.; Bank, S. R.; Gossard, A. C.; Goldhaber-Gordon, D.

    2010-09-01

    We propose a probe technique capable of performing local low-temperature spectroscopy on a two-dimensional electron system (2DES) in a semiconductor heterostructure. Motivated by predicted spatially-structured electron phases, the probe uses a charged metal tip to induce electrons to tunnel locally, directly below the tip, from a "probe" 2DES to a "subject" 2DES of interest. We test this concept with large-area (nonscanning) tunneling measurements, and predict a high spatial resolution and spectroscopic capability, with minimal influence on the physics in the subject 2DES.

  7. Correlating electronic transport to atomic structures in self-assembled quantum wires.

    PubMed

    Qin, Shengyong; Kim, Tae-Hwan; Zhang, Yanning; Ouyang, Wenjie; Weitering, Hanno H; Shih, Chih-Kang; Baddorf, Arthur P; Wu, Ruqian; Li, An-Ping

    2012-02-08

    Quantum wires, as a smallest electronic conductor, are expected to be a fundamental component in all quantum architectures. The electronic conductance in quantum wires, however, is often dictated by structural instabilities and electron localization at the atomic scale. Here we report on the evolutions of electronic transport as a function of temperature and interwire coupling as the quantum wires of GdSi(2) are self-assembled on Si(100) wire-by-wire. The correlation between structure, electronic properties, and electronic transport are examined by combining nanotransport measurements, scanning tunneling microscopy, and density functional theory calculations. A metal-insulator transition is revealed in isolated nanowires, while a robust metallic state is obtained in wire bundles at low temperature. The atomic defects lead to electron localizations in isolated nanowire, and interwire coupling stabilizes the structure and promotes the metallic states in wire bundles. This illustrates how the conductance nature of a one-dimensional system can be dramatically modified by the environmental change on the atomic scale. © 2012 American Chemical Society

  8. Electronic and structural properties of Lu under pressure: Relation to structural phases of the rare-earth metals

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

    Min, B.I.; Oguchi, T.; Jansen, H.J.F.

    1986-07-15

    Ground-state electronic and structural properties of Lu under pressure are investigated with use of the self-consistent all-electron total-energy linear muffin-tin orbital band-structure method within a local-density-functional approximation. Pressure-induced structural transitions are found to occur in the following sequence: hcp--(Sm-type)--dhcp--fcc, which is the same as that observed in the crystal structures of the trivalent rare-earth metals with decreasing atomic number. This structural transition is correlated with the increase in the number of d-italic electrons under pressure.

  9. Extended electron energy loss fine structure simulation of the local boron environment in sodium aluminoborosilicate glasses containing gadolinium

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

    Qian, Morris; Li, Hong; Li, Liyu

    Gadolinium can be dissolved in sodium-alumino-borosilicate glasses up to 47 wt% in a baseline borosilicate glass (mol%) 20 B2O3, 5 Al2O3, 60 SiO2,and 20 Na2O. Understanding of Gd dissolution in borosilicate melts is important in glass formulation optimization. Electron energy loss fine structure (ELFS) spectroscopy is chosen, which provides well resolved local atomic structure information for both amorphous and crystalline materials with high sensitivity to low Z elements such as Al, B, Na, O, and Si where the x-ray absorption fine structure (XAFS) technique faces experimental difficulty. In this study, we report our results of boron K-edge ELFS study. Twomore » borosilicate glass samples with 30 and 47 mass% Gd2O3, B20Gd30 and B20Gd47were chosen for B K-edge ELFS study. EEL spectra were acquired on a Philips 430 TEM equipped with Gatan PEELS system 666 and EL/P 2.1 software with Custom function AcqLong. The ELFS data analysis was performed using UWELFS, UWXAFS and FEFF software. From our Gd solubility study, the local structure of Gd in the borate environment possibly resembles double chain structure found in crystalline Gd(BO2)3 as proposed by Chakraborty et al. The B/Gd ratio's in both glasses are smaller then 3, which means the excess Gd atoms in the Si-sites would be 17 and 60 mol% of the total Gd atoms, respectively according to the model, yet the local environment of borate sites saturated with Gd should be remained. To verity above hypothesis, the double chain structure model was applied to fit boron K-edge. The model was shown to well fit experimental boron K-edge EELS spectra for both glasses with some degree of distance distortion which is understandable in amorphous structure. Therefore, it is very likely that Gd stabilized in borate sites has a local structure resembling the double chain Gd(BO2)3 structure as proposed by our solubility study and literature.« less

  10. Bulk and surface electronic structures of MgO

    NASA Astrophysics Data System (ADS)

    Schönberger, U.; Aryasetiawan, F.

    1995-09-01

    The bulk electronic structure of MgO is calculated from first principles including correlation effects within the GW approximation. The band gap, the position of the 2s O band, and the valence band width are in good agreement with experiment. From the quasiparticle band structure, optical transitions corresponding to the main optical absorption peaks are identified. The energy-loss spectrum is also calculated and compared with experiment. The surface electronic structure of MgO(100) is calculated self-consistently within the local-density approximation. It is found that states observed in a recent photoemission experiment outside the bulk allowed states are close to surface states.

  11. Electronic structure of PrBa2Cu3O7: A local-spin-density approximation with on-site Coulomb interaction

    NASA Astrophysics Data System (ADS)

    Biagini, M.; Calandra, C.; Ossicini, Stefano

    1995-10-01

    Electronic structure calculations based on the local-spin-density approximation (LSDA) fail to reproduce the antiferromagnetic ground state of PrBa2Cu3O7 (PBCO). We have performed linear muffin-tin orbital-atomic sphere approximation calculations, based on the local-spin-density approximation with on-site Coulomb correlation applied to Cu(1) and Cu(2) 3d states. We have found that inclusion of the on-site Coulomb interaction modifies qualitatively the electronic structure of PBCO with respect to the LSDA results, and gives Cu spin moments in good agreement with the experimental values. The Cu(2) upper Hubbard band lies about 1 eV above the Fermi energy, indicating a CuII oxidation state. On the other hand, the Cu(1) upper Hubbard band is located across the Fermi level, which implies an intermediate oxidation state for the Cu(1) ion, between CuI and CuII. The metallic character of the CuO chains is preserved, in agreement with optical reflectivity [K. Takenaka et al., Phys. Rev. B 46, 5833 (1992)] and positron annihilation experiments [L. Hoffmann et al., Phys. Rev. Lett. 71, 4047 (1993)]. These results support the view of an extrinsic origin of the insulating character of PrBa2Cu3O7.

  12. Electronic and structural ground state of heavy alkali metals at high pressure

    DOE PAGES

    Fabbris, G.; Lim, J.; Veiga, L. S. I.; ...

    2015-02-17

    Here, alkali metals display unexpected properties at high pressure, including emergence of low symmetry crystal structures, that appear to occur due to enhanced electronic correlations among the otherwise nearly-free conduction electrons. We investigate the high pressure electronic and structural ground state of K, Rb, and Cs using x-ray absorption spectroscopy and x-ray diffraction measurements together with ab initio theoretical calculations. The sequence of phase transitions under pressure observed at low temperature is similar in all three heavy alkalis except for the absence of the oC84 phase in Cs. Both the experimental and theoretical results point to pressure-enhanced localization of themore » valence electrons characterized by pseudo-gap formation near the Fermi level and strong spd hybridization. Although the crystal structures predicted to host magnetic order in K are not observed, the localization process appears to drive these alkalis closer to a strongly correlated electron state.« less

  13. Electronic and structural ground state of heavy alkali metals at high pressure

    NASA Astrophysics Data System (ADS)

    Fabbris, G.; Lim, J.; Veiga, L. S. I.; Haskel, D.; Schilling, J. S.

    2015-02-01

    Alkali metals display unexpected properties at high pressure, including emergence of low-symmetry crystal structures, which appear to occur due to enhanced electronic correlations among the otherwise nearly free conduction electrons. We investigate the high-pressure electronic and structural ground state of K, Rb, and Cs using x-ray absorption spectroscopy and x-ray diffraction measurements together with a b i n i t i o theoretical calculations. The sequence of phase transitions under pressure observed at low temperature is similar in all three heavy alkalis except for the absence of the o C 84 phase in Cs. Both the experimental and theoretical results point to pressure-enhanced localization of the valence electrons characterized by pseudogap formation near the Fermi level and strong s p d hybridization. Although the crystal structures predicted to host magnetic order in K are not observed, the localization process appears to drive these alkalis closer to a strongly correlated electron state.

  14. Local atomic and electronic structures of epitaxial strained LaCoO3 thin films

    NASA Astrophysics Data System (ADS)

    Sterbinsky, G. E.; Ryan, P. J.; Kim, J.-W.; Karapetrova, E.; Ma, J. X.; Shi, J.; Woicik, J. C.

    2012-01-01

    We have examined the atomic and electronic structures of perovskite lanthanum cobaltite (LaCoO3) thin films using Co K-edge x-ray absorption fine structure (XAFS) spectroscopy. Extended XAFS (EXAFS) demonstrates that a large difference between in-plane and out-of-plane Co-O bond lengths results from tetragonal distortion in highly strained films. The structural distortions are strongly coupled to the hybridization between atomic orbitals of the Co and O atoms, as shown by x-ray absorption near edge spectroscopy (XANES). Our results indicate that increased hybridization is not the cause of ferromagnetism in strained LaCoO3 films. Instead, we suggest that the strain-induced distortions of the oxygen octahedra increase the population of eg electrons and concurrently depopulate t2g electrons beyond a stabilization threshold for ferromagnetic order.

  15. Electronic structure and magneto-optical effects in CeSb

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

    Liechtenstein, A.I.; Antropov, V.P.; Harmon, B.N.

    1994-04-15

    The electronic structure and magneto-optical spectra of CeSb have been calculated using the self-consistent local-density approximation with explicit on-site Coulomb parameters for the correlated [ital f] state of cerium. The essential electronic structure of cerium antimonide consists of one occupied [ital f] band, predominantly with orbital [ital m]=[minus]3 character and spin [sigma]=1 located 2 eV below the Fermi level and interacting with broad Sb [ital p] bands crossing [ital E][sub [ital F

  16. Distortion of Local Atomic Structures in Amorphous Ge-Sb-Te Phase Change Materials

    NASA Astrophysics Data System (ADS)

    Hirata, A.; Ichitsubo, T.; Guan, P. F.; Fujita, T.; Chen, M. W.

    2018-05-01

    The local atomic structures of amorphous Ge-Sb-Te phase-change materials have yet to be clarified and the rapid crystal-amorphous phase change resulting in distinct optical contrast is not well understood. We report the direct observation of local atomic structures in amorphous Ge2Sb2Te5 using "local" reverse Monte Carlo modeling dedicated to an angstrom-beam electron diffraction analysis. The results corroborated the existence of local structures with rocksalt crystal-like topology that were greatly distorted compared to the crystal symmetry. This distortion resulted in the breaking of ideal octahedral atomic environments, thereby forming local disordered structures that basically satisfied the overall amorphous structure factor. The crystal-like distorted octahedral structures could be the main building blocks in the formation of the overall amorphous structure of Ge-Sb-Te.

  17. Analysis of Local Structure, Chemistry and Bonding by Electron Energy Loss Spectroscopy

    NASA Astrophysics Data System (ADS)

    Mayer, Joachim

    In the present chapter, the reader will first be introduced briefly to the basic principles of analytical transmission electron microscopy (ATEM) with special emphasis on electron energy-loss spectroscopy (EELS) and energy-filtering TEM. The quantification of spectra to obtain chemical information and the origin and interpretation of near-edge fine structures in EELS (ELNES) are discussed. Special attention will be given to the characterization of internal interfaces and the literature in this area will be reviewed. Selected examples of the application of ATEM in the investigation of internal interfaces will be given. These examples include both EELS in the energy-filtering TEM and in the scanning transmission electron microscope (STEM).

  18. Electronic structure of antibiotic erythromycin

    NASA Astrophysics Data System (ADS)

    Novak, Igor; Kovač, Branka

    2015-03-01

    The electronic structure of erythromycin A (ERYMA) molecule has been studied by UV photoelectron spectroscopy and assigned (in the low ionization energy region only) by empirical arguments. The two orbitals with highest energy (lowest ionization energy) are localized on the nitrogen of the desosamine sugar functional group and on the ester group of macrolide (lactone) ring. We discuss how these orbital energies can help to rationalize the known mode of binding of ERYMA to their biological receptors.

  19. Local and electronic structure around manganese in Cd0.98Mn0.02Te0.97Se0.03 studied by XAFS

    NASA Astrophysics Data System (ADS)

    Radisavljević, I.; Novaković, N.; Romčević, N.; Ivanović, N.

    2013-04-01

    X-ray Absorption Fine Structure (XAFS) technique was employed to study local electronic and structural features of Mn ions incorporated in Cd0.98Mn0.02Te0.97Se0.03. XAFS measurements performed at Mn K edge revealed that manganese Mn(II) ions are well incorporated into the host CdTe lattice (cubic zinc-blende structure type) and their immediate surrounding is found to be composed exclusively of Te atoms. The observed preference of Mn ions distribution around Te opposes earlier observations on the similar systems, where preferential Mn-Se over Mn-Te paring was found.

  20. Structural and electronic properties of the alkali metal incommensurate phases

    NASA Astrophysics Data System (ADS)

    Woolman, Gavin; Naden Robinson, Victor; Marqués, Miriam; Loa, Ingo; Ackland, Graeme J.; Hermann, Andreas

    2018-05-01

    Under pressure, the alkali elements sodium, potassium, and rubidium adopt nonperiodic structures based on two incommensurate interpenetrating lattices. While all elements form the same "host" lattice, their "guest" lattices are all distinct. The physical mechanism that stabilizes these phases is not known, and detailed calculations are challenging due to the incommensurability of the lattices. Using a series of commensurate approximant structures, we tackle this issue using density functional theory calculations. In Na and K, the calculations prove accurate enough to reproduce not only the stability of the host-guest phases, but also the complicated pressure dependence of the host-guest ratio and the two guest-lattice transitions. We find Rb-IV to be metastable at all pressures, and suggest it is a high-temperature phase. The electronic structure of these materials is unique: they exhibit two distinct, coexisting types of electride behavior, with both fully localized pseudoanions and electrons localized in 1D wells in the host lattice, leading to low conductivity. While all phases feature pseudogaps in the electronic density of states, the perturbative free-electron picture applies to Na, but not to K and Rb, due to significant d -orbital population in the latter.

  1. A soft X-ray spectroscopic perspective of electron localization and transport in tungsten doped bismuth vanadate single crystals.

    PubMed

    Jovic, Vedran; Rettie, Alexander J E; Singh, Vijay R; Zhou, Jianshi; Lamoureux, Bethany; Buddie Mullins, C; Bluhm, Hendrik; Laverock, Jude; Smith, Kevin E

    2016-11-23

    Doped BiVO 4 is a promising photoelectrochemical water splitting anode, whose activity is hampered by poor charge transport. Here we use a set of X-ray spectroscopic methods to probe the origin and nature of localized electron states in W:BiVO 4 . Furthermore, using the polarized nature of the X-rays, we probe variations in the electronic structure along the crystal axes. In this manner, we reveal aspects of the electronic structure related to electron localization and observations consistent with conductivity anisotropy between the ab-plane and c-axis. We verify that tungsten substitutes as W 6+ for V 5+ in BiVO 4 . This is shown to result in the presence of inter-band gap states related to electrons at V 4+ sites of e symmetry. The energetic position of the states in the band gap suggest that they are highly localized and may act as recombination centres. Polarization dependent X-ray absorption spectra reveal anisotropy in the electronic structure between the ab-plane and c-axis. Results show the superior hybridization between V 3d and O 2p states, higher V wavefunction overlap and broader conduction bands in the ab-plane than in the c-axis. These insights into the electronic structure are discussed in the context of existing experimental and theoretical reports regarding charge transport in BiVO 4 .

  2. Conductivity and local structure in LaNiO3

    NASA Astrophysics Data System (ADS)

    Fowlie, Jennifer; Gibert, Marta; Tieri, Giulio; Gloter, Alexandre; à+/-Iguez, Jorge; Filippetti, Alessio; Catalano, Sara; Gariglio, Stefano; StéPhan, Odile; Triscone, Jean-Marc

    In this study we approach the thickness-dependence of the properties of LaNiO3 films along multiple, complementary avenues: sophisticated ab initio calculations, scanning transmission electron microscopy and electronic transport. Specifically, we find an unexpected maximum in conductivity in films of thickness 6 - 10 unit cells (3 nm) for several series of LaNiO3 films. Ab initio transport based on the detailed crystal structure also reveals a maximum in conductivity at the same thickness. In agreement with the structure obtained from scanning transmission electron microscopy (STEM), our simulated structures reveal that the substrate- and surface-induced distortions lead to three types of local structure (heterointerface, interior-layer, surface). Based on this observation, a 3-element parallel conductor model neatly reproduces the trend of conductivity with thickness. This study addresses the question of how structural distortions at the atomic scale evolve in a thin film under the influence of the substrate and the surface. This topic is key to the understanding of the physics of heterostructures and the design of functional oxides.

  3. Attractive electron-electron interactions within robust local fitting approximations.

    PubMed

    Merlot, Patrick; Kjærgaard, Thomas; Helgaker, Trygve; Lindh, Roland; Aquilante, Francesco; Reine, Simen; Pedersen, Thomas Bondo

    2013-06-30

    An analysis of Dunlap's robust fitting approach reveals that the resulting two-electron integral matrix is not manifestly positive semidefinite when local fitting domains or non-Coulomb fitting metrics are used. We present a highly local approximate method for evaluating four-center two-electron integrals based on the resolution-of-the-identity (RI) approximation and apply it to the construction of the Coulomb and exchange contributions to the Fock matrix. In this pair-atomic resolution-of-the-identity (PARI) approach, atomic-orbital (AO) products are expanded in auxiliary functions centered on the two atoms associated with each product. Numerical tests indicate that in 1% or less of all Hartree-Fock and Kohn-Sham calculations, the indefinite integral matrix causes nonconvergence in the self-consistent-field iterations. In these cases, the two-electron contribution to the total energy becomes negative, meaning that the electronic interaction is effectively attractive, and the total energy is dramatically lower than that obtained with exact integrals. In the vast majority of our test cases, however, the indefiniteness does not interfere with convergence. The total energy accuracy is comparable to that of the standard Coulomb-metric RI method. The speed-up compared with conventional algorithms is similar to the RI method for Coulomb contributions; exchange contributions are accelerated by a factor of up to eight with a triple-zeta quality basis set. A positive semidefinite integral matrix is recovered within PARI by introducing local auxiliary basis functions spanning the full AO product space, as may be achieved by using Cholesky-decomposition techniques. Local completion, however, slows down the algorithm to a level comparable with or below conventional calculations. Copyright © 2013 Wiley Periodicals, Inc.

  4. Electron and Nucleon Localization Functions of Oganesson: Approaching the Thomas-Fermi Limit

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

    Jerabek, Paul; Schuetrumpf, Bastian; Schwerdtfeger, Peter

    Fermion localization functions are used to discuss electronic and nucleonic shell structure effects in the superheavy element oganesson, the heaviest element discovered to date. Spin-orbit splitting in the 7p electronic shell becomes so large (~10 eV) that Og is expected to show uniform-gas-like behavior in the valence region with a rather large dipole polarizability compared to the lighter rare gas elements. The nucleon localization in Og is also predicted to undergo a transition to the Thomas-Fermi gas behavior in the valence region. Finally, this effect, particularly strong for neutrons, is due to the high density of single-particle orbitals.

  5. Electron and Nucleon Localization Functions of Oganesson: Approaching the Thomas-Fermi Limit

    DOE PAGES

    Jerabek, Paul; Schuetrumpf, Bastian; Schwerdtfeger, Peter; ...

    2018-01-31

    Fermion localization functions are used to discuss electronic and nucleonic shell structure effects in the superheavy element oganesson, the heaviest element discovered to date. Spin-orbit splitting in the 7p electronic shell becomes so large (~10 eV) that Og is expected to show uniform-gas-like behavior in the valence region with a rather large dipole polarizability compared to the lighter rare gas elements. The nucleon localization in Og is also predicted to undergo a transition to the Thomas-Fermi gas behavior in the valence region. Finally, this effect, particularly strong for neutrons, is due to the high density of single-particle orbitals.

  6. Electron and Nucleon Localization Functions of Oganesson: Approaching the Thomas-Fermi Limit

    NASA Astrophysics Data System (ADS)

    Jerabek, Paul; Schuetrumpf, Bastian; Schwerdtfeger, Peter; Nazarewicz, Witold

    2018-02-01

    Fermion localization functions are used to discuss electronic and nucleonic shell structure effects in the superheavy element oganesson, the heaviest element discovered to date. Spin-orbit splitting in the 7 p electronic shell becomes so large (˜10 eV ) that Og is expected to show uniform-gas-like behavior in the valence region with a rather large dipole polarizability compared to the lighter rare gas elements. The nucleon localization in Og is also predicted to undergo a transition to the Thomas-Fermi gas behavior in the valence region. This effect, particularly strong for neutrons, is due to the high density of single-particle orbitals.

  7. Structural and electronic properties of L-amino acids

    NASA Astrophysics Data System (ADS)

    Tulip, P. R.; Clark, S. J.

    2005-05-01

    The structural and electronic properties of four L-amino acids alanine, leucine, isoleucine, and valine have been investigated using density functional theory (DFT) and the generalized gradient approximation. Within the crystals, it is found that the constituent molecules adopt zwitterionic configurations, in agreement with experimental work. Lattice constants are found to be in good agreement with experimentally determined values, although certain discrepancies do exist due to the description of van der Waals interactions. We find that these materials possess wide DFT band gaps in the region of 5 eV, with electrons highly localized to the constituent molecules. It is found that the main mechanisms behind crystal formation are dipolar interactions and hydrogen bonding of a primarily electrostatic character, in agreement with current biochemical understanding of these systems. The electronic structure suggests that the amine and carboxy functional groups are dominant in determining band structure.

  8. Local atomic structure inheritance in Ag{sub 50}Sn{sub 50} melt

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

    Bai, Yanwen; Bian, Xiufang, E-mail: xfbian@sdu.edu.cn; Qin, Jingyu

    2014-01-28

    Local structure inheritance signatures were observed during the alloying process of the Ag{sub 50}Sn{sub 50} melt, using high-temperature X-ray diffraction and ab initio molecular dynamics simulations. The coordination number N{sub m} around Ag atom is similar in the alloy and in pure Ag melts (N{sub m} ∼ 10), while, during the alloying process, the local structure around Sn atoms rearranges. Sn-Sn covalent bonds were substituted by Ag-Sn chemical bonds, and the total coordination number around Sn increases by about 70% as compared with those in the pure Sn melt. Changes in the electronic structure of the alloy have been studied by Agmore » and Sn K-edge X-ray absorption spectroscopy, as well as by calculations of the partial density of states. We propose that a leading mechanism for local structure inheritance in Ag{sub 50}Sn{sub 50} is due to s-p dehybridization of Sn and to the interplay between Sn-s and Ag-d electrons.« less

  9. Structural and electronic properties for atomic clusters

    NASA Astrophysics Data System (ADS)

    Sun, Yan

    We have studied the structural and electronic properties for different groups of atomic clusters by doing a global search on the potential energy surface using the Taboo Search in Descriptors Space (TSDS) method and calculating the energies with Kohn-Sham Density Functional Theory (KS-DFT). Our goal was to find the structural and electronic principles for predicting the structure and stability of clusters. For Ben (n = 3--20), we have found that the evolution of geometric and electronic properties with size reflects a change in the nature of the bonding from van der Waals to metallic and then bulk-like. The cluster sizes with extra stability agree well with the predictions of the jellium model. In the 4d series of transition metal (TM) clusters, as the d-type bonding becomes more important, the preferred geometric structure changes from icosahedral (Y, Zr), to distorted compact structures (Nb, Mo), and FCC or simple cubic crystal fragments (Tc, Ru, Rh) due to the localized nature of the d-type orbital. Analysis of relative isomer energies and their electronic density of states suggest that these clusters tend to follow a maximum hardness principle (MHP). For A4B12 clusters (A is divalent, B is monovalent), we found unusually large (on average 1.95 eV) HOMO-LUMO gap values. This shows the extra stability at an electronic closed shell (20 electrons) predicted by the jellium model. The importance of symmetry, closed electronic and ionic shells in stability is shown by the relative stability of homotops of Mg4Ag12 which also provides support for the hypothesis that clusters that satisfy more than one stability criterion ("double magic") should be particularly stable.

  10. Ripple-modulated electronic structure of a 3D topological insulator.

    PubMed

    Okada, Yoshinori; Zhou, Wenwen; Walkup, D; Dhital, Chetan; Wilson, Stephen D; Madhavan, V

    2012-01-01

    Three-dimensional topological insulators host linearly dispersing states with unique properties and a strong potential for applications. An important ingredient in realizing some of the more exotic states in topological insulators is the ability to manipulate local electronic properties. Direct analogy to the Dirac material graphene suggests that a possible avenue for controlling local properties is via a controlled structural deformation such as the formation of ripples. However, the influence of such ripples on topological insulators is yet to be explored. Here we use scanning tunnelling microscopy to determine the effects of one-dimensional buckling on the electronic properties of Bi(2)Te(3.) By tracking spatial variations of the interference patterns generated by the Dirac electrons we show that buckling imposes a periodic potential, which locally modulates the surface-state dispersion. This suggests that forming one- and two-dimensional ripples is a viable method for creating nanoscale potential landscapes that can be used to control the properties of Dirac electrons in topological insulators.

  11. Electronic structure and electron energy-loss spectroscopy of ZrO2 zirconia

    NASA Astrophysics Data System (ADS)

    Dash, L. K.; Vast, Nathalie; Baranek, Philippe; Cheynet, Marie-Claude; Reining, Lucia

    2004-12-01

    The atomic and electronic structures of zirconia are calculated within density functional theory, and their evolution is analyzed as the crystal-field symmetry changes from tetrahedral [cubic (c-ZrO2) and tetragonal (t-ZrO2) phases] to octahedral (hypothetical rutile ZrO2 ), to a mixing of these symmetries (monoclinic phase, m-ZrO2 ). We find that the theoretical bulk modulus in c-ZrO2 is 30% larger than the experimental value, showing that the introduction of yttria in zirconia has a significant effect. Electronic structure fingerprints which characterize each phase from their electronic spectra are identified. We have carried out electron energy-loss spectroscopy experiments at low momentum transfer and compared these results to the theoretical spectra calculated within the random phase approximation. We show a dependence of the valence and 4p ( N2,3 edge) plasmons on the crystal structure, the dependence of the latter being brought into the spectra by local-field effects. Last, we attribute low energy excitations observed in EELS of m-ZrO2 to defect states 2eV above the top of the intrinsic valence band, and the EELS fundamental band gap value is reconciled with the 5.2 or 5.8eV gaps determined by vacuum ultraviolet spectroscopy.

  12. The [(AI 2O 3) 2] - Anion Cluster: Electron Localization-Delocalization Isomerism

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

    Sierka, Marek; Dobler, Jens; Sauer, Joachim

    2009-10-05

    Three-dimensional bulk alumina and its two-dimensional thin films show great structural diversity, posing considerable challenges to their experimental structural characterization and computational modeling. Recently, structural diversity has also been demonstrated for zerodimensional gas phase aluminum oxide clusters. Mass-selected clusters not only make systematic studies of the structural and electronic properties as a function of size possible, but lately have also emerged as powerful molecular models of complex surfaces and solid catalysts. In particular, the [(Al 2O 3) 3-5] + clusters were the first example of polynuclear maingroup metal oxide cluster that are able to thermally activate CH 4. Over themore » past decades gas phase aluminum oxide clusters have been extensively studied both experimentally and computationally, but definitive structural assignments were made for only a handful of them: the planar [Al 3O 3] - and [Al 5O 4] - cluster anions, and the [(Al 2O 3) 1-4(AlO)] + cluster cations. For stoichiometric clusters only the atomic structures of [(Al 2O 3) 4] +/0 have been nambiguously resolved. Here we report on the structures of the [(Al 2O 3) 2] -/0 clusters combining photoelectron spectroscopy (PES) and quantum chemical calculations employing a genetic algorithm as a global optimization technique. The [(Al 2O 3) 2] - cluster anion show energetically close lying but structurally distinct cage and sheet-like isomers which differ by delocalization/localization of the extra electron. The experimental results are crucial for benchmarking the different computational methods applied with respect to a proper description of electron localization and the relative energies for the isomers which will be of considerable value for future computational studies of aluminum oxide and related systems.« less

  13. Electronic structure of the benzene dimer cation

    NASA Astrophysics Data System (ADS)

    Pieniazek, Piotr A.; Krylov, Anna I.; Bradforth, Stephen E.

    2007-07-01

    The benzene and benzene dimer cations are studied using the equation-of-motion coupled-cluster model with single and double substitutions for ionized systems. The ten lowest electronic states of the dimer at t-shaped, sandwich, and displaced sandwich configurations are described and cataloged based on the character of the constituent fragment molecular orbitals. The character of the states, bonding patterns, and important features of the electronic spectrum are explained using qualitative dimer molecular orbital linear combination of fragment molecular orbital framework. Relaxed ground state geometries are obtained for all isomers. Calculations reveal that the lowest energy structure of the cation has a displaced sandwich structure and a binding energy of 20kcal/mol, while the t-shaped isomer is 6kcal/mol higher. The calculated electronic spectra agree well with experimental gas phase action spectra and femtosecond transient absorption in liquid benzene. Both sandwich and t-shaped structures feature intense charge resonance bands, whose location is very sensitive to the interfragment distance. Change in the electronic state ordering was observed between σ and πu states, which correlate to the B˜ and C˜ bands of the monomer, suggesting a reassignment of the local excitation peaks in the gas phase experimental spectrum.

  14. Localized to itinerant transition of f electrons in ordered Ce films on W(110)

    NASA Astrophysics Data System (ADS)

    Chen, Q. Y.; Feng, W.; Xie, D. H.; Lai, X. C.; Zhu, X. G.; Huang, L.

    2018-04-01

    A key issue to understand the driving force and underlying physics in the isostructural γ -α transition in Cerium is the character of the 4 f states, whether it is localized or itinerant. Here the surface topography and electronic structure of the well-ordered Ce metal films on a W(110) substrate were investigated by using scanning tunneling microscopy, angle-resolved photoemission spectroscopy and density functional theory, and single-site dynamical mean-field theory calculations. Three nearly flat f bands can be observed, and a weakly dispersive quasiparticle band near the Fermi level has been directly observed at low temperature, indicating the hybridization between f electrons and conduction electrons in the low-temperature α phase. The hybridization strength becomes weaker upon increasing temperature, and the f electrons become almost fully localized at 300 K in the high-temperature γ phase. The observed localized-to-itinerant transition of the f electrons with decreasing temperature gives direct experimental proof for the changes of the 4 f character in the isostructural γ -α phase transition. Our results suggest that the character of the f electrons plays a crucial role during the γ -α phase transition.

  15. Electronic Structure of Actinides under Pressure

    NASA Astrophysics Data System (ADS)

    Johansson, Borje

    2006-03-01

    The series of heavy radioactive elements known as the actinides all have similar elemental properties. However, when the volume per atom in the condensed phase is illustrated as a function of atomic number, perhaps the most dramatic anomaly in the periodic table becomes apparent. The atomic volume of americium is almost 50% larger than it is for the preceding element plutonium. For the element after americium, curium, the atomic volume is very close to that of americium. The same holds also for the next elements berkelium and californium. Accordingly from americium and onwards the actinides behave very similar to the corresponding rare-earth elements - a second lanthanide series of metallic elements can be identified. This view is strongly supported by the fact that all these elements adopt the dhcp structure, a structure typical for the lanthanides. The reason for this behavior is found in the behavior of the 5f electrons. For the earlier actinides, up to and including plutonium, the 5f electrons form metallic states and contribute most significantly to the bonding. In Np and Pu they even dominate the bonding, while all of a sudden they become localized in Am, very much like the 4f electrons in the lanthanide series, and contribute no longer to the cohesion. This withdrawal of 5f bonding gives rise to the large volume expansion between plutonium and americium. This difference between the light and heavy actinide suggests that it would be most worthwhile to strongly compress the transplutonium elements, thereby forcing the individual 5f electron wave functions into strong contact with each other (overlap). Recently high pressure experiments have been performed for americium and curium and dramatic crystal structure changes have been observed. These results and other high pressure data will be discussed in relation to the basic electronic structure of these elements.

  16. Electronic structure of metals and semiconductors: bulk, surface, and interface properties

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

    Louie, S.G.S.

    1976-09-01

    A theoretical study of the electronic structure of various metals and semiconductors is presented with the emphasis on understanding the properties of these materials when they are subjected to extreme conditions and in various different configurations. Among the bulk systems studied, the properties of cesium under high pressure are discussed in terms of the electronic structure calculated at various cell volumes using the pseudopotential method. Local fields or umklapp processes in semiconductors are studied within the random phase approximation (RPA). Specifically the dielectric response matrix epsilon/sub GG'/ (q = 0,omega) is evaluated numerically to determine the effects of local-field correctionsmore » in the optical spectrum of Si. Also, some comments on the excitonic mechanism of superconductivity are presented and the role of local fields is discussed. The pseudo-potential method is next extended to calculate the electronic structure of a transition metal Nb. The calculation is performed self-consistently with the use of a non-local ionic potential determined from atomic spectra. Finally the theory of the superconducting transition temperature T/sub c/ is discussed in the strong-coupling formulation of the BCS theory. The Eliashberg equations in the Matsubara representation are solved analytically and a general T/sub c/ equation is obtained. A new method is developed using pseudopotentials in a self-consistent manner to describe non-periodic systems. The method is applicable to localized configurations such as molecules, surfaces, impurities, vacancies, finite chains of atoms, adsorbates, and solid interfaces. Specific applications to surfaces, metal-semiconductor interfaces and vacancies are presented.« less

  17. Electronic structure properties of UO2 as a Mott insulator

    NASA Astrophysics Data System (ADS)

    Sheykhi, Samira; Payami, Mahmoud

    2018-06-01

    In this work using the density functional theory (DFT), we have studied the structural, electronic and magnetic properties of uranium dioxide with antiferromagnetic 1k-, 2k-, and 3k-order structures. Ordinary approximations in DFT, such as the local density approximation (LDA) or generalized gradient approximation (GGA), usually predict incorrect metallic behaviors for this strongly correlated electron system. Using Hubbard term correction for f-electrons, LDA+U method, as well as using the screened Heyd-Scuseria-Ernzerhof (HSE) hybrid functional for the exchange-correlation (XC), we have obtained the correct ground-state behavior as an insulator, with band gaps in good agreement with experiment.

  18. Electronic structure of BaNi2As2

    NASA Astrophysics Data System (ADS)

    Zhou, Bo; Xu, Min; Zhang, Yan; Xu, Gang; He, Cheng; Yang, L. X.; Chen, Fei; Xie, B. P.; Cui, Xiao-Yu; Arita, Masashi; Shimada, Kenya; Namatame, Hirofumi; Taniguchi, Masaki; Dai, X.; Feng, D. L.

    2011-01-01

    BaNi2As2, with a first-order phase transition around 131 K, is studied by the angle-resolved photoemission spectroscopy. The measured electronic structure is compared to the local-density approximation calculations, revealing similar large electronlike bands around M¯ and differences along Γ¯-X¯. We further show that the electronic structure of BaNi2As2 is distinct from that of the sibling iron pnictides. Particularly, there is no signature of band folding, indicating no collinear spin-density-wave-related magnetic ordering. Moreover, across the strong first-order phase transition, the band shift exhibits a hysteresis, which is directly related to the significant lattice distortion in BaNi2As2.

  19. Electronic structure and properties of lanthanum

    NASA Astrophysics Data System (ADS)

    Nixon, Lane; Papaconstantopoulos, Dimitrios

    2008-03-01

    The total energy and electronic structure of lanthanum have been calculated in the bcc, fcc, hcp and dhcp structures for pressures up to 50 GPa. The full potential linearized-augmented-planewave method was used with both the local-density and general-gradient approximations. The correct phase ordering has been found, with lattice parameters and bulk moduli in good agreement with experimental data. The GGA method shows excellent agreement overall while the LDA results show larger discrepancies. The calculated strain energies for the fcc and bcc structures demonstrate the respective stable and unstable configurations at ambient conditions. The calculated superconductivity properties under pressure for the fcc structure are also found to agree well with measurements. Both LDA and GGA, with minor differences, reproduce well the experimental results for Tc.

  20. Delocalized and localized states of eg electrons in half-doped manganites.

    PubMed

    Winkler, E L; Tovar, M; Causa, M T

    2013-07-24

    We have studied the magnetic behaviour of half-doped manganite Y0.5Ca0.5MnO3 in an extended range of temperatures by means of magnetic susceptibility, χ(T), and electron spin resonance (ESR) experiments. At high temperature the system crystallizes in an orthorhombic structure. The resistivity value, ρ ≃ 0.05 Ω cm at 500 K, indicates a metallic behaviour, while the Curie-Weiss dependence of χ(T) and the thermal evolution of the ESR parameters are very well described by a model that considers a system conformed by localized Mn(4+) cores, [Formula: see text], and itinerant, eg, electrons. The strong coupling between t2g and eg electrons results in an enhanced Curie constant and an FM Curie-Weiss temperature that overcomes the AFM interactions between the [Formula: see text] cores. A transition to a more distorted phase is observed at T ≈ 500 K and signatures of localization of the eg electrons appear in the χ(T) behaviour below 300 K. A new Curie-Weiss regime is observed, where the Curie-constant value is consistent with dimer formation. Based on mean-field calculations, the dimer formation is predicted as a function of the interaction strength between the t2g and eg electrons.

  1. Quantum currents and pair correlation of electrons in a chain of localized dots

    NASA Astrophysics Data System (ADS)

    Morawetz, Klaus

    2017-03-01

    The quantum transport of electrons in a wire of localized dots by hopping, interaction and dissipation is calculated and a representation by an equivalent RCL circuit is found. The exact solution for the electric-field induced currents allows to discuss the role of virtual currents to decay initial correlations and Bloch oscillations. The dynamical response function in random phase approximation (RPA) is calculated analytically with the help of which the static structure function and pair correlation function are determined. The pair correlation function contains a form factor from the Brillouin zone and a structure factor caused by the localized dots in the wire.

  2. Interplay of local structure, charge, and spin in bilayered manganese perovskites

    NASA Astrophysics Data System (ADS)

    Rybicki, Damian; Sikora, Marcin; Przewoznik, Janusz; Kapusta, Czesław; Mitchell, John F.

    2018-03-01

    Chemical doping is a reliable method of modification of the electronic properties of transition metal compounds. In manganese perovskites, it leads to charge transfer and peculiar ordering phenomena. However, depending on the interplay of the local crystal structure and electronic properties, synthesis of stable compounds in the entire doping range is often impossible. Here, we show results of high-energy resolution x-ray absorption and emission spectroscopies on a La2 -2 xSr1 +2 xMn2O7 family of bilayered manganites in a broad doping range (0.5 ≤x ≤1 ). We established a relation between local Mn charge and Mn-O distances as a function of doping. Based on a comparison of such relation with other manganites, we suggest why stable structures cannot be realized for certain doping levels of bilayered compounds.

  3. Local electronic structure and photoelectrochemical activity of partial chemically etched Ti-doped hematite

    NASA Astrophysics Data System (ADS)

    Rioult, Maxime; Belkhou, Rachid; Magnan, Hélène; Stanescu, Dana; Stanescu, Stefan; Maccherozzi, Francesco; Rountree, Cindy; Barbier, Antoine

    2015-11-01

    The direct conversion of solar light into chemical energy or fuel through photoelectrochemical water splitting is promising as a clean hydrogen production solution. Ti-doped hematite (Ti:α-Fe2O3) is a potential key photoanode material, which despite its optimal band gap, excellent chemical stability, abundance, non-toxicity and low cost, still has to be improved. Here we give evidence of a drastic improvement of the water splitting performances of Ti-doped hematite photoanodes upon a HCl wet-etching. In addition to the topography investigation by atomic force microscopy, a detailed determination of the local electronic structure has been carried out in order to understand the phenomenon and to provide new insights in the understanding of solar water splitting. Using synchrotron radiation based spectromicroscopy (X-PEEM), we investigated the X-ray absorption spectral features at the L3 Fe edge of the as grown surface and of the wet-etched surface on the very same sample thanks to patterning. We show that HCl wet etching leads to substantial surface modifications of the oxide layer including increased roughness and chemical reduction (presence of Fe2 +) without changing the band gap. We demonstrate that these changes are profitable and correlated to the drastic changes of the photocatalytic activity.

  4. Actinide electronic structure and atomic forces

    NASA Astrophysics Data System (ADS)

    Albers, R. C.; Rudin, Sven P.; Trinkle, Dallas R.; Jones, M. D.

    2000-07-01

    We have developed a new method[1] of fitting tight-binding parameterizations based on functional forms developed at the Naval Research Laboratory.[2] We have applied these methods to actinide metals and report our success using them (see below). The fitting procedure uses first-principles local-density-approximation (LDA) linear augmented plane-wave (LAPW) band structure techniques[3] to first calculate an electronic-structure band structure and total energy for fcc, bcc, and simple cubic crystal structures for the actinide of interest. The tight-binding parameterization is then chosen to fit the detailed energy eigenvalues of the bands along symmetry directions, and the symmetry of the parameterization is constrained to agree with the correct symmetry of the LDA band structure at each eigenvalue and k-vector that is fit to. By fitting to a range of different volumes and the three different crystal structures, we find that the resulting parameterization is robust and appears to accurately calculate other crystal structures and properties of interest.

  5. Localized heating of electrons in ionization zones: Going beyond the Penning-Thornton paradigm in magnetron sputtering

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

    Anders, Andre

    2014-12-07

    The fundamental question of how energy is supplied to a magnetron discharge is commonly answered by the Penning-Thornton paradigm invoking secondary electrons. Huo et al. (Plasma Sources Sci. Technol. 22, 045005, (2013)) used a global discharge model to show that electron heating in the electric field of the magnetic presheath is dominant. In this contribution, this concept is applied locally taking into account the electric potential structure of ionization zones. Images of ionization zones can and should be interpreted as diagrams of the localization of electric potential and related electron energy, where certain collisions promote or dampen their formation.

  6. An experimental study of the local electronic structure of B-site gallium doped bismuth ferrite powders

    NASA Astrophysics Data System (ADS)

    Gholam, Turghunjan; Ablat, Abduleziz; Mamat, Mamatrishat; Wu, Rong; Aimidula, Aimierding; Bake, Muhammad Ali; Zheng, Lirong; Wang, Jiaou; Qian, Haijie; Wu, Rui; Ibrahim, Kurash

    2017-08-01

    The un-doped and gallium (Ga) doped multiferroic bismuth ferrite (BiFeO3) compounds were successfully synthesized by the hydrothermal technique. This is then followed by a series of detailed investigations into the influence of Ga doping on the structural, morphological, optical and magnetic properties of BiFe1 - xGaxO3 (0 ≤ x ≤ 0.15). X-ray diffraction (XRD) analyses reveal that B-site doping of Ga may lead to the transformation of its crystal structure from a rhombohedral with a space group of R3c to an orthorhombic with a space group of Pbnm phase. The scanning electron microscope (SEM) images show that doping with Ga causes a significant reduction in particle size, when compared to un-doped BiFeO3. X-ray absorption near-edge structure (XANES) spectra have also shown that as the substitution of Ga increases, the Fe K and Bi LIII-edge absorption spectra shift towards higher energy site. It also implies that doping of Ga affects the local structures of both Bi and Fe atoms. Distinct transmission band fluctuations, as shown by Fourier transform infrared (FT-IR) spectra, can provide significant evidence for a transformation in crystal structure, following the increase of Ga concentration. The magnetization hysteresis measurements show that the magnetization decreases when Ga content is x ≥ 0.05. Such a phenomenon mainly stems from the substitution of Fe for an excessive amount of Ga, resulting in reduction of both valence fluctuations and the magnetization in the BiFe1 - xGaxO3 system.

  7. Electronic structure and magnetic properties of dilute U impurities in metals

    NASA Astrophysics Data System (ADS)

    Mohanta, S. K.; Cottenier, S.; Mishra, S. N.

    2016-05-01

    The electronic structure and magnetic moment of dilute U impurity in metallic hosts have been calculated from first principles. The calculations have been performed within local density approximation of the density functional theory using Augmented plane wave+local orbital (APW+lo) technique, taking account of spin-orbit coupling and Coulomb correlation through LDA+U approach. We present here our results for the local density of states, magnetic moment and hyperfine field calculated for an isolated U impurity embedded in hosts with sp-, d- and f-type conduction electrons. The results of our systematic study provide a comprehensive insight on the pressure dependence of 5f local magnetism in metallic systems. The unpolarized local density of states (LDOS), analyzed within the frame work of Stoner model suggest the occurrence of local moment for U in sp-elements, noble metals and f-block hosts like La, Ce, Lu and Th. In contrast, U is predicted to be nonmagnetic in most transition metal hosts except in Sc, Ti, Y, Zr, and Hf consistent with the results obtained from spin polarized calculation. The spin and orbital magnetic moments of U computed within the frame of LDA+U formalism show a scaling behavior with lattice compression. We have also computed the spin and orbital hyperfine fields and a detail analysis has been carried out. The host dependent trends for the magnetic moment, hyperfine field and 5f occupation reflect pressure induced change of electronic structure with U valency changing from 3+ to 4+ under lattice compression. In addition, we have made a detailed analysis of the impurity induced host spin polarization suggesting qualitatively different roles of f-band electrons on moment stability. The results presented in this work would be helpful towards understanding magnetism and spin fluctuation in U based alloys.

  8. Transmission electron microscopy: direct observation of crystal structure in refractory ceramics.

    PubMed

    Shaw, T M; Thomas, G

    1978-11-10

    Using high-resolution multibeam interference techniques in the transmission electron microscope, images have been obtained that make possible a real-space structure analysis of a beryllium-silicon-nitrogen compound. The results illustrate the usefulness of lattice imaging in the analysis of local crystal structure in these technologically promising ceramic materials.

  9. Electronic structures of Plutonium compounds with the NaCl-type monochalcogenides structure

    NASA Astrophysics Data System (ADS)

    Maehira, Takahiro; Tatetsu, Yasutomi

    2012-12-01

    We calculate the energy band structure and the Fermi surface of PuS, PuSe and PuTe by using a self-consistent relativistic linear augmented-plane-wave method with the exchange and correlation potential in a local density approximation. It is found in common that the energy bands in the vicinity of the Fermi level are mainly due to the hybridization between Pu 5/ and monochalcogenide p electrons. The obtained main Fermi surfaces are composed of two hole sheets and one electron sheet, all of which are constructed from the band having the Pu 5/ state and the monochalcogenide p state.

  10. Research Update: Spatially resolved mapping of electronic structure on atomic level by multivariate statistical analysis

    NASA Astrophysics Data System (ADS)

    Belianinov, Alex; Ganesh, Panchapakesan; Lin, Wenzhi; Sales, Brian C.; Sefat, Athena S.; Jesse, Stephen; Pan, Minghu; Kalinin, Sergei V.

    2014-12-01

    Atomic level spatial variability of electronic structure in Fe-based superconductor FeTe0.55Se0.45 (Tc = 15 K) is explored using current-imaging tunneling-spectroscopy. Multivariate statistical analysis of the data differentiates regions of dissimilar electronic behavior that can be identified with the segregation of chalcogen atoms, as well as boundaries between terminations and near neighbor interactions. Subsequent clustering analysis allows identification of the spatial localization of these dissimilar regions. Similar statistical analysis of modeled calculated density of states of chemically inhomogeneous FeTe1-xSex structures further confirms that the two types of chalcogens, i.e., Te and Se, can be identified by their electronic signature and differentiated by their local chemical environment. This approach allows detailed chemical discrimination of the scanning tunneling microscopy data including separation of atomic identities, proximity, and local configuration effects and can be universally applicable to chemically and electronically inhomogeneous surfaces.

  11. Interplay of local structure, charge, and spin in bilayered manganese perovskites

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

    Rybicki, Damian; Sikora, Marcin; Przewoznik, Janusz

    Chemical doping is a reliable method of modification of the electronic properties of transition metal compounds. In manganese perovskites, it leads to charge transfer and peculiar ordering phenomena. However, depending on the interplay of the local crystal structure and electronic properties, synthesis of stable compounds in the entire doping range is often impossible. In this paper, we show results of high-energy resolution x-ray absorption and emission spectroscopies on amore » $${\\mathrm{La}}_{2{-}2x}{\\mathrm{Sr}}_{1+2x}{\\mathrm{Mn}}_{2}{\\mathrm{O}}_{7}$$ family of bilayered manganites in a broad doping range $$(0.5{\\le}x{\\le}1)$$. We established a relation between local Mn charge and Mn-O distances as a function of doping. Finally, based on a comparison of such relation with other manganites, we suggest why stable structures cannot be realized for certain doping levels of bilayered compounds.« less

  12. Interplay of local structure, charge, and spin in bilayered manganese perovskites

    DOE PAGES

    Rybicki, Damian; Sikora, Marcin; Przewoznik, Janusz; ...

    2018-03-27

    Chemical doping is a reliable method of modification of the electronic properties of transition metal compounds. In manganese perovskites, it leads to charge transfer and peculiar ordering phenomena. However, depending on the interplay of the local crystal structure and electronic properties, synthesis of stable compounds in the entire doping range is often impossible. In this paper, we show results of high-energy resolution x-ray absorption and emission spectroscopies on amore » $${\\mathrm{La}}_{2{-}2x}{\\mathrm{Sr}}_{1+2x}{\\mathrm{Mn}}_{2}{\\mathrm{O}}_{7}$$ family of bilayered manganites in a broad doping range $$(0.5{\\le}x{\\le}1)$$. We established a relation between local Mn charge and Mn-O distances as a function of doping. Finally, based on a comparison of such relation with other manganites, we suggest why stable structures cannot be realized for certain doping levels of bilayered compounds.« less

  13. Electronic structure of gadolinium complexes in ZnO in the GW approximation

    NASA Astrophysics Data System (ADS)

    Rosa, A. L.; Frauenheim, Th.

    2018-04-01

    The role of intrinsic defects has been investigated to determine binding energies and the electronic structure of Gd complexes in ZnO. We use density-functional theory and the GW method to show that the presence of vacancies and interstitials affect the electronic structure of Gd doped ZnO. However, the strong localization of the Gd-f and d states suggest that carrier mediated ferromagnetism in this material may be difficult to achieve.

  14. In situ KPFM imaging of local photovoltaic characteristics of structured organic photovoltaic devices.

    PubMed

    Watanabe, Satoshi; Fukuchi, Yasumasa; Fukasawa, Masako; Sassa, Takafumi; Kimoto, Atsushi; Tajima, Yusuke; Uchiyama, Masanobu; Yamashita, Takashi; Matsumoto, Mutsuyoshi; Aoyama, Tetsuya

    2014-02-12

    Here, we discuss the local photovoltaic characteristics of a structured bulk heterojunction, organic photovoltaic devices fabricated with a liquid carbazole, and a fullerene derivative based on analysis by scanning kelvin probe force microscopy (KPFM). Periodic photopolymerization induced by an interference pattern from two laser beams formed surface relief gratings (SRG) in the structured films. The surface potential distribution in the SRGs indicates the formation of donor and acceptor spatial distribution. Under illumination, the surface potential reversibly changed because of the generation of fullerene anions and hole transport from the films to substrates, which indicates that we successfully imaged the local photovoltaic characteristics of the structured photovoltaic devices. Using atomic force microscopy, we confirmed the formation of the SRG because of the material migration to the photopolymerized region of the films, which was induced by light exposure through photomasks. The structuring technique allows for the direct fabrication and the control of donor and acceptor spatial distribution in organic photonic and electronic devices with minimized material consumption. This in situ KPFM technique is indispensable to the fabrication of nanoscale electron donor and electron acceptor spatial distribution in the devices.

  15. Distinct local structure of superconducting Ca10M4As8(Fe2As2)5 (M =Pt ,Ir)

    NASA Astrophysics Data System (ADS)

    Paris, E.; Wakita, T.; Proux, O.; Yokoya, T.; Kudo, K.; Mitsuoka, D.; Kimura, T.; Fujimura, K.; Nishimoto, N.; Ioka, S.; Nohara, M.; Mizokawa, T.; Saini, N. L.

    2017-12-01

    We have studied the local structure of superconducting Ca10Pt4As8(Fe2As2)5 (Pt10418) and Ca10Ir4As8(Fe2As2)5 (Ir10418) iron arsenides, showing different transition temperatures (Tc=38 and 16 K, respectively), by polarized Fe K -edge extended x-ray absorption fine-structure measurements. Despite the similar average crystal structures, the local structures of the FeAs4 tetrahedra in the two compounds are found to be very different. The FeAs4 in Pt10418 is close to a regular tetrahedron, while it deviates largely in Ir10418. The Fe-Fe correlations in the two compounds are characterized by similar bond-length characteristics; however, the static disorder in Pt10418 is significantly lower than that in Ir10418. The results suggest that the optimized local structure and reduced disorder are the reasons for higher Tc and well-defined electronic states in Pt10418 unlike Ir10418 showing the coexistence of glassy and normal electrons at the Fermi surface, and hence provide direct evidence of the local-structure-driven optimization of the electronic structure and superconductivity in iron arsenides.

  16. Atomic electron tomography: 3D structures without crystals

    DOE PAGES

    Miao, Jianwei; Ercius, Peter; Billinge, S. J. L.

    2016-09-23

    Crystallography has been fundamental to the development of many fields of science over the last century. However, much of our modern science and technology relies on materials with defects and disorders, and their three-dimensional (3D) atomic structures are not accessible to crystallography. One method capable of addressing this major challenge is atomic electron tomography. By combining advanced electron microscopes and detectors with powerful data analysis and tomographic reconstruction algorithms, it is now possible to determine the 3D atomic structure of crystal defects such as grain boundaries, stacking faults, dislocations, and point defects, as well as to precisely localize the 3Dmore » coordinates of individual atoms in materials without assuming crystallinity. In this work, we review the recent advances and the interdisciplinary science enabled by this methodology. We also outline further research needed for atomic electron tomography to address long-standing unresolved problems in the physical sciences.« less

  17. Effect of rare-earth ion size on local electron structure in RBa 2Cu 3O 7- δ (R = Tm, Dy, Gd, Eu, Nd and Y) superconductors: A positron study

    NASA Astrophysics Data System (ADS)

    Chen, Zhenping; Zhang, Jincang; Su, Yuling; Xue, Yuncai; Cao, Shixun

    2006-02-01

    The effects of rare-earth ionic size on the local electron structure, lattice parameters and superconductivity have been investigated by positron annihilation technique (PAT) and related experiments for RBa 2Cu 3O 7- δ (R = Tm, Dy, Gd, Eu, Nd and Y) superconductors. The local electron density ne is evaluated as a function of the rare-earth radius. The results show that both the bulk-lifetime τB and the defect lifetime τ2 increase with increasing rare-earth ionic radius, while the local electron density ne decrease with increasing rare-earth ionic radius. These results prove that the changes of ne, the degree of orthorhombic distortion and the coupling between the Cu-O chains and the CuO 2 planes all have an effect on the superconductivity of RBa 2Cu 3O 7- δ systems.

  18. First-principles study of Al2Sm intermetallic compound on structural, mechanical properties and electronic structure

    NASA Astrophysics Data System (ADS)

    Lin, Jingwu; Wang, Lei; Hu, Zhi; Li, Xiao; Yan, Hong

    2017-02-01

    The structural, thermodynamic, mechanical and electronic properties of cubic Al2Sm intermetallic compound are investigated by the first-principles method on the basis of density functional theory. In light of the strong on-site Coulomb repulsion between the highly localized 4f electrons of Sm atoms, the local spin density approximation approach paired with additional Hubbard terms is employed to achieve appropriate results. Moreover, to examine the reliability of this study, the experimental value of lattice parameter is procured from the analysis of the TEM image and diffraction pattern of Al2Sm phase in the AZ31 alloy to verify the authenticity of the results originated from the computational method. The value of cohesive energy reveals Al2Sm to be a stable in absolute zero Kelvin. According to the stability criteria, the subject of this work is mechanically stable. Afterward, elastic moduli are deduced by performing Voigt-Reuss-Hill approximation. Furthermore, elastic anisotropy and anisotropy of sound velocity are discussed. Finally, the calculation of electronic density of states is implemented to explore the underlying mechanism of structural stability.

  19. Control of Wigner localization and electron cavity effects in near-field emission spectra of In(Ga)P/GaInP quantum-dot structures

    NASA Astrophysics Data System (ADS)

    Mintairov, A. M.; Kapaldo, J.; Merz, J. L.; Rouvimov, S.; Lebedev, D. V.; Kalyuzhnyy, N. A.; Mintairov, S. A.; Belyaev, K. G.; Rakhlin, M. V.; Toropov, A. A.; Brunkov, P. N.; Vlasov, A. S.; Zadiranov, Yu. M.; Blundell, S. A.; Mozharov, A. M.; Mukhin, I.; Yakimov, M.; Oktyabrsky, S.; Shelaev, A. V.; Bykov, V. A.

    2018-05-01

    Structural and emission properties of few-electron In(Ga)P/GaInP quantum dots (QDs) representing natural Wigner molecules (WM) and whispering gallery mode (WGM) electron (e ) cavities have been investigated. QD structures were grown using self-organized metal-organic vapor phase epitaxy and deposition from ˜3 to 7 monolayers of InP at 700 °C. Using atomic force microscopy, transmission electron microscopy, near-field scanning optical microscopy (NSOM), and μ -photoluminescence (μ -PL) spectra we obtained In(Ga)P/GaInP QDs having lateral size 80-180 nm, height 5-30 nm, Ga content 0.0-0.4, density 2 -10 μm-2 , and electron population up to 20 and demonstrated control of their density and size distribution. Using high-spatial-resolution low-temperature PL spectra, NSOM imaging, and calculations of charge density distributions we observed Wigner localization and e -cavity effects for a series of dots having quantum confinement ℏ ω0=0.5 -6 meV . We used these data together with time-resolved PL measurements to clarify the effect of Coulomb interaction and WM formation on emission spectra of few-electron QDs. We present direct observation of 2 e , 6 e , and 9 e WMs; 2 e and 4 e WGMs; and Fabry-Perot e modes and establish conditions of e -WGM-cavity formation in these QDs.

  20. Calculation of smooth potential energy surfaces using local electron correlation methods

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

    Mata, Ricardo A.; Werner, Hans-Joachim

    2006-11-14

    The geometry dependence of excitation domains in local correlation methods can lead to noncontinuous potential energy surfaces. We propose a simple domain merging procedure which eliminates this problem in many situations. The method is applied to heterolytic bond dissociations of ketene and propadienone, to SN2 reactions of Cl{sup -} with alkylchlorides, and in a quantum mechanical/molecular mechanical study of the chorismate mutase enzyme. It is demonstrated that smooth potentials are obtained in all cases. Furthermore, basis set superposition error effects are reduced in local calculations, and it is found that this leads to better basis set convergence when computing barriermore » heights or weak interactions. When the electronic structure strongly changes between reactants or products and the transition state, the domain merging procedure leads to a balanced description of all structures and accurate barrier heights.« less

  1. Research Update: Spatially resolved mapping of electronic structure on atomic level by multivariate statistical analysis

    DOE PAGES

    Belianinov, Alex; Panchapakesan, G.; Lin, Wenzhi; ...

    2014-12-02

    Atomic level spatial variability of electronic structure in Fe-based superconductor FeTe0.55Se0.45 (Tc = 15 K) is explored using current-imaging tunneling-spectroscopy. Multivariate statistical analysis of the data differentiates regions of dissimilar electronic behavior that can be identified with the segregation of chalcogen atoms, as well as boundaries between terminations and near neighbor interactions. Subsequent clustering analysis allows identification of the spatial localization of these dissimilar regions. Similar statistical analysis of modeled calculated density of states of chemically inhomogeneous FeTe1 x Sex structures further confirms that the two types of chalcogens, i.e., Te and Se, can be identified by their electronic signaturemore » and differentiated by their local chemical environment. This approach allows detailed chemical discrimination of the scanning tunneling microscopy data including separation of atomic identities, proximity, and local configuration effects and can be universally applicable to chemically and electronically inhomogeneous surfaces.« less

  2. Research Update: Spatially resolved mapping of electronic structure on atomic level by multivariate statistical analysis

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

    Belianinov, Alex, E-mail: belianinova@ornl.gov; Ganesh, Panchapakesan; Lin, Wenzhi

    2014-12-01

    Atomic level spatial variability of electronic structure in Fe-based superconductor FeTe{sub 0.55}Se{sub 0.45} (T{sub c} = 15 K) is explored using current-imaging tunneling-spectroscopy. Multivariate statistical analysis of the data differentiates regions of dissimilar electronic behavior that can be identified with the segregation of chalcogen atoms, as well as boundaries between terminations and near neighbor interactions. Subsequent clustering analysis allows identification of the spatial localization of these dissimilar regions. Similar statistical analysis of modeled calculated density of states of chemically inhomogeneous FeTe{sub 1−x}Se{sub x} structures further confirms that the two types of chalcogens, i.e., Te and Se, can be identified bymore » their electronic signature and differentiated by their local chemical environment. This approach allows detailed chemical discrimination of the scanning tunneling microscopy data including separation of atomic identities, proximity, and local configuration effects and can be universally applicable to chemically and electronically inhomogeneous surfaces.« less

  3. Structured electronic physiotherapy records.

    PubMed

    Buyl, Ronald; Nyssen, Marc

    2009-07-01

    With the introduction of the electronic health record, physiotherapists too are encouraged to store their patient records in a structured digital format. The typical nature of a physiotherapy treatment requires a specific record structure to be implemented, with special attention to user-friendliness and communication with other healthcare providers. The objective of this study was to establish a framework for the electronic physiotherapy record and to define a model for the interoperability with the other healthcare providers involved in the patients' care. Although we started from the Belgian context, we used a generic approach so that the results can easily be extrapolated to other countries. The framework we establish here defines not only the different building blocks of the electronic physiotherapy record, but also describes the structure and the content of the exchanged data elements. Through a combined effort by all involved parties, we elaborated an eight-level structure for the electronic physiotherapy record. Furthermore we designed a server-based model for the exchange of data between electronic record systems held by physicians and those held by physiotherapists. Two newly defined XML messages enable data interchange: the physiotherapy prescription and the physiotherapy report. We succeeded in defining a solid, structural model for electronic physiotherapist record systems. Recent wide scale implementation of operational elements such as the electronic registry has proven to make the administrative work easier for the physiotherapist. Moreover, within the proposed framework all the necessary building blocks are present for further data exchange and communication with other healthcare parties in the future. Although we completed the design of the structure and already implemented some new aspects of the electronic physiotherapy record, the real challenge lies in persuading the end-users to start using these electronic record systems. Via a quality label

  4. Structural and electron diffraction scaling of twisted graphene bilayers

    NASA Astrophysics Data System (ADS)

    Zhang, Kuan; Tadmor, Ellad B.

    2018-03-01

    Multiscale simulations are used to study the structural relaxation in twisted graphene bilayers and the associated electron diffraction patterns. The initial twist forms an incommensurate moiré pattern that relaxes to a commensurate microstructure comprised of a repeating pattern of alternating low-energy AB and BA domains surrounding a high-energy AA domain. The simulations show that the relaxation mechanism involves a localized rotation and shrinking of the AA domains that scales in two regimes with the imposed twist. For small twisting angles, the localized rotation tends to a constant; for large twist, the rotation scales linearly with it. This behavior is tied to the inverse scaling of the moiré pattern size with twist angle and is explained theoretically using a linear elasticity model. The results are validated experimentally through a simulated electron diffraction analysis of the relaxed structures. A complex electron diffraction pattern involving the appearance of weak satellite peaks is predicted for the small twist regime. This new diffraction pattern is explained using an analytical model in which the relaxation kinematics are described as an exponentially-decaying (Gaussian) rotation field centered on the AA domains. Both the angle-dependent scaling and diffraction patterns are in quantitative agreement with experimental observations. A Matlab program for extracting the Gaussian model parameters accompanies this paper.

  5. Interplay of hot electrons from localized and propagating plasmons.

    PubMed

    Hoang, Chung V; Hayashi, Koki; Ito, Yasuo; Gorai, Naoki; Allison, Giles; Shi, Xu; Sun, Quan; Cheng, Zhenzhou; Ueno, Kosei; Goda, Keisuke; Misawa, Hiroaki

    2017-10-03

    Plasmon-induced hot-electron generation has recently received considerable interest and has been studied to develop novel applications in optoelectronics, photovoltaics and green chemistry. Such hot electrons are typically generated from either localized plasmons in metal nanoparticles or propagating plasmons in patterned metal nanostructures. Here we simultaneously generate these heterogeneous plasmon-induced hot electrons and exploit their cooperative interplay in a single metal-semiconductor device to demonstrate, as an example, wavelength-controlled polarity-switchable photoconductivity. Specifically, the dual-plasmon device produces a net photocurrent whose polarity is determined by the balance in population and directionality between the hot electrons from localized and propagating plasmons. The current responsivity and polarity-switching wavelength of the device can be varied over the entire visible spectrum by tailoring the hot-electron interplay in various ways. This phenomenon may provide flexibility to manipulate the electrical output from light-matter interaction and offer opportunities for biosensors, long-distance communications, and photoconversion applications.Plasmon-induced hot electrons have potential applications spanning photodetection and photocatalysis. Here, Hoang et al. study the interplay between hot electrons generated by localized and propagating plasmons, and demonstrate wavelength-controlled polarity-switchable photoconductivity.

  6. Electronic-structure calculations of praseodymium metal by means of modified density-functional theory

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

    Svane, A.; Trygg, J.; Johansson, B.

    1997-09-01

    Electronic-structure calculations of elemental praseodymium are presented. Several approximations are used to describe the Pr f electrons. It is found that the low-pressure, trivalent phase is well described using either the self-interaction corrected (SIC) local-spin-density (LSD) approximation or the generalized-gradient approximation (GGA) with spin and orbital polarization (OP). In the SIC-LSD approach the Pr f electrons are treated explicitly as localized with a localization energy given by the self-interaction of the f orbital. In the GGA+OP scheme the f-electron localization is described by the onset of spin and orbital polarization, the energetics of which is described by spin-moment formation energymore » and a term proportional to the total orbital moment, L{sub z}{sup 2}. The high-pressure phase is well described with the f electrons treated as band electrons, in either the LSD or the GGA approximations, of which the latter describes more accurately the experimental equation of state. The calculated pressure of the transition from localized to delocalized behavior is 280 kbar in the SIC-LSD approximation and 156 kbar in the GGA+OP approach, both comparing favorably with the experimentally observed transition pressure of 210 kbar. {copyright} {ital 1997} {ital The American Physical Society}« less

  7. Local Fine Structural Insight into Mechanism of Electrochemical Passivation of Titanium.

    PubMed

    Wang, Lu; Yu, Hongying; Wang, Ke; Xu, Haisong; Wang, Shaoyang; Sun, Dongbai

    2016-07-20

    Electrochemically formed passive film on titanium in 1.0 M H2SO4 solution and its thickness, composition, chemical state, and local fine structure are examined by Auger electron spectroscopy (AES), X-ray photoelectron spectroscopy (XPS), and X-ray absorption fine structure. AES analysis reveals that the thickness and composition of oxide film are proportional to the reciprocal of current density in potentiodynamic polarization. XPS depth profiles of the chemical states of titanium exhibit the coexistence of various valences cations in the surface. Quantitative X-ray absorption near edge structure analysis of the local electronic structure of the topmost surface (∼5.0 nm) shows that the ratio of [TiO2]/[Ti2O3] is consistent with that of passivation/dissolution of electrochemical activity. Theoretical calculation and analysis of extended X-ray absorption fine structure spectra at Ti K-edge indicate that both the structures of passivation and dissolution are distorted caused by the appearance of two different sites of Ti-O and Ti-Ti. And the bound water in the topmost surface plays a vital role in structural disorder confirmed by XPS. Overall, the increase of average Ti-O coordination causes the electrochemical passivation, and the dissolution is due to the decrease of average Ti-Ti coordination. The structural variations of passivation in coordination number and interatomic distance are in good agreement with the prediction of point defect model.

  8. Study of electronic structure of liquid Pb

    NASA Astrophysics Data System (ADS)

    Vora, A. M.; Gajjar, P. N.

    2018-04-01

    The Fiolhais et al.'s universal model potential in conjunction with the hard sphere technique of Percus and Yevick has been used for the study of electronic structure, Fermi energy and density of states of liquid Pb. The screening influence of the different forms of the local field correction functions proposed by Hartree (H) and Taylor (T) on the afore said properties is studied, which replicates the changing effects of screening and found suitable for the present study.

  9. Electronic Structure in Thin Film Organic Semiconductors

    DTIC Science & Technology

    2009-06-27

    Peltekis, C. McGuinness, and A. Matsuura, J. Chem. Phys. 129, 224705, (2008) c) "The Local Electronic Structure of Tin Phthalocyanine studied by...interfaces in a Cu(100)-benzenethiolate- pentacene heterostructure", Phys. Rev. Lett. 100, 027601 (2008). 21. O.V. Molodtsova, M. Grobosch, M. Knupfer...1999). 37. N.J. Watkins, S. Zorba, and Y. Gao, "Interface formation of pentacene on Al2O3", J. Appl. Phys. 96, 425 (2004). 38. K.V. Chauhan, I

  10. Localization of electrons and excitations

    NASA Astrophysics Data System (ADS)

    Larsson, Sven

    2006-07-01

    Electrons, electron holes, or excitations in finite or infinite 'multimer systems' may be localized or delocalized. In the theory of Hush, localization depends on the ratio Δ/ λ ( Δ/2 = coupling; λ = reorganization energy). The latter theory has been extended to the infinite system [S. Larsson, A. Klimkāns, Mol. Cryst. Liq. Cryst. 355 (2000) 217]. The metal/insulator transition often takes place abruptly as a function of Δ/ λ. It is argued that localization in a system with un-filled bands cannot be determined on the basis of Mott-Hubbard U alone, but depends on the number of accessible valence states, reorganization energy λ and coupling Δ (=2t). In fact U = 0 does not necessarily imply delocalization. The analysis here shows that there are many different situations for an insulator to metal transition. Charge transfer in doped NiO is characterized by Ni 2+ - Ni 3+ exchange while charge transfer in pure NiO is characterized by a disproportionation 2Ni 2+ → Ni + + Ni 3+. In spite of the great differences between these two cases, U has been applied without discrimination to both. The relevant localization parameters appear to be Δ and λ in the first case, with only two oxidation states, and U, Δ and λ in the second case with three oxidation states. The analysis is extended to insulator-metal transitions, giant magnetic resistance (GMR) and high Tc superconductivity (SC). λ and Δ can be determined quite accurately in quantum mechanical calculations involving only one and two monomers, respectively.

  11. Wedge-shaped potential and Airy-function electron localization in oxide superlattices.

    PubMed

    Popovic, Z S; Satpathy, S

    2005-05-06

    Oxide superlattices and microstructures hold the promise for creating a new class of devices with unprecedented functionalities. Density-functional studies of the recently fabricated, lattice-matched perovskite titanates (SrTiO3)n/(LaTiO3)m reveal a classic wedge-shaped potential well for the monolayer (m = 1) structure, originating from the Coulomb potential of a two-dimensional charged La sheet. The potential in turn confines the electrons in the Airy-function-localized states. Magnetism is suppressed for the monolayer structure, while in structures with a thicker LaTiO3 part, bulk antiferromagnetism is recovered, with a narrow transition region separating the magnetic LaTiO3 and the nonmagnetic SrTiO3.

  12. Electronic structure and optical properties of GdNi2Mnx compounds

    NASA Astrophysics Data System (ADS)

    Knyazev, Yu. V.; Lukoyanov, A. V.; Kuz'min, Yu. I.; Gaviko, V. S.

    2018-02-01

    The electronic structure and optical properties of GdNi2Mnx compounds (x = 0, 0.4, 0.6) were investigated. Spin-polarized electronic structure calculations were performed in the approximation of local electron spin density corrected for strong electron correlations using the LSDA+U method. The changes in the magnetic moments and exchange interactions in GdNi2Mnx (x = 0, 0.4, 0.6) governing the increase in the Curie temperature with manganese concentration were determined. The optical constants of the compounds were measured by the ellipsometric method in the wide spectral range of 0.22-15 μm. The peculiarities of the evolution of the frequency dependences of optical conductivity with a change in the manganese content were revealed. Based on the calculated densities of electron states, the behavior of these dispersion curves in the region of interband absorption of light was discussed. The concentration dependences of several electronic characteristics were determined.

  13. Structural, electronic structure and antibacterial properties of graphene-oxide nano-sheets

    NASA Astrophysics Data System (ADS)

    Sharma, Aditya; Varshney, Mayora; Nanda, Sitansu Sekhar; Shin, Hyun Joon; Kim, Namdong; Yi, Dong Kee; Chae, Keun-Hwa; Ok Won, Sung

    2018-04-01

    Correlation between the structural/electronic structure properties and bio-activity of graphene-based materials need to be thoroughly evaluated before their commercial implementation in the health and environment precincts. To better investigate the local hybridization of sp2/sp3 orbitals of the functional groups of graphene-oxide (GO) and their execution in the antimicrobial mechanism, we exemplify the antibacterial activity of GO sheets towards the Escherichia coli bacteria (E. coli) by applying the field-emission scanning electron microscopy (FESEM), near edge X-ray absorption fine structure (NEXAFS) and scanning transmission X-ray microscope (STXM) techniques. C K-edge and O K-edge NEXAFS spectra have revealed lesser sp2 carbon atoms in the aromatic ring and attachment of functional oxygen groups at GO sheets. Entrapment of E. coli bacteria by GO sheets is evidenced by FESEM investigations and has also been corroborated by nano-scale imaging of bacteria using the STXM. Spectroscopy evidence of functional oxygen moieties with GO sheets and physiochemical entrapment of E. coli bacteria have assisted us to elaborate the mechanism of cellular oxidative stress-induced disruption of bacterial membrane.

  14. Local and average structure of Mn- and La-substituted BiFeO3

    NASA Astrophysics Data System (ADS)

    Jiang, Bo; Selbach, Sverre M.

    2017-06-01

    The local and average structure of solid solutions of the multiferroic perovskite BiFeO3 is investigated by synchrotron X-ray diffraction (XRD) and electron density functional theory (DFT) calculations. The average experimental structure is determined by Rietveld refinement and the local structure by total scattering data analyzed in real space with the pair distribution function (PDF) method. With equal concentrations of La on the Bi site or Mn on the Fe site, La causes larger structural distortions than Mn. Structural models based on DFT relaxed geometry give an improved fit to experimental PDFs compared to models constrained by the space group symmetry. Berry phase calculations predict a higher ferroelectric polarization than the experimental literature values, reflecting that structural disorder is not captured in either average structure space group models or DFT calculations with artificial long range order imposed by periodic boundary conditions. Only by including point defects in a supercell, here Bi vacancies, can DFT calculations reproduce the literature results on the structure and ferroelectric polarization of Mn-substituted BiFeO3. The combination of local and average structure sensitive experimental methods with DFT calculations is useful for illuminating the structure-property-composition relationships in complex functional oxides with local structural distortions.

  15. Local and average structure of Mn- and La-substituted BiFeO 3

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

    Jiang, Bo; Selbach, Sverre M.

    2017-06-01

    The local and average structure of solid solutions of the multiferroic perovskite BiFeO 3 is investigated by synchrotron X-ray diffraction (XRD) and electron density functional theory (DFT) calculations. The average experimental structure is determined by Rietveld refinement and the local structure by total scattering data analyzed in real space with the pair distribution function (PDF) method. With equal concentrations of La on the Bi site or Mn on the Fe site, La causes larger structural distortions than Mn. Structural models based on DFT relaxed geometry give an improved fit to experimental PDFs compared to models constrained by the space groupmore » symmetry. Berry phase calculations predict a higher ferroelectric polarization than the experimental literature values, reflecting that structural disorder is not captured in either average structure space group models or DFT calculations with artificial long range order imposed by periodic boundary conditions. Only by including point defects in a supercell, here Bi vacancies, can DFT calculations reproduce the literature results on the structure and ferroelectric polarization of Mn-substituted BiFeO 3. The combination of local and average structure sensitive experimental methods with DFT calculations is useful for illuminating the structure-property-composition relationships in complex functional oxides with local structural distortions.« less

  16. Structural and electronic properties of GaAs and GaP semiconductors

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

    Rani, Anita; Kumar, Ranjan

    2015-05-15

    The Structural and Electronic properties of Zinc Blende phase of GaAs and GaP compounds are studied using self consistent SIESTA-code, pseudopotentials and Density Functional Theory (DFT) in Local Density Approximation (LDA). The Lattice Constant, Equillibrium Volume, Cohesive Energy per pair, Compressibility and Band Gap are calculated. The band gaps calcultated with DFT using LDA is smaller than the experimental values. The P-V data fitted to third order Birch Murnaghan equation of state provide the Bulk Modulus and its pressure derivatives. Our Structural and Electronic properties estimations are in agreement with available experimental and theoretical data.

  17. Effect of Al-doped YCrO3 on structural, electronic and magnetic properties

    NASA Astrophysics Data System (ADS)

    Durán, A.; Verdín, E.; Conde, A.; Escamilla, R.

    2018-05-01

    Structural, dielectric and magnetic properties were investigated in the YCr1-xAlxO3 with 0 < x < 0.5 compositions. XRD and XPS studies show that the partial substitution of the Al3+ ion decreases the cell volume of the orthorhombic structure without changes in the oxidation state of the Cr3+ ions. We discuss two mechanisms that could have a significant influence on the magnetic properties. The first is related to local deformation occurring for x < 0.1 of Al content and the second is related to change of the electronic structure. The local deformation is controlled by the inclination of the octahedrons and the octahedral distortion having a strong effect on the TN and the coercive field at low Al concentrations. On the other hand, the decreasing of the magnetization values (Mr and Hc) is ascribed to changes in the electronic structure, which is confirmed by a decreasing of the contribution of Cr 3d states at Fermi level due to increasing Al3+ content. Thus, we analyzed and discussed that both mechanisms influence the electronic properties of the YCr1-xAlxO3 solid solution.

  18. Localized Electron Heating by Strong Guide-Field Magnetic Reconnection

    NASA Astrophysics Data System (ADS)

    Guo, Xuehan; Sugawara, Takumichi; Inomoto, Michiaki; Yamasaki, Kotaro; Ono, Yasushi; UTST Team

    2015-11-01

    Localized electron heating of magnetic reconnection was studied under strong guide-field (typically Bt 15Bp) using two merging spherical tokamak plasmas in Univ. Tokyo Spherical Tokamak (UTST) experiment. Our new slide-type two-dimensional Thomson scattering system documented for the first time the electron heating localized around the X-point. The region of high electron temperature, which is perpendicular to the magnetic field, was found to have a round shape with radius of 2 [cm]. Also, it was localized around the X-point and does not agree with that of energy dissipation term Et .jt . When we include a guide-field effect term Bt / (Bp + αBt) for Et .jt where α =√{ (vin2 +vout2) /v∥2 } , the energy dissipation area becomes localized around the X-point, suggesting that the electrons are accelerated by the reconnection electric field parallel to the magnetic field and thermalized around the X-point. This work was supported by JSPS A3 Foresight Program ``Innovative Tokamak Plasma Startup and Current Drive in Spherical Torus,'' a Grant-in-Aid from the Japan Society for the Promotion of Science (JSPS) Fellows 15J03758.

  19. Local Electronic Structure Changes in Polycrystalline CdTe with CdCl 2 Treatment and Air Exposure

    DOE PAGES

    Berg, Morgann; Kephart, Jason M.; Munshi, Amit; ...

    2018-03-12

    Postdeposition CdCl 2 treatment of polycrystalline CdTe is known to increase the photovoltaic device efficiency. However, the precise chemical, structural, and electronic changes that underpin this improvement are still debated. In this work, spectroscopic photoemission electron microscopy was used to spatially map the vacuum level and ionization energy of CdTe films, enabling the identification of electronic structure variations between grains and grain boundaries (GBs). In vacuo preparation and inert transfer of oxide-free CdTe surfaces isolated the separate effects of CdCl 2 treatment and ambient oxygen exposure. Qualitatively, grain boundaries displayed lower work function and downward band bending relative to grainmore » interiors, but only after air exposure of CdCl 2-treated CdTe. Analysis of numerous space charge regions at grain boundaries showed an average depletion width of 290 nm and an average band bending magnitude of 70 meV, corresponding to a GB trap density of 10 11 cm –2 and a net carrier density of 10 15 cm –3. Finally, these results suggest that both CdCl 2 treatment and oxygen exposure may be independently tuned to enhance the CdTe photovoltaic performance by engineering the interface and bulk electronic structure.« less

  20. Local Electronic Structure Changes in Polycrystalline CdTe with CdCl 2 Treatment and Air Exposure

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

    Berg, Morgann; Kephart, Jason M.; Munshi, Amit

    Postdeposition CdCl 2 treatment of polycrystalline CdTe is known to increase the photovoltaic device efficiency. However, the precise chemical, structural, and electronic changes that underpin this improvement are still debated. In this work, spectroscopic photoemission electron microscopy was used to spatially map the vacuum level and ionization energy of CdTe films, enabling the identification of electronic structure variations between grains and grain boundaries (GBs). In vacuo preparation and inert transfer of oxide-free CdTe surfaces isolated the separate effects of CdCl 2 treatment and ambient oxygen exposure. Qualitatively, grain boundaries displayed lower work function and downward band bending relative to grainmore » interiors, but only after air exposure of CdCl 2-treated CdTe. Analysis of numerous space charge regions at grain boundaries showed an average depletion width of 290 nm and an average band bending magnitude of 70 meV, corresponding to a GB trap density of 10 11 cm –2 and a net carrier density of 10 15 cm –3. Finally, these results suggest that both CdCl 2 treatment and oxygen exposure may be independently tuned to enhance the CdTe photovoltaic performance by engineering the interface and bulk electronic structure.« less

  1. Ion Streaming Instabilities in Pair Ion Plasma and Localized Structure with Non-Thermal Electrons

    NASA Astrophysics Data System (ADS)

    Nasir Khattak, M.; Mushtaq, A.; Qamar, A.

    2015-12-01

    Pair ion plasma with a fraction of non-thermal electrons is considered. We investigate the effects of the streaming motion of ions on linear and nonlinear properties of unmagnetized, collisionless plasma by using the fluid model. A dispersion relation is derived, and the growth rate of streaming instabilities with effect of streaming motion of ions and non-thermal electrons is calculated. A qausi-potential approach is adopted to study the characteristics of ion acoustic solitons. An energy integral equation involving Sagdeev potential is derived during this process. The presence of the streaming term in the energy integral equation affects the structure of the solitary waves significantly along with non-thermal electrons. Possible application of the work to the space and laboratory plasmas are highlighted.

  2. Excess Electron Localization in Solvated DNA Bases

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

    Smyth, Maeve; Kohanoff, Jorge

    2011-06-10

    We present a first-principles molecular dynamics study of an excess electron in condensed phase models of solvated DNA bases. Calculations on increasingly large microsolvated clusters taken from liquid phase simulations show that adiabatic electron affinities increase systematically upon solvation, as for optimized gas-phase geometries. Dynamical simulations after vertical attachment indicate that the excess electron, which is initially found delocalized, localizes around the nucleobases within a 15 fs time scale. This transition requires small rearrangements in the geometry of the bases.

  3. Excess electron localization in solvated DNA bases.

    PubMed

    Smyth, Maeve; Kohanoff, Jorge

    2011-06-10

    We present a first-principles molecular dynamics study of an excess electron in condensed phase models of solvated DNA bases. Calculations on increasingly large microsolvated clusters taken from liquid phase simulations show that adiabatic electron affinities increase systematically upon solvation, as for optimized gas-phase geometries. Dynamical simulations after vertical attachment indicate that the excess electron, which is initially found delocalized, localizes around the nucleobases within a 15 fs time scale. This transition requires small rearrangements in the geometry of the bases.

  4. Thermal transfer structures coupling electronics card(s) to coolant-cooled structure(s)

    DOEpatents

    David, Milnes P; Graybill, David P; Iyengar, Madhusudan K; Kamath, Vinod; Kochuparambil, Bejoy J; Parida, Pritish R; Schmidt, Roger R

    2014-12-16

    Cooling apparatuses and coolant-cooled electronic systems are provided which include thermal transfer structures configured to engage with a spring force one or more electronics cards with docking of the electronics card(s) within a respective socket(s) of the electronic system. A thermal transfer structure of the cooling apparatus includes a thermal spreader having a first thermal conduction surface, and a thermally conductive spring assembly coupled to the conduction surface of the thermal spreader and positioned and configured to reside between and physically couple a first surface of an electronics card to the first surface of the thermal spreader with docking of the electronics card within a socket of the electronic system. The thermal transfer structure is, in one embodiment, metallurgically bonded to a coolant-cooled structure and facilitates transfer of heat from the electronics card to coolant flowing through the coolant-cooled structure.

  5. Electronic structure imperfections and chemical bonding at graphene interfaces

    NASA Astrophysics Data System (ADS)

    Schultz, Brian Joseph

    nanomaterial with lateral dimensions in the hundreds of microns if not larger, with a corresponding atomic vertical thickness poses significant difficulties. Graphene's unique structure is dominated by surface area or potentially hybridized interfaces; consequently, the true realization of this remarkable nanomaterial in device constructs relies on engineering graphene interfaces at the surface in order to controllably mold the electronic structure. Near-edge X-ray absorption fine-structure (NEXAFS) spectroscopy and the transmission mode analogue scanning transmission X-ray microscopy (STXM) are particularly useful tools to study the unoccupied states of graphene and graphene interfaces. In addition, polarized NEXAFS and STXM studies provide information on surface orientation, bond sterics, and the extent of substrate alignment before and after interfacial hybridization. The work presented in this dissertation is fundamentally informed by NEXAFS and STXM measurements on graphene/metal, graphene/dielectric, and graphene/organic interfaces. We start with a general review of the electronic structure of freestanding graphene and graphene interfaces in Chapter 1. In Chapter 2, we investigate freestanding single-layer graphene via STXM and NEXAFS demonstrating that electronic structure heterogeneities from synthesis and processing are ubiquitous in 2-dimensional graphene. We show the mapping of discrete charge transfer regions as a result of doped impurities that decorate the surfaces of graphene and that transfer processing imparts local electronic corrugations or ripples. In corroboration with density functional theory, definitive assignments to the spectral features, global steric orientations of the localized domains, and quantitative charge transfer schemes are evidenced. In the following chapters, we deliberately (Chapter 3) incorporate substitutional nitrogen into reduced graphene oxide to induce C--N charge redistribution and improve global conductivity, (Chapter 4

  6. Electron acceleration at localized wave structures in the solar corona (German Title: Elektronenbeschleunigung an lokalen Wellenstrukturen in der Sonnenkorona)

    NASA Astrophysics Data System (ADS)

    Miteva, Rositsa Stoycheva

    2007-07-01

    Our dynamic Sun manifests its activity by different phenomena: from the 11-year cyclic sunspot pattern to the unpredictable and violent explosions in the case of solar flares. During flares, a huge amount of the stored magnetic energy is suddenly released and a substantial part of this energy is carried by the energetic electrons, considered to be the source of the nonthermal radio and X-ray radiation. One of the most important and still open question in solar physics is how the electrons are accelerated up to high energies within (the observed in the radio emission) short time scales. Because the acceleration site is extremely small in spatial extent as well (compared to the solar radius), the electron acceleration is regarded as a local process. The search for localized wave structures in the solar corona that are able to accelerate electrons together with the theoretical and numerical description of the conditions and requirements for this process, is the aim of the dissertation. Two models of electron acceleration in the solar corona are proposed in the dissertation: I. Electron acceleration due to the solar jet interaction with the background coronal plasma (the jet--plasma interaction) A jet is formed when the newly reconnected and highly curved magnetic field lines are relaxed by shooting plasma away from the reconnection site. Such jets, as observed in soft X-rays with the Yohkoh satellite, are spatially and temporally associated with beams of nonthermal electrons (in terms of the so-called type III metric radio bursts) propagating through the corona. A model that attempts to give an explanation for such observational facts is developed here. Initially, the interaction of such jets with the background plasma leads to an (ion-acoustic) instability associated with growing of electrostatic fluctuations in time for certain range of the jet initial velocity. During this process, any test electron that happen to feel this electrostatic wave field is drawn to co

  7. Electron Beam Freeform Fabrication of Titanium Alloy Gradient Structures

    NASA Technical Reports Server (NTRS)

    Brice, Craig A.; Newman, John A.; Bird, Richard Keith; Shenoy, Ravi N.; Baughman, James M.; Gupta, Vipul K.

    2014-01-01

    Historically, the structural optimization of aerospace components has been done through geometric methods. A monolithic material is chosen based on the best compromise between the competing design limiting criteria. Then the structure is geometrically optimized to give the best overall performance using the single material chosen. Functionally graded materials offer the potential to further improve structural efficiency by allowing the material composition and/or microstructural features to spatially vary within a single structure. Thus, local properties could be tailored to the local design limiting criteria. Additive manufacturing techniques enable the fabrication of such graded materials and structures. This paper presents the results of a graded material study using two titanium alloys processed using electron beam freeform fabrication, an additive manufacturing process. The results show that the two alloys uniformly mix at various ratios and the resultant static tensile properties of the mixed alloys behave according to rule-of-mixtures. Additionally, the crack growth behavior across an abrupt change from one alloy to the other shows no discontinuity and the crack smoothly transitions from one crack growth regime into another.

  8. Computational Study on Atomic Structures, Electronic Properties, and Chemical Reactions at Surfaces and Interfaces and in Biomaterials

    NASA Astrophysics Data System (ADS)

    Takano, Yu; Kobayashi, Nobuhiko; Morikawa, Yoshitada

    2018-06-01

    Through computer simulations using atomistic models, it is becoming possible to calculate the atomic structures of localized defects or dopants in semiconductors, chemically active sites in heterogeneous catalysts, nanoscale structures, and active sites in biological systems precisely. Furthermore, it is also possible to clarify physical and chemical properties possessed by these nanoscale structures such as electronic states, electronic and atomic transport properties, optical properties, and chemical reactivity. It is sometimes quite difficult to clarify these nanoscale structure-function relations experimentally and, therefore, accurate computational studies are indispensable in materials science. In this paper, we review recent studies on the relation between local structures and functions for inorganic, organic, and biological systems by using atomistic computer simulations.

  9. Electronic Structure and Transport in Solids from First Principles

    NASA Astrophysics Data System (ADS)

    Mustafa, Jamal Ibrahim

    The focus of this dissertation is the determination of the electronic structure and trans- port properties of solids. We first review some of the theory and computational methodology used in the calculation of electronic structure and materials properties. Throughout the dissertation, we make extensive use of state-of-the-art software packages that implement density functional theory, density functional perturbation theory, and the GW approximation, in addition to specialized methods for interpolating matrix elements for extremely accurate results. The first application of the computational framework introduced is the determination of band offsets in semiconductor heterojunctions using a theory of quantum dipoles at the interface. This method is applied to the case of heterojunction formed between a new metastable phase of silicon, with a rhombohedral structure, and cubic silicon. Next, we introduce a novel method for the construction of localized Wannier functions, which we have named the optimized projection functions method (OPFM). We illustrate the method on a variety of systems and find that it can reliably construct localized Wannier functions with minimal user intervention. We further develop the OPFM to investigate a class of materials called topological insulators, which are insulating in the bulk but have conductive surface states. These properties are a result of a nontrivial topology in their band structure, which has interesting effects on the character of the Wannier functions. In the last sections of the main text, the noble metals are studied in great detail, including their electronic properties and carrier dynamics. In particular, we investigate, the Fermi surface properties of the noble metals, specifically electron-phonon scattering lifetimes, and subsequently the transport properties determined by carriers on the Fermi surface. To achieve this, a novel sampling technique is developed, with wide applicability to transport calculations

  10. Phase Diagram and Electronic Structure of Praseodymium and Plutonium

    DOE PAGES

    Lanatà, Nicola; Yao, Yongxin; Wang, Cai-Zhuang; ...

    2015-01-29

    We develop a new implementation of the Gutzwiller approximation in combination with the local density approximation, which enables us to study complex 4f and 5f systems beyond the reach of previous approaches. We calculate from first principles the zero-temperature phase diagram and electronic structure of Pr and Pu, finding good agreement with the experiments. Our study of Pr indicates that its pressure-induced volume-collapse transition would not occur without change of lattice structure—contrarily to Ce. Our study of Pu shows that the most important effect originating the differentiation between the equilibrium densities of its allotropes is the competition between the Peierlsmore » effect and the Madelung interaction and not the dependence of the electron correlations on the lattice structure.« less

  11. Local Structure Analysis and Interface Layer Effect of Phase-Change Recording Material Using Actual Media

    NASA Astrophysics Data System (ADS)

    Nakai, Tsukasa; Yoshiki, Masahiko; Satoh, Yasuhiro; Ashida, Sumio

    2008-07-01

    The influences of the interface layer on crystal structure, the local atomic arrangement, and the electronic and chemical structure of a GeBiTe (GBT) phase-change recording material have been investigated using X-ray diffraction (XRD), X-ray absorption fine structure (XAFS), and hard X-ray photoelectron spectroscopy (HX-PES) methods using actual rewritable high-speed HD DVD media without special sample processing. XRD results showed that the crystal structure of laser-crystallized GBT alloy in the actual HD DVD media is the same as that of GeSbTe (GST) alloy, which has a NaCl-type structure. No differences between samples with and without interface layers were found. The lattice constant of GBT is larger than that of GST. Bi increases the lattice constant of GST with respect to the Bi substitution ratio of Sb. According to HX-PES, the DOS of in the recording film amorphous state with an interface layer is closer to that of the crystalline state than the recording film without an interface layer. From XAFS results, clear differences between amorphous (Amo.) and crystalline states (Cry.) were observed. The interatomic distance of amorphous recording material is independent of the existence of an interface layer. On the other hand, the coordination number varied slightly due to the presence of the interface layer. Therefore, the electronic state of the recording layer changes because of the interface layer, although the local structure changes only slightly except for the coordination number. Combining these results, we conclude that the interface layer changes the electronic state of the recording layer and promotes crystallization, but only affects the local structure of the atomic arrangement slightly.

  12. Variability of Protein Structure Models from Electron Microscopy.

    PubMed

    Monroe, Lyman; Terashi, Genki; Kihara, Daisuke

    2017-04-04

    An increasing number of biomolecular structures are solved by electron microscopy (EM). However, the quality of structure models determined from EM maps vary substantially. To understand to what extent structure models are supported by information embedded in EM maps, we used two computational structure refinement methods to examine how much structures can be refined using a dataset of 49 maps with accompanying structure models. The extent of structure modification as well as the disagreement between refinement models produced by the two computational methods scaled inversely with the global and the local map resolutions. A general quantitative estimation of deviations of structures for particular map resolutions are provided. Our results indicate that the observed discrepancy between the deposited map and the refined models is due to the lack of structural information present in EM maps and thus these annotations must be used with caution for further applications. Copyright © 2017 Elsevier Ltd. All rights reserved.

  13. Electronically controllable spoof localized surface plasmons

    NASA Astrophysics Data System (ADS)

    Zhou, Yong Jin; Zhang, Chao; Yang, Liu; Xun Xiao, Qian

    2017-10-01

    Electronically controllable multipolar spoof localized surface plasmons (LSPs) are experimentally demonstrated in the microwave frequencies. It has been shown that half integer order LSPs modes exist on the corrugated ring loaded with a slit, which actually arise from the Fabry-Perot-like resonances. By mounting active components across the slit in the corrugated rings, electronic switchability and tunability of spoof LSPs modes have been accomplished. Both simulated and measured results demonstrate efficient dynamic control of the spoof LSPs. These elements may form the basis of highly integrated programmable plasmonic circuits in microwave and terahertz regimes.

  14. Localization-delocalization transition of electrons at the percolation threshold of semiconductor GaAs1-xNx alloys: The appearance of a mobility edge

    NASA Astrophysics Data System (ADS)

    Alberi, K.; Fluegel, B.; Beaton, D. A.; Ptak, A. J.; Mascarenhas, A.

    2012-07-01

    Electrons in semiconductor alloys have generally been described in terms of Bloch states that evolve from constructive interference of electron waves scattering from perfectly periodic potentials, despite the loss of structural periodicity that occurs on alloying. Using the semiconductor alloy GaAs1-xNx as a prototype, we demonstrate a localized to delocalized transition of the electronic states at a percolation threshold, the emergence of a mobility edge, and the onset of an abrupt perturbation to the host GaAs electronic structure, shedding light on the evolution of electronic structure in these abnormal alloys.

  15. Local electrical properties of n-AlInAs/i-GaInAs electron channel structures characterized by the probe-electron-beam-induced current technique.

    PubMed

    Watanabe, Kentaro; Nokuo, Takeshi; Chen, Jun; Sekiguchi, Takashi

    2014-04-01

    We developed a probe-electron-beam-induced current (probe-EBIC) technique to investigate the electrical properties of n-Al(0.48)In(0.52)As/i-Ga(0.30)In(0.70)As electron channel structures for a high-electron-mobility transistor, grown on a lattice-matched InP substrate and lattice-mismatched GaAs (001) and Si (001) substrates. EBIC imaging of planar surfaces at low magnifications revealed misfit dislocations originating from the AlInAs-graded buffer layer. The cross-sections of GaInAs channel structures on an InP substrate were studied by high-magnification EBIC imaging as well as cathodoluminescence (CL) spectroscopy. EBIC imaging showed that the structure is nearly defect-free and the carrier depletion zone extends from the channel toward the i-AlInAs buffer layer.

  16. The imprint of Gould's belt on the local cosmic ray electron spectrum

    NASA Astrophysics Data System (ADS)

    Pohl, M.; Perrot, C.; Grenier, I.

    2001-08-01

    In a recent paper Pohl and Esposito (1998) demonstrated that if the sources of cosmic-rays are discrete, as are Supernova Remnants (SNR), then the spectra of cosmic-ray electrons largely vary with location and time and the locally measured electron spectrum may not be representative of the electron spectra elsewhere in the Galaxy, which could be substantially harder than the local one. They have shown that the observed excess of γ-ray emission above 1 GeV can in fact be partially explained as a correspondingly hard inverse Compton component, provided the bulk of cosmic-ray electrons is produced in SNR. As part of a program to model the Galactic γ-ray foreground we have continued the earlier studies by investigating the impact of the star forming region Gould's Belt on the local electron spectrum. If the electron sources in Gould's Belt were continous, the local electron spectrum would be slightly hardened. If the electron sources are discrete, which is the more probable case, the variation in the local electron spectrum found by Pohl & Esposito persists. 1 The local cosmic-ray electron spectrum The recent detections of non-thermal X-ray synchrotron radiation from the supernova remnants SN1006 (Koyama et al., 1995), RX J1713.7-3946 (Koyama et al., 1997), IC443 (Keohane et al., 1997; Slane et al., 1999), Cas A (Allen et al., 1997), and RCW86 (Borkowski et al., 2001) and the subsequent detections of SN1006 (Tanimori et al., 1998), RX J1713.7-3946 (Muraishi et al., 2000), and Cas A (Aharonian et al., 2001) at TeV energies support the hypothesis that at least Galactic cosmic-ray electrons are accelerated predominantly in SNR. The Galactic distribution and spectrum of cosmic-ray electrons are intimately linked to the distribution and nature of their sources. Supernovae and hence their remnants are tran-

  17. Electronic and crystal structure of NiTi martensite

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

    Sanati, M.; Albers, R.C.; Pinski, F.J.

    1998-11-01

    All of the first-principles electronic-structure calculations for the martensitic structure of NiTi have used the experimental atomic parameters reported by Michal and Sinclair [Acta Crystallogr., Sect. B: Struct. Crystallogr. Cryst. Chem. {bold B37}, 1803 (1981)]. We have used first-principles, full-potential, linear muffin-tin orbital calculations to examine the total energy of all the experimental martensitic structures reported in the literature. We find that another crystal structure, that of Kudoh {ital et al.} [Acta Metall. Mater. {bold 33}, 2049 (1985)], has the lowest total energy at zero temperature. Ground-state and formation energies were calculated for all of the experimental structures. Total andmore » local densities of states were calculated and compared with each other for the structures of both Kudoh {ital et al.} and Michal and Sinclair thinsp {copyright} {ital 1998} {ital The American Physical Society}« less

  18. Monte Carlo simulations of disorder in ZnSn N 2 and the effects on the electronic structure

    DOE PAGES

    Lany, Stephan; Fioretti, Angela N.; Zawadzki, Paweł P.; ...

    2017-08-10

    In multinary compound semiconductors, cation disorder can decisively alter the electronic properties and impact potential applications. ZnSnN 2 is a ternary nitride of interest for photovoltaics, which forms in a wurtzite-derived crystal structure. In the ground state, every N anion is coordinated by two Zn and two Sn cations, thereby observing the octet rule locally. Using a motif-based model Hamiltonian, we performed Monte Carlo simulations that provide atomistic representations of ZnSnN 2 with varying degrees of cation disorder. Subsequent electronic structure calculations describe the evolution of band gaps, optical properties, and carrier localization effects as a function of the disorder.more » We find that octet-rule conserving disorder is practically impossible to avoid but perfectly benign, with hardly any effects on the electronic structure. In contrast, a fully random cation distribution would be very detrimental, but fortunately it is energetically highly unfavorable. A degree of disorder that can realistically be expected for nonequilibrium thin-film deposition leads to a moderate band-gap reduction and to moderate carrier localization effects. Comparing the simulated structures with experimental samples grown by sputtering, we find evidence that these samples indeed incorporate a certain degree of octet-rule violating disorder, which is reflected in the x-ray diffraction and in the optical absorption spectra. This study demonstrates that the electronic properties of ZnSnN 2 are dominated by changes of the local coordination environments rather than long-range ordering effects.« less

  19. Monte Carlo simulations of disorder in ZnSn N 2 and the effects on the electronic structure

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

    Lany, Stephan; Fioretti, Angela N.; Zawadzki, Paweł P.

    In multinary compound semiconductors, cation disorder can decisively alter the electronic properties and impact potential applications. ZnSnN 2 is a ternary nitride of interest for photovoltaics, which forms in a wurtzite-derived crystal structure. In the ground state, every N anion is coordinated by two Zn and two Sn cations, thereby observing the octet rule locally. Using a motif-based model Hamiltonian, we performed Monte Carlo simulations that provide atomistic representations of ZnSnN 2 with varying degrees of cation disorder. Subsequent electronic structure calculations describe the evolution of band gaps, optical properties, and carrier localization effects as a function of the disorder.more » We find that octet-rule conserving disorder is practically impossible to avoid but perfectly benign, with hardly any effects on the electronic structure. In contrast, a fully random cation distribution would be very detrimental, but fortunately it is energetically highly unfavorable. A degree of disorder that can realistically be expected for nonequilibrium thin-film deposition leads to a moderate band-gap reduction and to moderate carrier localization effects. Comparing the simulated structures with experimental samples grown by sputtering, we find evidence that these samples indeed incorporate a certain degree of octet-rule violating disorder, which is reflected in the x-ray diffraction and in the optical absorption spectra. This study demonstrates that the electronic properties of ZnSnN 2 are dominated by changes of the local coordination environments rather than long-range ordering effects.« less

  20. Local structure distortion induced by Ti dopants boosting the pseudocapacitance of RuO2-based supercapacitors

    NASA Astrophysics Data System (ADS)

    Chen, I.-Li; Wei, Yu-Chen; Lu, Kueih-Tzu; Chen, Tsan-Yao; Hu, Chi-Chang; Chen, Jin-Ming

    2015-09-01

    Binary oxides with atomic ratios of Ru/Ti = 90/10, 70/30, and 50/50 were fabricated using H2O2-oxidative precipitation with the assistance of a cetyltrimethylammonium bromide (CTAB) template, followed by a thermal treatment at 200 °C. The characteristics of electron structure and local structure extracted from X-ray absorption spectroscopy (XAS) and transmission electron microscopy (TEM) analyses indicate that incorporation of Ti into the RuO2 lattice produces not only the local structural distortion of the RuO6 octahedra in (Ru-Ti)O2 with an increase in the central Ru-Ru distance but also a local crystallization of RuO2. Among the three binary oxides studied, (Ru70-Ti30)O2 exhibits a capacitance improvement of about 1.4-fold relative to the CTAB-modified RuO2, mainly due to the enhanced crystallinity of the distorted RuO6 structure rather than the surface area effect. Upon increasing the extent of Ti doping, the deteriorated supercapacitive performance of (Ru50-Ti50)O2 results from the formation of localized nano-clusters of TiO2 crystallites. These results provide insight into the important role of Ti doping in RuO2 that boosts the pseudocapacitive performance for RuO2-based supercapacitors. The present result is crucial for the design of new binary oxides for supercapacitor applications with extraordinary performance.Binary oxides with atomic ratios of Ru/Ti = 90/10, 70/30, and 50/50 were fabricated using H2O2-oxidative precipitation with the assistance of a cetyltrimethylammonium bromide (CTAB) template, followed by a thermal treatment at 200 °C. The characteristics of electron structure and local structure extracted from X-ray absorption spectroscopy (XAS) and transmission electron microscopy (TEM) analyses indicate that incorporation of Ti into the RuO2 lattice produces not only the local structural distortion of the RuO6 octahedra in (Ru-Ti)O2 with an increase in the central Ru-Ru distance but also a local crystallization of RuO2. Among the three binary

  1. Electronic transport property in Weyl semimetal with local Weyl cone tilt

    NASA Astrophysics Data System (ADS)

    Jiang, Liwei; Feng, Lanting; Yao, Haibo; Zheng, Yisong

    2018-03-01

    In realistic materials of Weyl semimetal (WSM), the Weyl cone tilt (WCT) is allowed due to the absence of Lorentz invariance in condensed matter physics. In this context, we theoretically study the electronic transport property in WSM with the local WCT as the scattering mechanism. In so doing, we establish an electronic transport structure of WSM with the WCT occurring only in the central region sandwiched between two pieces of semi-infinite WSM without the WCT. By means of two complementary theoretical approaches, i.e. the continuum-model method and the lattice-model method, the electronic transmission probability, the conductivity and the Fano factor as functions of the incident electron energy are calculated respectively. We find that the WCT can give rise to nontrivial intervalley scattering, as a result, the Klein tunneling is notably suppressed. More importantly, the minimal conductivity of a WSM shifts in energy from the Weyl nodal point. The Fano factor of the shot noise deviates obviously from the sub-Poissonian value in a two dimensional WSM with the WCT.

  2. Two-dimensional Si nanosheets with local hexagonal structure on a MoS(2) surface.

    PubMed

    Chiappe, Daniele; Scalise, Emilio; Cinquanta, Eugenio; Grazianetti, Carlo; van den Broek, Bas; Fanciulli, Marco; Houssa, Michel; Molle, Alessandro

    2014-04-02

    The structural and electronic properties of a Si nanosheet (NS) grown onto a MoS2 substrate by means of molecular beam epitaxy are assessed. Epitaxially grown Si is shown to adapt to the trigonal prismatic surface lattice of MoS2 by forming two-dimensional nanodomains. The Si layer structure is distinguished from the underlying MoS2 surface structure. The local electronic properties of the Si nanosheet are dictated by the atomistic arrangement of the layer and unlike the MoS2 hosting substrate they are qualified by a gap-less density of states. © 2013 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.

  3. Efficient O(N) integration for all-electron electronic structure calculation using numeric basis functions

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

    Havu, V.; Fritz Haber Institute of the Max Planck Society, Berlin; Blum, V.

    2009-12-01

    We consider the problem of developing O(N) scaling grid-based operations needed in many central operations when performing electronic structure calculations with numeric atom-centered orbitals as basis functions. We outline the overall formulation of localized algorithms, and specifically the creation of localized grid batches. The choice of the grid partitioning scheme plays an important role in the performance and memory consumption of the grid-based operations. Three different top-down partitioning methods are investigated, and compared with formally more rigorous yet much more expensive bottom-up algorithms. We show that a conceptually simple top-down grid partitioning scheme achieves essentially the same efficiency as themore » more rigorous bottom-up approaches.« less

  4. How the Electronic Structure in URu2Si2 Changes with Temperature: A High-Resolution Compton Scattering Study

    NASA Astrophysics Data System (ADS)

    Koizumi, Akihisa; Kubo, Yasunori; Motoyama, Gaku; Yamamura, Tomoo; Sakurai, Yoshiharu

    2018-06-01

    We have measured directional Compton profiles on the (001) plane in URu2Si2 single crystal at several temperatures. Two-dimensional electron occupation number densities (2D-EONDs) were obtained from the profiles through electron momentum reconstruction and Lock-Crisp-West folding analyses. We have also performed band calculations based on 5f-electron itinerant and localized models and derived theoretical 2D-EONDs for comparison. The experimental 2D-EOND at 300 K is well described by the localized model, and the 2D-EOND at 10 K is consistent with the theoretical one based on the itinerant model. The difference between 2D-EONDs at 30 and 100 K reflects a gradual change in the electronic structure, which reveals some of the crossover phenomena from localized to itinerant states. The change from localized to itinerant states is also reflected in a B(r) function, which is obtained in the reconstruction analysis and is an autocorrelation function of the wave function in the position space. The process by which the electronic structure in URu2Si2 changes is demonstrated through a series of experimental results.

  5. High-sensitivity visualization of localized electric fields using low-energy electron beam deflection

    NASA Astrophysics Data System (ADS)

    Jeong, Samuel; Ito, Yoshikazu; Edwards, Gary; Fujita, Jun-ichi

    2018-06-01

    The visualization of localized electronic charges on nanocatalysts is expected to yield fundamental information about catalytic reaction mechanisms. We have developed a high-sensitivity detection technique for the visualization of localized charges on a catalyst and their corresponding electric field distribution, using a low-energy beam of 1 to 5 keV electrons and a high-sensitivity scanning transmission electron microscope (STEM) detector. The highest sensitivity for visualizing a localized electric field was ∼0.08 V/µm at a distance of ∼17 µm from a localized charge at 1 keV of the primary electron energy, and a weak local electric field produced by 200 electrons accumulated on the carbon nanotube (CNT) apex can be visualized. We also observed that Au nanoparticles distributed on a CNT forest tended to accumulate a certain amount of charges, about 150 electrons, at a ‑2 V bias.

  6. Mechanism of the high transition temperature for the 1111-type iron-based superconductors R FeAsO (R =rare earth ): Synergistic effects of local structures and 4 f electrons

    NASA Astrophysics Data System (ADS)

    Zhang, Lifang; Meng, Junling; Liu, Xiaojuan; Yao, Fen; Meng, Jian; Zhang, Hongjie

    2017-07-01

    Among the iron-based superconductors, the 1111-type Fe-As-based superconductors REFeAs O1 -xFx (RE = rare earth) exhibit high transition temperatures (Tc) above 40 K. We perform first-principles calculations based on density functional theory with the consideration of both electronic correlations and spin-orbit couplings on rare earths and Fe ions to study the underlying mechanism as the microscopic structural distortions in REFeAsO tuned by both lanthanide contraction and external strain. The electronic structures evolve similarly in both cases. It is found that there exist an optimal structural regime that will not only initialize but also optimize the orbital fluctuations due to the competing Fe-As and Fe-Fe crystal fields. We also find that the key structural features in REFeAsO, such as As-Fe-As bond angle, intrinsically induce the modification of the Fermi surface and dynamic spin fluctuation. These results suggest that the superconductivity is mediated by antiferromagnetic spin fluctuations. Simultaneously, we show that the rare-earth 4 f electrons play important roles on the high transition temperature whose behavior might be analogous to that of the heavy-fermion superconductors. The superconductivity of these 1111-type iron-based superconductors with high-Tc is considered to originate from the synergistic effects of local structures and 4 f electrons.

  7. Electron localization and optical absorption of polygonal quantum rings

    NASA Astrophysics Data System (ADS)

    Sitek, Anna; Serra, Llorenç; Gudmundsson, Vidar; Manolescu, Andrei

    2015-06-01

    We investigate theoretically polygonal quantum rings and focus mostly on the triangular geometry where the corner effects are maximal. Such rings can be seen as short core-shell nanowires, a generation of semiconductor heterostructures with multiple applications. We show how the geometry of the sample determines the electronic energy spectrum, and also the localization of electrons, with effects on the optical absorption. In particular, we show that irrespective of the ring shape low-energy electrons are always attracted by corners and are localized in their vicinity. The absorption spectrum in the presence of a magnetic field shows only two peaks within the corner-localized state domain, each associated with different circular polarization. This picture may be changed by an external electric field which allows previously forbidden transitions, and thus enables the number of corners to be determined. We show that polygonal quantum rings allow absorption of waves from distant ranges of the electromagnetic spectrum within one sample.

  8. Electronic and structural transitions in dense liquid sodium.

    PubMed

    Raty, Jean-Yves; Schwegler, Eric; Bonev, Stanimir A

    2007-09-27

    At ambient conditions, the light alkali metals are free-electron-like crystals with a highly symmetric structure. However, they were found recently to exhibit unexpected complexity under pressure. It was predicted from theory--and later confirmed by experiment--that lithium and sodium undergo a sequence of symmetry-breaking transitions, driven by a Peierls mechanism, at high pressures. Measurements of the sodium melting curve have subsequently revealed an unprecedented (and still unexplained) pressure-induced drop in melting temperature from 1,000 K at 30 GPa down to room temperature at 120 GPa. Here we report results from ab initio calculations that explain the unusual melting behaviour in dense sodium. We show that molten sodium undergoes a series of pressure-induced structural and electronic transitions, analogous to those observed in solid sodium but commencing at much lower pressure in the presence of liquid disorder. As pressure is increased, liquid sodium initially evolves by assuming a more compact local structure. However, a transition to a lower-coordinated liquid takes place at a pressure of around 65 GPa, accompanied by a threefold drop in electrical conductivity. This transition is driven by the opening of a pseudogap, at the Fermi level, in the electronic density of states--an effect that has not hitherto been observed in a liquid metal. The lower-coordinated liquid emerges at high temperatures and above the stability region of a close-packed free-electron-like metal. We predict that similar exotic behaviour is possible in other materials as well.

  9. Electronic structure and magnetic properties of Ni-doped SnO2 thin films

    NASA Astrophysics Data System (ADS)

    Sharma, Mayuri; Kumar, Shalendra; Alvi, P. A.

    2018-05-01

    This paper reports the electronic structure and magnetic properties of Ni-doped SnO2 thin film which were grown on Si (100) substrate by PLD (pulse laser deposition) technique under oxygen partial pressure (PO2). For getting electronic structure and magnetic behavior, the films were characterized using near edge X-ray absorption fine structure spectroscopy (NEXAFS) and DC magnetization measurements. The NEXAFS study at Ni L3,2 edge has been done to understand the local environment of Ni and Sn ions within SnO2 lattice. DC magnetization measurement shows that the saturation magnetization increases with the increase in substitution of Ni2+ ions in the system.

  10. Electronic and local atomistic structure of MgSiO3 glass under pressure: a study of X-ray Raman scattering at the silicon and magnesium L-edges

    NASA Astrophysics Data System (ADS)

    Fukui, Hiroshi; Hiraoka, Nozomu

    2018-02-01

    We applied X-ray Raman scattering technique to MgSiO3 glass, a precursor to magnesium silicate melts, with respect to magnesium and silicon under high-pressure conditions as well as some polycrystalline phases of MgSiO3 at ambient conditions. We also performed ab initio calculations to interpret the X-ray Raman spectra. Experimentally obtained silicon L-edge spectra indicate that the local environment around silicon started changing at pressure above 10 GPa, where the electronic structure of oxygen is known to change. In contrast, the shape of the magnesium L-edge spectrum changed below 10 GPa. This indicates that the magnesium sites in MgSiO3 glass first distort and that the local structure around magnesium shows a wide variation under pressure. The framework structure consisting of silicon and oxygen changed above 10 GPa, where the coordination number of silicon was more than four. Our results imply that 6-oxygen-coordinated silicon was formed above 20 GPa.

  11. Electron Pitch-Angle Distribution in Pressure Balance Structures Measured by Ulysses/SWOOPS

    NASA Technical Reports Server (NTRS)

    Yamauchi, Yohei; Suess, Steven T.; Sakurai, Takashi; Six, N. Frank (Technical Monitor)

    2002-01-01

    Pressure balance structures (PBSs) are a common feature in the high-latitude solar wind near solar minimum. From previous studies, PBSs are believed to be remnants of coronal plumes. Yamauchi et al [2002] investigated the magnetic structures of the PBSs, applying a minimum variance analysis to Ulysses/Magnetometer data. They found that PBSs contain structures like current sheets or plasmoids, and suggested that PBSs are associated with network activity such as magnetic reconnection in the photosphere at the base of polar plumes. We have investigated energetic electron data from Ulysses/SWOOPS to see whether bi-directional electron flow exists and we have found evidence supporting the earlier conclusions. We find that 45 ot of 53 PBSs show local bi-directional or isotopic electron flux or flux associated with current-sheet structure. Only five events show the pitch-angle distribution expected for Alfvenic fluctuations. We conclude that PBSs do contain magnetic structures such as current sheets or plasmoids that are expected as a result of network activity at the base of polar plumes.

  12. Advancing Efficient All-Electron Electronic Structure Methods Based on Numeric Atom-Centered Orbitals for Energy Related Materials

    NASA Astrophysics Data System (ADS)

    Blum, Volker

    This talk describes recent advances of a general, efficient, accurate all-electron electronic theory approach based on numeric atom-centered orbitals; emphasis is placed on developments related to materials for energy conversion and their discovery. For total energies and electron band structures, we show that the overall accuracy is on par with the best benchmark quality codes for materials, but scalable to large system sizes (1,000s of atoms) and amenable to both periodic and non-periodic simulations. A recent localized resolution-of-identity approach for the Coulomb operator enables O (N) hybrid functional based descriptions of the electronic structure of non-periodic and periodic systems, shown for supercell sizes up to 1,000 atoms; the same approach yields accurate results for many-body perturbation theory as well. For molecular systems, we also show how many-body perturbation theory for charged and neutral quasiparticle excitation energies can be efficiently yet accurately applied using basis sets of computationally manageable size. Finally, the talk highlights applications to the electronic structure of hybrid organic-inorganic perovskite materials, as well as to graphene-based substrates for possible future transition metal compound based electrocatalyst materials. All methods described here are part of the FHI-aims code. VB gratefully acknowledges contributions by numerous collaborators at Duke University, Fritz Haber Institute Berlin, TU Munich, USTC Hefei, Aalto University, and many others around the globe.

  13. Electronics for Piezoelectric Smart Structures

    NASA Technical Reports Server (NTRS)

    Warkentin, D. J.; Tani, J.

    1997-01-01

    This paper briefly presents work addressing some of the basic considerations for the electronic components used in smart structures incorporating piezoelectric elements. After general remarks on the application of piezoelectric elements to the problem of structural vibration control, three main topics are described. Work to date on the development of techniques for embedding electronic components within structural parts is presented, followed by a description of the power flow and dissipation requirements of those components. Finally current work on the development of electronic circuits for use in an 'active wall' for acoustic noise is introduced.

  14. Fingerprint-Based Structure Retrieval Using Electron Density

    PubMed Central

    Yin, Shuangye; Dokholyan, Nikolay V.

    2010-01-01

    We present a computational approach that can quickly search a large protein structural database to identify structures that fit a given electron density, such as determined by cryo-electron microscopy. We use geometric invariants (fingerprints) constructed using 3D Zernike moments to describe the electron density, and reduce the problem of fitting of the structure to the electron density to simple fingerprint comparison. Using this approach, we are able to screen the entire Protein Data Bank and identify structures that fit two experimental electron densities determined by cryo-electron microscopy. PMID:21287628

  15. Magnetic Local Time Dependant Low Energy Electron Flux Models at Geostationary Earth Orbit

    NASA Astrophysics Data System (ADS)

    Boynton, R.; Balikhin, M. A.; Walker, S. N.

    2017-12-01

    The low energy electron fluxes in the outer radiation belts at Geostationary Earth Orbit (GEO) can vary widely in Magnetic Local Time (MLT). This spatial variation is due to the convective and substorm-associated electric fields and can take place on short time scales. This makes it difficult to deduce a data based model of the low energy electrons. For higher energies, where there is negligible spatial variation at a particular L-star, data based models employ averaged fluxes over the orbit. This removes the diurnal variation as GEO passes through various L-star due to the structure of Earth's magnetic field. This study develops a number of models for the low energy electron fluxes measured by GOES 13 and 15 for different MLT to capture the dynamics of the spatial variations.

  16. Electronic structures of of PuX (X=S, Se, Te)

    NASA Astrophysics Data System (ADS)

    Maehira, Takahiro; Sakai, Eijiro; Tatetsu, Yasutomi

    2013-08-01

    We have calculated the energy band structures and the Fermi surfaces of PuS, PuSe, and PuTe by using a self-consistent relativistic linear augmented-plane-wave method with the exchange and correlation potential in the local density approximation. In general, the energy bands near the Fermi level are mainly caused by the hybridization between the Pu 5 f and the monochalcogenide p electrons. The obtained main Fermi surfaces consisted of two hole sheets and one electron sheet, which were constructed from the band having both the Pu 5 f state and the monochalcogenide p state.

  17. High-Resolution Structural and Electronic Properties of Epitaxial Topological Crystalline Insulator Films

    NASA Astrophysics Data System (ADS)

    Dagdeviren, Omur; Zhou, Chao; Zou, Ke; Simon, Georg; Albright, Stephen; Mandal, Subhasish; Morales-Acosta, Mayra; Zhu, Xiaodong; Ismail-Beigi, Sohrab; Walker, Frederick; Ahn, Charles; Schwarz, Udo; Altman, Eric

    Revealing the local electronic properties of surfaces and their link to structural properties is an important problem for topological crystalline insulators (TCI) in which metallic surface states are protected by crystal symmetry. The microstructure and electronic properties of TCI SnTe film surfaces grown by molecular beam epitaxy were characterized using scanning probe microscopy. These results reveal the influence of various defects on the electronic properties: tilt boundaries leading to dislocation arrays that serve as periodic nucleation sites for pit growth; screw dislocations, and point defects. These features have varying length scale and display variations in the electronic structure of the surface, which are mapped with scanning tunneling microscopy images as standing waves superimposed on atomic scale images of the surface topography that consequently shape the wave patterns. Since the growth process results in symmetry breaking defects that patterns the topological states, we propose that the scanning probe tip can pattern the surface and electronic structure and enable the fabrication of topological devices on the SnTe surface. Financial support from the National Science Foundation through the Yale Materials Research Science and Engineering Center (Grant No. MRSEC DMR-1119826) and FAME.

  18. Criticality of the electron-nucleus cusp condition to local effective potential-energy theories

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

    Pan Xiaoyin; Sahni, Viraht; Graduate School of the City University of New York, 360 Fifth Avenue, New York, New York 10016

    2003-01-01

    Local(multiplicative) effective potential energy-theories of electronic structure comprise the transformation of the Schroedinger equation for interacting Fermi systems to model noninteracting Fermi or Bose systems whereby the equivalent density and energy are obtained. By employing the integrated form of the Kato electron-nucleus cusp condition, we prove that the effective electron-interaction potential energy of these model fermions or bosons is finite at a nucleus. The proof is general and valid for arbitrary system whether it be atomic, molecular, or solid state, and for arbitrary state and symmetry. This then provides justification for all prior work in the literature based on themore » assumption of finiteness of this potential energy at a nucleus. We further demonstrate the criticality of the electron-nucleus cusp condition to such theories by an example of the hydrogen molecule. We show thereby that both model system effective electron-interaction potential energies, as determined from densities derived from accurate wave functions, will be singular at the nucleus unless the wave function satisfies the electron-nucleus cusp condition.« less

  19. Local structural aspects of metal-metal transition in IrTe2 from x-ray PDF

    NASA Astrophysics Data System (ADS)

    Yu, Runze; Abeykoon, Milinda; Zhou, Haidong; Yin, Weiguo; Bozin, Emil S.

    Evolution of local atomic structure across the metal-metal transition in IrTe2 is explored by pair distribution function (PDF) analysis of x-ray total scattering data over 80 K Local and average structures are found to be in accord at all temperatures conforming to P-1 and P-3m1 symmetry at low and high temperature, respectively. We find no evidence of short-range Ir-dimers surviving into the high-T regime, in stark contrast to the earlier EXAFS study proposing Ir-dimer order-disorder mechanism. Phase fraction obtained from explicit 2-phase structural modeling displays hysteretic behavior across the transition, in agreement with electronic transport measurements, indicative of a strong tie between the lattice and electronic configurations. Bond valence methodology applied to structural parameters further indicates significant bond charge disproportionation in association with the transition. Work at Brookhaven National Laboratory was supported by US DOE, Office of Science, Office of Basic Energy Sciences (DOE-BES) under Contract No. DE-SC0012704.

  20. Effect of potassium doping on electronic structure and thermoelectric properties of topological crystalline insulator

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

    Roychowdhury, Subhajit; Biswas, Kanishka, E-mail: kanishka@jncasr.ac.in; Sandhya Shenoy, U.

    2016-05-09

    Topological crystalline insulator (TCI), Pb{sub 0.6}Sn{sub 0.4}Te, exhibits metallic surface states protected by crystal mirror symmetry with negligibly small band gap. Enhancement of its thermoelectric performances needs tuning of its electronic structure particularly through engineering of its band gap. While physical perturbations tune the electronic structure of TCI by breaking of the crystal mirror symmetry, chemical means such as doping have been more attractive recently as they result in better thermoelectric performance in TCIs. Here, we demonstrate that K doping in TCI, Pb{sub 0.6}Sn{sub 0.4}Te, breaks the crystal mirror symmetry locally and widens electronic band gap, which is confirmed bymore » direct electronic absorption spectroscopy and electronic structure calculations. K doping in Pb{sub 0.6}Sn{sub 0.4}Te increases p-type carrier concentration and suppresses the bipolar conduction via widening a band gap, which collectively boosts the thermoelectric figure of merit (ZT) to 1 at 708 K.« less

  1. Quantum transport through disordered 1D wires: Conductance via localized and delocalized electrons

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

    Gopar, Víctor A.

    Coherent electronic transport through disordered systems, like quantum wires, is a topic of fundamental and practical interest. In particular, the exponential localization of electron wave functions-Anderson localization-due to the presence of disorder has been widely studied. In fact, Anderson localization, is not an phenomenon exclusive to electrons but it has been observed in microwave and acoustic experiments, photonic materials, cold atoms, etc. Nowadays, many properties of electronic transport of quantum wires have been successfully described within a scaling approach to Anderson localization. On the other hand, anomalous localization or delocalization is, in relation to the Anderson problem, a less studiedmore » phenomenon. Although one can find signatures of anomalous localization in very different systems in nature. In the problem of electronic transport, a source of delocalization may come from symmetries present in the system and particular disorder configurations, like the so-called Lévy-type disorder. We have developed a theoretical model to describe the statistical properties of transport when electron wave functions are delocalized. In particular, we show that only two physical parameters determine the complete conductance distribution.« less

  2. Plasmonic hot electron transport drives nano-localized chemistry

    PubMed Central

    Cortés, Emiliano; Xie, Wei; Cambiasso, Javier; Jermyn, Adam S.; Sundararaman, Ravishankar; Narang, Prineha; Schlücker, Sebastian; Maier, Stefan A.

    2017-01-01

    Nanoscale localization of electromagnetic fields near metallic nanostructures underpins the fundamentals and applications of plasmonics. The unavoidable energy loss from plasmon decay, initially seen as a detriment, has now expanded the scope of plasmonic applications to exploit the generated hot carriers. However, quantitative understanding of the spatial localization of these hot carriers, akin to electromagnetic near-field maps, has been elusive. Here we spatially map hot-electron-driven reduction chemistry with 15 nm resolution as a function of time and electromagnetic field polarization for different plasmonic nanostructures. We combine experiments employing a six-electron photo-recycling process that modify the terminal group of a self-assembled monolayer on plasmonic silver nanoantennas, with theoretical predictions from first-principles calculations of non-equilibrium hot-carrier transport in these systems. The resulting localization of reactive regions, determined by hot-carrier transport from high-field regions, paves the way for improving efficiency in hot-carrier extraction science and nanoscale regio-selective surface chemistry. PMID:28348402

  3. Fingerprint-based structure retrieval using electron density.

    PubMed

    Yin, Shuangye; Dokholyan, Nikolay V

    2011-03-01

    We present a computational approach that can quickly search a large protein structural database to identify structures that fit a given electron density, such as determined by cryo-electron microscopy. We use geometric invariants (fingerprints) constructed using 3D Zernike moments to describe the electron density, and reduce the problem of fitting of the structure to the electron density to simple fingerprint comparison. Using this approach, we are able to screen the entire Protein Data Bank and identify structures that fit two experimental electron densities determined by cryo-electron microscopy. Copyright © 2010 Wiley-Liss, Inc.

  4. Local electric field direct writing – Electron-beam lithography and mechanism

    DOE PAGES

    Jiang, Nan; Su, Dong; Spence, John C. H.

    2017-08-24

    Local electric field induced by a focused electron probe in silicate glass thin films is evaluated in this paper by the migration of cations. Extremely strong local electric fields can be obtained by the focused electron probe from a scanning transmission electron microscope. As a result, collective atomic displacements occur. This newly revised mechanism provides an efficient tool to write patterned nanostructures directly, and thus overcome the low efficiency of the conventional electron-beam lithography. Applying this technique to silicate glass thin films, as an example, a grid of rods of nanometer dimension can be efficiently produced by rapidly scanning amore » focused electron probe. This nanopatterning is achieved through swift phase separation in the sample, without any post-development processes. The controlled phase separation is induced by massive displacements of cations (glass modifiers) within the glass-former network, driven by the strong local electric fields. The electric field is induced by accumulated charge within the electron probed region, which is generated by the excitation of atomic electrons by the incident electron. Throughput is much improved compared to other scanning probe techniques. Finally, the half-pitch spatial resolution of nanostructure in this particular specimen is 2.5 nm.« less

  5. Local electric field direct writing – Electron-beam lithography and mechanism

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

    Jiang, Nan; Su, Dong; Spence, John C. H.

    Local electric field induced by a focused electron probe in silicate glass thin films is evaluated in this paper by the migration of cations. Extremely strong local electric fields can be obtained by the focused electron probe from a scanning transmission electron microscope. As a result, collective atomic displacements occur. This newly revised mechanism provides an efficient tool to write patterned nanostructures directly, and thus overcome the low efficiency of the conventional electron-beam lithography. Applying this technique to silicate glass thin films, as an example, a grid of rods of nanometer dimension can be efficiently produced by rapidly scanning amore » focused electron probe. This nanopatterning is achieved through swift phase separation in the sample, without any post-development processes. The controlled phase separation is induced by massive displacements of cations (glass modifiers) within the glass-former network, driven by the strong local electric fields. The electric field is induced by accumulated charge within the electron probed region, which is generated by the excitation of atomic electrons by the incident electron. Throughput is much improved compared to other scanning probe techniques. Finally, the half-pitch spatial resolution of nanostructure in this particular specimen is 2.5 nm.« less

  6. Non-local electron transport validation using 2D DRACO simulations

    NASA Astrophysics Data System (ADS)

    Cao, Duc; Chenhall, Jeff; Moll, Eli; Prochaska, Alex; Moses, Gregory; Delettrez, Jacques; Collins, Tim

    2012-10-01

    Comparison of 2D DRACO simulations, using a modified versionfootnotetextprivate communications with M. Marinak and G. Zimmerman, LLNL. of the Schurtz, Nicolai and Busquet (SNB) algorithmfootnotetextSchurtz, Nicolai and Busquet, ``A nonlocal electron conduction model for multidimensional radiation hydrodynamics codes,'' Phys. Plasmas 7, 4238(2000). for non-local electron transport, with direct drive shock timing experimentsfootnotetextT. Boehly, et. al., ``Multiple spherically converging shock waves in liquid deuterium,'' Phys. Plasmas 18, 092706(2011). and with the Goncharov non-local modelfootnotetextV. Goncharov, et. al., ``Early stage of implosion in inertial confinement fusion: Shock timing and perturbation evolution,'' Phys. Plasmas 13, 012702(2006). in 1D LILAC will be presented. Addition of an improved SNB non-local electron transport algorithm in DRACO allows direct drive simulations with no need for an electron conduction flux limiter. Validation with shock timing experiments that mimic the laser pulse profile of direct drive ignition targets gives a higher confidence level in the predictive capability of the DRACO code. This research was supported by the University of Rochester Laboratory for Laser Energetics.

  7. Numerical investigation of electron localization in polymer chains

    NASA Astrophysics Data System (ADS)

    Paulsson, Magnus; Stafström, Sven

    1998-01-01

    Using finite-size scaling, we have calculated the localization-delocalization phase diagrams for electronic wave functions in different disordered polymeric systems. The disorder considered here simulates finite polymer chain lengths, breaks in the conjugation, and disorder in an external potential. It is shown that a system of interacting chains, even at rather weak interchain interactions, allows for enough flexibility for the scattered waves to avoid dephasing and localization. Localization and the metal-insulator transition in highly conducting polymers are discussed in view of these results.

  8. Spin-orbit excitations and electronic structure of the putative Kitaev magnet α -RuCl3

    NASA Astrophysics Data System (ADS)

    Sandilands, Luke J.; Tian, Yao; Reijnders, Anjan A.; Kim, Heung-Sik; Plumb, K. W.; Kim, Young-June; Kee, Hae-Young; Burch, Kenneth S.

    2016-02-01

    Mott insulators with strong spin-orbit coupling have been proposed to host unconventional magnetic states, including the Kitaev quantum spin liquid. The 4 d system α -RuCl3 has recently come into view as a candidate Kitaev system, with evidence for unusual spin excitations in magnetic scattering experiments. We apply a combination of optical spectroscopy and Raman scattering to study the electronic structure of this material. Our measurements reveal a series of orbital excitations involving localized total angular momentum states of the Ru ion, implying that strong spin-orbit coupling and electron-electron interactions coexist in this material. Analysis of these features allows us to estimate the spin-orbit coupling strength, as well as other parameters describing the local electronic structure, revealing a well-defined hierarchy of energy scales within the Ru d states. By comparing our experimental results with density functional theory calculations, we also clarify the overall features of the optical response. Our results demonstrate that α -RuCl3 is an ideal material system to study spin-orbit coupled magnetism on the honeycomb lattice.

  9. Local representation of the electronic dielectric response function

    DOE PAGES

    Lu, Deyu; Ge, Xiaochuan

    2015-12-11

    We present a local representation of the electronic dielectric response function, based on a spatial partition of the dielectric response into contributions from each occupied Wannier orbital using a generalized density functional perturbation theory. This procedure is fully ab initio, and therefore allows us to rigorously define local metrics, such as “bond polarizability,” on Wannier centers. We show that the locality of the bare response function is determined by the locality of three quantities: Wannier functions of the occupied manifold, the density matrix, and the Hamiltonian matrix. Furthermore, in systems with a gap, the bare dielectric response is exponentially localized,more » which supports the physical picture of the dielectric response function as a collection of interacting local responses that can be captured by a tight-binding model.« less

  10. Observing electron localization in a dissociating H2+ molecule in real time

    PubMed Central

    Xu, H.; Li, Zhichao; He, Feng; Wang, X.; Atia-Tul-Noor, A.; Kielpinski, D.; Sang, R. T.; Litvinyuk, I. V.

    2017-01-01

    Dissociation of diatomic molecules with odd number of electrons always causes the unpaired electron to localize on one of the two resulting atomic fragments. In the simplest diatomic molecule H2+ dissociation yields a hydrogen atom and a proton with the sole electron ending up on one of the two nuclei. That is equivalent to breaking of a chemical bond—the most fundamental chemical process. Here we observe such electron localization in real time by performing a pump–probe experiment. We demonstrate that in H2+ electron localization is complete in just 15 fs when the molecule’s internuclear distance reaches 8 atomic units. The measurement is supported by a theoretical simulation based on numerical solution of the time-dependent Schrödinger equation. This observation advances our understanding of detailed dynamics of molecular dissociation. PMID:28621332

  11. Localization-delocalization transition of electrons at the percolation threshold of semiconductor GaAs 1–xN x alloys: The appearance of a mobility edge

    DOE PAGES

    Alberi, K.; Fluegel, B.; Beaton, D. A.; ...

    2012-07-09

    Electrons in semiconductor alloys have generally been described in terms of Bloch states that evolve from constructive interference of electron waves scattering from perfectly periodic potentials, despite the loss of structural periodicity that occurs on alloying. Using the semiconductor alloy GaAs₁₋ xN x as a prototype, we demonstrate a localized to delocalized transition of the electronic states at a percolation threshold, the emergence of a mobility edge, and the onset of an abrupt perturbation to the host GaAs electronic structure, shedding light on the evolution of electronic structure in these abnormal alloys.

  12. Electronic and structural properties of vacancies and hydrogen adsorbates on trilayer graphene

    NASA Astrophysics Data System (ADS)

    Menezes, Marcos G.; Capaz, Rodrigo B.

    2015-08-01

    Using ab initio calculations, we study the electronic and structural properties of vacancies and hydrogen adsorbates on trilayer graphene. Those defects are found to share similar low-energy electronic features, since they both remove a pz electron from the honeycomb lattice and induce a defect level near the Fermi energy. However, a vacancy also leaves unpaired σ electrons on the lattice, which lead to important structural differences and also contribute to magnetism. We explore both ABA and ABC stackings and compare properties such as formation energies, magnetic moments, spin density and the local density of states (LDOS) of the defect levels. These properties show a strong sensitivity to the layer in which the defect is placed and smaller sensitivities to sublattice placing and stacking type. Finally, for the ABC trilayer, we also study how these states behave in the presence of an external field, which opens a tunable gap in the band structure of the non-defective system. The pz defect states show a strong hybridization with band states as the field increases, with reduction and eventually loss of magnetization, and a non-magnetic, midgap-like state is found when the defect is at the middle layer.

  13. Electronic and Structural Properties of Vacancies and Hydrogen Adsorbates on Trilayer Graphene

    NASA Astrophysics Data System (ADS)

    Menezes, Marcos; Capaz, Rodrigo

    2015-03-01

    Using ab initio calculations, we study the electronic and structural properties of vacancies and hydrogen adsorbates on trilayer graphene. Those defects are found to share similar low-energy electronic features, since they both remove a pz electron from the honeycomb lattice and induce a defect level near the Fermi energy. However, a vacancy also leaves unpaired σ electrons on the lattice, which lead to important structural differences and also contribute to magnetism. We explore both ABA and ABC stackings and compare properties such as formation energies, magnetic moments, spin density and the local density of states (LDOS) of the defect levels. These properties show a strong sensitivity to the layer in which the defect is placed and smaller sensitivities to sublattice placing and stacking type. Finally, for the ABC trilayer, we also study how these states behave in the presence of an external electrical field, which opens a tunable gap in the band structure of the non-defective system. The pz defect states show a strong hybridization with band states as the field increases, with reduction and eventually loss of magnetization, and a non-magnetic, midgap-like state is found when the defect is at the middle layer.

  14. Unravelling surface and interfacial structures of a metal-organic framework by transmission electron microscopy.

    PubMed

    Zhu, Yihan; Ciston, Jim; Zheng, Bin; Miao, Xiaohe; Czarnik, Cory; Pan, Yichang; Sougrat, Rachid; Lai, Zhiping; Hsiung, Chia-En; Yao, Kexin; Pinnau, Ingo; Pan, Ming; Han, Yu

    2017-05-01

    Metal-organic frameworks (MOFs) are crystalline porous materials with designable topology, porosity and functionality, having promising applications in gas storage and separation, ion conduction and catalysis. It is challenging to observe MOFs with transmission electron microscopy (TEM) due to the extreme instability of MOFs upon electron beam irradiation. Here, we use a direct-detection electron-counting camera to acquire TEM images of the MOF ZIF-8 with an ultralow dose of 4.1 electrons per square ångström to retain the structural integrity. The obtained image involves structural information transferred up to 2.1 Å, allowing the resolution of individual atomic columns of Zn and organic linkers in the framework. Furthermore, TEM reveals important local structural features of ZIF-8 crystals that cannot be identified by diffraction techniques, including armchair-type surface terminations and coherent interfaces between assembled crystals. These observations allow us to understand how ZIF-8 crystals self-assemble and the subsequent influence of interfacial cavities on mass transport of guest molecules.

  15. Unravelling surface and interfacial structures of a metal-organic framework by transmission electron microscopy

    NASA Astrophysics Data System (ADS)

    Zhu, Yihan; Ciston, Jim; Zheng, Bin; Miao, Xiaohe; Czarnik, Cory; Pan, Yichang; Sougrat, Rachid; Lai, Zhiping; Hsiung, Chia-En; Yao, Kexin; Pinnau, Ingo; Pan, Ming; Han, Yu

    2017-05-01

    Metal-organic frameworks (MOFs) are crystalline porous materials with designable topology, porosity and functionality, having promising applications in gas storage and separation, ion conduction and catalysis. It is challenging to observe MOFs with transmission electron microscopy (TEM) due to the extreme instability of MOFs upon electron beam irradiation. Here, we use a direct-detection electron-counting camera to acquire TEM images of the MOF ZIF-8 with an ultralow dose of 4.1 electrons per square ångström to retain the structural integrity. The obtained image involves structural information transferred up to 2.1 Å, allowing the resolution of individual atomic columns of Zn and organic linkers in the framework. Furthermore, TEM reveals important local structural features of ZIF-8 crystals that cannot be identified by diffraction techniques, including armchair-type surface terminations and coherent interfaces between assembled crystals. These observations allow us to understand how ZIF-8 crystals self-assemble and the subsequent influence of interfacial cavities on mass transport of guest molecules.

  16. Local structure distortion induced by Ti dopants boosting the pseudocapacitance of RuO2-based supercapacitors.

    PubMed

    Chen, I-Li; Wei, Yu-Chen; Lu, Kueih-Tzu; Chen, Tsan-Yao; Hu, Chi-Chang; Chen, Jin-Ming

    2015-10-07

    Binary oxides with atomic ratios of Ru/Ti = 90/10, 70/30, and 50/50 were fabricated using H2O2-oxidative precipitation with the assistance of a cetyltrimethylammonium bromide (CTAB) template, followed by a thermal treatment at 200 °C. The characteristics of electron structure and local structure extracted from X-ray absorption spectroscopy (XAS) and transmission electron microscopy (TEM) analyses indicate that incorporation of Ti into the RuO2 lattice produces not only the local structural distortion of the RuO6 octahedra in (Ru-Ti)O2 with an increase in the central Ru-Ru distance but also a local crystallization of RuO2. Among the three binary oxides studied, (Ru70-Ti30)O2 exhibits a capacitance improvement of about 1.4-fold relative to the CTAB-modified RuO2, mainly due to the enhanced crystallinity of the distorted RuO6 structure rather than the surface area effect. Upon increasing the extent of Ti doping, the deteriorated supercapacitive performance of (Ru50-Ti50)O2 results from the formation of localized nano-clusters of TiO2 crystallites. These results provide insight into the important role of Ti doping in RuO2 that boosts the pseudocapacitive performance for RuO2-based supercapacitors. The present result is crucial for the design of new binary oxides for supercapacitor applications with extraordinary performance.

  17. Chemical Defects, Electronic Structure, and Transport in N-type and P-type Organic Semiconductors: First Principles Theory

    DTIC Science & Technology

    2012-11-29

    of localized states extending into the gap. We also introduced a simple model allowing estimates of the upper limit of the intra-grain mobility in...well as to pentacene , and DATT. This research will be described below. In addition to our work on the electronic structure and charge mobility, we have...stacking distance gives rise to a tail of localized states which act as traps for electrons and holes. We introduced a simple effective Hamiltonian model

  18. Electronic Structure of Semiconductor Interfaces.

    DTIC Science & Technology

    1984-11-01

    Workshop on Effective One-Electron Potentials In Real Materials, Ossining , New York, Mar. 21-22, 1980 Member, Organizing Committee, Annual Conferences on...Workshop on Effective One-Electron Potentials in Real Materials, Ossining , New York, Mar. 21-22, 1980 (Invited Paper) Electronic Structure of

  19. Effect of strain on the electronic structure and optical properties of germanium

    NASA Astrophysics Data System (ADS)

    Wen, Shumin; Zhao, Chunwang; Li, Jijun; Hou, Qingyu

    2018-05-01

    The effects of biaxial strain parallel to the (001) plane on the electronic structures and optical properties of Ge are calculated using the first-principles plane-wave pseudopotential method based on density functional theory. The screened-exchange local-density approximation function was used to obtain more reliable band structures, while strain was changed from ‑4% to +4%. The results show that the bandgap of Ge decreases with the increase of strain. Ge becomes a direct-bandgap semiconductor when the tensile strain reaches to 2%, which is in good agreement with the experimental results. The density of electron states of strained Ge becomes more localized. The tensile strain can increase the static dielectric constant distinctly, whereas the compressive strain can decrease the static dielectric constant slightly. The strain makes the absorption band edge move toward low energy. Both the tensile strain and compressive strain can significantly increase the reflectivity in the range from 7 eV to 14 eV. The tensile strain can decrease the optical conductivity, but the compressive strain can increase the optical conductivity significantly.

  20. Structural “ δ Doping” to Control Local Magnetization in Isovalent Oxide Heterostructures

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

    Moon, E. J.; He, Q.; Ghosh, S.

    Modulation and δ-doping strategies, in which atomically thin layers of charged dopants are precisely deposited within a heterostructure, have played enabling roles in the discovery of new physical behavior in electronic materials. Here in this paper, we demonstrate a purely structural “δ-doping” strategy in complex oxide heterostructures, in which atomically thin manganite layers are inserted into an isovalent manganite host, thereby modifying the local rotations of corner-connected MnO 6 octahedra. Combining scanning transmission electron microscopy, polarized neutron reflectometry, and density functional theory, we reveal how local magnetic exchange interactions are enhanced within the spatially confined regions of suppressed octahedral rotations.more » Finally, the combined experimental and theoretical results illustrate the potential to utilize noncharge-based approaches to “doping” in order to enhance or suppress functional properties within spatially confined regions of oxide heterostructures.« less

  1. Structural “ δ Doping” to Control Local Magnetization in Isovalent Oxide Heterostructures

    DOE PAGES

    Moon, E. J.; He, Q.; Ghosh, S.; ...

    2017-11-08

    Modulation and δ-doping strategies, in which atomically thin layers of charged dopants are precisely deposited within a heterostructure, have played enabling roles in the discovery of new physical behavior in electronic materials. Here in this paper, we demonstrate a purely structural “δ-doping” strategy in complex oxide heterostructures, in which atomically thin manganite layers are inserted into an isovalent manganite host, thereby modifying the local rotations of corner-connected MnO 6 octahedra. Combining scanning transmission electron microscopy, polarized neutron reflectometry, and density functional theory, we reveal how local magnetic exchange interactions are enhanced within the spatially confined regions of suppressed octahedral rotations.more » Finally, the combined experimental and theoretical results illustrate the potential to utilize noncharge-based approaches to “doping” in order to enhance or suppress functional properties within spatially confined regions of oxide heterostructures.« less

  2. Visualizing spatial correlation: structural and electronic orders in iron-based superconductors on atomic scale

    NASA Astrophysics Data System (ADS)

    Maksov, Artem; Ziatdinov, Maxim; Li, Li; Sefat, Athena; Maksymovych, Petro; Kalinin, Sergei

    Crystalline matter on the nanoscale level often exhibits strongly inhomogeneous structural and electronic orders, which have a profound effect on macroscopic properties. This may be caused by subtle interplay between chemical disorder, strain, magnetic, and structural order parameters. We present a novel approach based on combination of high resolution scanning tunneling microscopy/spectroscopy (STM/S) and deep data style analysis for automatic separation, extraction, and correlation of structural and electronic behavior which might lead us to uncovering the underlying sources of inhomogeneity in in iron-based family of superconductors (FeSe, BaFe2As2) . We identify STS spectral features using physically robust Bayesian linear unmixing, and show their direct relevance to the fundamental physical properties of the system, including electronic states associated with individual defects and impurities. We collect structural data from individual unit cells on the crystalline lattice, and calculate both global and local indicators of spatial correlation with electronic features, demonstrating, for the first time, a direct quantifiable connection between observed structural order parameters extracted from the STM data and electronic order parameters identified within the STS data. This research was sponsored by the Division of Materials Sciences and Engineering, Office of Science, Basic Energy Sciences, US DOE.

  3. Structural, electronic and optical properties of well-known primary explosive: Mercury fulminate

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

    Yedukondalu, N.; Vaitheeswaran, G., E-mail: gvsp@uohyd.ernet.in

    2015-11-28

    Mercury Fulminate (MF) is one of the well-known primary explosives since 17th century and it has rendered invaluable service over many years. However, the correct molecular and crystal structures are determined recently after 300 years of its discovery. In the present study, we report pressure dependent structural, elastic, electronic and optical properties of MF. Non-local correction methods have been employed to capture the weak van der Waals interactions in layered and molecular energetic MF. Among the non-local correction methods tested, optB88-vdW method works well for the investigated compound. The obtained equilibrium bulk modulus reveals that MF is softer than themore » well known primary explosives Silver Fulminate (SF), silver azide and lead azide. MF exhibits anisotropic compressibility (b > a > c) under pressure, consequently the corresponding elastic moduli decrease in the following order: C{sub 22} > C{sub 11} > C{sub 33}. The structural and mechanical properties suggest that MF is more sensitive to detonate along c-axis (similar to RDX) due to high compressibility of Hg⋯O non-bonded interactions along that axis. Electronic structure and optical properties were calculated including spin-orbit (SO) interactions using full potential linearized augmented plane wave method within recently developed Tran-Blaha modified Becke-Johnson (TB-mBJ) potential. The calculated TB-mBJ electronic structures of SF and MF show that these compounds are indirect bandgap insulators. Also, SO coupling is found to be more pronounced for 4d and 5d-states of Ag and Hg atoms of SF and MF, respectively. Partial density of states and electron charge density maps were used to describe the nature of chemical bonding. Ag—C bond is more directional than Hg—C bond which makes SF to be more unstable than MF. The effect of SO coupling on optical properties has also been studied and found to be significant for both (SF and MF) of the compounds.« less

  4. The limits of local correlation theory: electronic delocalization and chemically smooth potential energy surfaces.

    PubMed

    Subotnik, Joseph E; Sodt, Alex; Head-Gordon, Martin

    2008-01-21

    Local coupled-cluster theory provides an algorithm for measuring electronic correlation quickly, using only the spatial locality of localized electronic orbitals. Previously, we showed [J. Subotnik et al., J. Chem. Phys. 125, 074116 (2006)] that one may construct a local coupled-cluster singles-doubles theory which (i) yields smooth potential energy surfaces and (ii) achieves near linear scaling. That theory selected which orbitals to correlate based only on the distances between the centers of different, localized orbitals, and the approximate potential energy surfaces were characterized as smooth using only visual identification. This paper now extends our previous algorithm in three important ways. First, locality is now based on both the distances between the centers of orbitals as well as the spatial extent of the orbitals. We find that, by accounting for the spatial extent of a delocalized orbital, one can account for electronic correlation in systems with some electronic delocalization using fast correlation methods designed around orbital locality. Second, we now enforce locality on not just the amplitudes (which measure the exact electron-electron correlation), but also on the two-electron integrals themselves (which measure the bare electron-electron interaction). Our conclusion is that we can bump integrals as well as amplitudes, thereby gaining a tremendous increase in speed and paradoxically increasing the accuracy of our LCCSD approach. Third and finally, we now make a rigorous definition of chemical smoothness as requiring that potential energy surfaces not support artificial maxima, minima, or inflection points. By looking at first and second derivatives from finite difference techniques, we demonstrate complete chemical smoothness of our potential energy surfaces (bumping both amplitudes and integrals). These results are significant both from a theoretical and from a computationally practical point of view.

  5. Electronic structure of stoichiometric and reduced ZnO from periodic relativistic all electron hybrid density functional calculations using numeric atom-centered orbitals.

    PubMed

    Viñes, Francesc; Illas, Francesc

    2017-03-30

    The atomic and electronic structure of stoichiometric and reduced ZnO wurtzite has been studied using a periodic relativistic all electron hybrid density functional (PBE0) approach and numeric atom-centered orbital basis set with quality equivalent to aug-cc-pVDZ. To assess the importance of relativistic effects, calculations were carried out without and with explicit inclusion of relativistic effects through the zero order regular approximation. The calculated band gap is ∼0.2 eV smaller than experiment, close to previous PBE0 results including relativistic calculation through the pseudopotential and ∼0.25 eV smaller than equivalent nonrelativistic all electron PBE0 calculations indicating possible sources of error in nonrelativistic all electron density functional calculations for systems containing elements with relatively high atomic number. The oxygen vacancy formation energy converges rather fast with the supercell size, the predicted value agrees with previously hybrid density functional calculations and analysis of the electronic structure evidences the presence of localized electrons at the vacancy site with a concomitant well localized peak in the density of states ∼0.5 eV above the top of the valence band and a significant relaxation of the Zn atoms near to the oxygen vacancy. Finally, present work shows that accurate results can be obtained in systems involving large supercells containing up to ∼450 atoms using a numeric atomic-centered orbital basis set within a full all electron description including scalar relativistic effects at an affordable cost. © 2017 Wiley Periodicals, Inc. © 2017 Wiley Periodicals, Inc.

  6. Local structure study of Fe dopants in Ni-deficit Ni 3Al alloys

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

    V. N. Ivanovski; Umicevic, A.; Belosevic-Cavor, J.

    2015-08-24

    We found that the local electronic and magnetic structure, hyperfine interactions, and phase composition of polycrystalline Ni–deficient Ni 3-x FexAl (x = 0.18 and 0.36) were investigated by means of 57 Fe Mössbauer spectroscopy. The samples were characterized by X–ray diffraction and magnetization measurements. The ab initio calculations performed with the projector augmented wave method and the calculations of the energies of iron point defects were done to elucidate the electronic structure and site preference of Fe doped Ni 3 Al. Moreover, the value of calculated electric field gradient tensor V zz=1.6 10 21Vm -2 matches well with the resultsmore » of Mössbauer spectroscopy and indicates that the Fe atoms occupy Ni sites.« less

  7. Electric field effect on the electronic structure of 2D Y2C electride

    NASA Astrophysics Data System (ADS)

    Oh, Youngtek; Lee, Junsu; Park, Jongho; Kwon, Hyeokshin; Jeon, Insu; Wng Kim, Sung; Kim, Gunn; Park, Seongjun; Hwang, Sung Woo

    2018-07-01

    Electrides are ionic compounds in which electrons confined in the interstitial spaces serve as anions and are attractive owing to their exotic physical and chemical properties in terms of their low work function and efficient charge-transfer characteristics. Depending on the topology of the anionic electrons, the surface electronic structures of electrides can be significantly altered. In particular, the electronic structures of two-dimensional (2D) electride surfaces are of interest because the localized anionic electrons at the interlayer space can be naturally exposed to cleaved surfaces. In this paper, we report the electronic structure of 2D Y2C electride surface using scanning tunneling microscopy (STM) and first-principles calculations, which reveals that anionic electrons at a cleaved surface are absorbed by the surface and subsequently resurged onto the surface due to an applied electric field. We highlight that the estranged anionic electrons caused by the electric field occupy the slightly shifted crystallographic site compared with a bulk Y2C electride. We also measure the work function of the Y2C single crystal, and it shows a slightly lower value than the calculated one, which appears to be due to the electric field from the STM junction.

  8. Electronic structure calculation by nonlinear optimization: Application to metals

    NASA Astrophysics Data System (ADS)

    Benedek, R.; Min, B. I.; Woodward, C.; Garner, J.

    1988-04-01

    There is considerable interest in the development of novel algorithms for the calculation of electronic structure (e.g., at the level of the local-density approximation of density-functional theory). In this paper we consider a first-order equation-of-motion method. Two methods of solution are described, one proposed by Williams and Soler, and the other base on a Born-Dyson series expansion. The extension of the approach to metallic systems is outlined and preliminary numerical calculations for Zintl-phase NaTl are presented.

  9. A Transport Model for Non-Local Heating of Electrons in ICP Reactors

    NASA Technical Reports Server (NTRS)

    Chang, C. H.; Bose, Deepak; Arnold, James O. (Technical Monitor)

    1998-01-01

    A new model has been developed for non-local heating of electrons in ICP reactors, based on a hydrodynamic approach. The model has been derived using the electron momentum conservation in azimuthal direction with electromagnetic and frictional forces respectively as driving force and damper of harmonic oscillatory motion of electrons. The resulting transport equations include the convection of azimuthal electron momentum in radial and axial directions, thereby accounting for the non-local effects. The azimuthal velocity of electrons and the resulting electrical current are coupled to the Maxwell's relations, thus forming a self-consistent model for non-local heating. This model is being implemented along with a set of Navier-Stokes equations for plasma dynamics and gas flow to simulate low-pressure (few mTorr's) ICP discharges. Characteristics of nitrogen plasma in a TCP 300mm etch reactor is being studied. The results will be compared against the available Langmuir probe measurements.

  10. A transport model for non-local heating of electrons in ICP reactors

    NASA Astrophysics Data System (ADS)

    Chang, C. H.; Bose, Deepak

    1998-10-01

    A new model has been developed for non-local heating of electrons in ICP reactors, based on a hydrodynamic approach. The model has been derived using the electron momentum conservation in azimuthal direction with electromagnetic and frictional forces respectively as driving force and damper of harmonic oscillatory motion of electrons. The resulting transport equations include the convection of azimuthal electron momentum in radial and axial directions, thereby accounting for the non-local effects. The azimuthal velocity of electrons and the resulting electrical current are coupled to the Maxwell's relations, thus forming a self-consistent model for non-local heating. This model is being implemented along with a set of Navier-Stokes equations for plasma dynamics and gas flow to simulate low-pressure (few mTorr's) ICP discharges. Characteristics of nitrogen plasma in a TCP 300mm etch reactor is being studied. The results will be compared against the available Langmuir probe measurements [Collison et al. JVST-A 16(1),1998].

  11. Local structure in BaTi O 3 - BiSc O 3 dipole glasses

    DOE PAGES

    Levin, I.; Krayzman, V.; Woicik, J. C.; ...

    2016-03-14

    Local structures in cubic perovskite-type (Ba 0.6Bi 0.4)(Ti 0.6Sc 0.4)O 3 solid solutions that exhibit reentrant dipole glass behavior have been studied with variable-temperature x-ray/neutron total scattering, extended x-ray absorption fine structure, and electron diffraction methods. Simultaneous fitting of these data using a reverse Monte Carlo algorithm provided instantaneous atomic configurations, which have been used to extract local displacements of the constituent species. The smaller Bi and Ti atoms exhibit probability density distributions that consist of 14 and 8 split sites, respectively. In contrast, Ba and Sc feature single-site distributions. The multisite distributions arise from large and strongly anisotropic off-centermore » displacements of Bi and Ti. The cation displacements are correlated over a short range, with a correlation length limited by chemical disorder. The magnitudes of these displacements and their anisotropy, which are largely determined by local chemistry, change relatively insignificantly on cooling from room temperature. The structure features a nonrandom distribution of local polarization with low-dimensional polar clusters that are several unit cells in size. In situ measurements of atomic pair-distribution function under applied electric field were used to study field-induced changes in the local structure; however, no significant effects besides lattice expansion in the direction of the field could be observed up to electric-field values of 4 kVmm -1.« less

  12. The degree of π electron delocalization and the formation of 3D-extensible sandwich structures.

    PubMed

    Wang, Xiang; Wang, Qiang; Yuan, Caixia; Zhao, Xue-Feng; Li, Jia-Jia; Li, Debao; Wu, Yan-Bo; Wang, Xiaotai

    2016-04-28

    DFT B3LYP/6-31G(d) calculations were performed to examine the feasibility of graphene-like C42H18 and starbenzene C6(BeH)6 (SBz) polymers as ligands of 3D-extensible sandwich compounds (3D-ESCs) with uninterrupted sandwich arrays. The results revealed that sandwich compounds with three or more C42H18 ligands were not feasible. The possible reason may be the localization of π electrons on certain C6 hexagons due to π-metal interactions, which makes the whole ligand lose its electronic structure basis (higher degree of π electron delocalization) to maintain the planar structure. For comparison, with the aid of benzene (Bz) molecules, the SBz polymers can be feasible ligands for designing 3D-ESCs because the C-Be interactions in individual SBz are largely ionic, which will deter the π electrons on one C6 ring from connecting to those on neighbouring C6 rings. This means that high degree of π electron delocalization is not necessary for maintaining the planarity of SBz polymers. Such a locally delocalized π electron structure is desirable for the ligands of 3D-ESCs. Remarkably, the formation of a sandwich compound with SBz is thermodynamically more favourable than that found for bis(Bz)chromium. The assembly of 3D-ESCs is largely exothermic, which will facilitate future experimental synthesis. The different variation trends on the HOMO-LUMO gaps in different directions (relative to the sandwich axes) suggest that they can be developed to form directional conductors or semiconductors, which may be useful in the production of electronic devices.

  13. Magnetic structure and local lattice distortion in giant negative thermal expansion material Mn3Cu1-xGexN

    NASA Astrophysics Data System (ADS)

    Iikubo, S.; Kodama, K.; Takenaka, K.; Takagi, H.; Shamoto, S.

    2010-11-01

    Magnetic and local structures in an antiperovskite system, Mn3Cu1-xGexN, with a giant negative thermal expansion have been studied by neutron powder diffraction measurement. We discuss (1) an importance of an averaged cubic crystal structure and a ΓG5g antiferromagnetic spin structure for the large magneto-volume effect (MVE) in this itinerant electron system, (2) an unique role of a local lattice distortion well described by the low temperature tetragonal structure of Mn3GeN for the broadening of MVE.

  14. Self-consistent electronic structure of disordered Fe/sub 0. 65/Ni/sub 0. 35/

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

    Johnson, D.D.; Pinski, F.J.; Stocks, G.M.

    1985-04-15

    We present the results of the first ab initio calculation of the electronic structure of the disordered alloy Fe/sub 0.65/Ni/sub 0.35/. The calculation is based on the multiple-scattering coherent-potential approach (KKR-CPA) and is fully self-consistent and spin polarized. Magnetic effects are included within local-spin-density functional theory using the exchange-correlation function of Vosko--Wilk--Nusair. The most striking feature of the calculation is that electrons of different spins experience different degrees of disorder. The minority spin electrons see a very large disorder, whereas the majority spin electrons see little disorder. Consequently, the minority spin density of states is smooth compared to the verymore » structured majority spin density of states. This difference is due to a subtle balance between exchange splitting and charge neutrality.« less

  15. Local structural distortion and electrical transport properties of Bi(Ni1/2Ti1/2)O3 perovskite under high pressure.

    PubMed

    Zhu, Jinlong; Yang, Liuxiang; Wang, Hsiu-Wen; Zhang, Jianzhong; Yang, Wenge; Hong, Xinguo; Jin, Changqing; Zhao, Yusheng

    2015-12-16

    Perovskite-structure materials generally exhibit local structural distortions that are distinct from long-range, average crystal structure. The characterization of such distortion is critical to understanding the structural and physical properties of materials. In this work, we combined Pair Distribution Function (PDF) technique with Raman spectroscopy and electrical resistivity measurement to study Bi(Ni1/2Ti1/2)O3 perovskite under high pressure. PDF analysis reveals strong local structural distortion at ambient conditions. As pressure increases, the local structure distortions are substantially suppressed and eventually vanish around 4 GPa, leading to concurrent changes in the electronic band structure and anomalies in the electrical resistivity. Consistent with PDF analysis, Raman spectroscopy data suggest that the local structure changes to a higher ordered state at pressures above 4 GPa.

  16. Electronic Structures of Silicene Nanoribbons: Two-Edge-Chemistry Modification and First-Principles Study.

    PubMed

    Yao, Yin; Liu, Anping; Bai, Jianhui; Zhang, Xuanmei; Wang, Rui

    2016-12-01

    In this paper, we investigate the structural and electronic properties of zigzag silicene nanoribbons (ZSiNRs) with edge-chemistry modified by H, F, OH, and O, using the ab initio density functional theory method and local spin-density approximation. Three kinds of spin polarized configurations are considered: nonspin polarization (NM), ferromagnetic spin coupling for all electrons (FM), ferromagnetic ordering along each edge, and antiparallel spin orientation between the two edges (AFM). The H, F, and OH groups modified 8-ZSiNRs have the AFM ground state. The directly edge oxidized (O1) ZSiNRs yield the same energy and band structure for NM, FM, and AFM configurations, owning to the same s p (2) hybridization. And replacing the Si atoms on the two edges with O atoms (O2) yields FM ground state. The edge-chemistry-modified ZSiNRs all exhibit metallic band structures. And the modifications introduce special edge state strongly localized at the Si atoms in the edge, except for the O1 form. The modification of the zigzag edges of silicene nanoribbons is a key issue to apply the silicene into the field effect transistors (FETs) and gives more necessity to better understand the experimental findings.

  17. Defect Induced Electronic Structure of Uranofullerene

    PubMed Central

    Dai, Xing; Cheng, Cheng; Zhang, Wei; Xin, Minsi; Huai, Ping; Zhang, Ruiqin; Wang, Zhigang

    2013-01-01

    The interaction between the inner atoms/cluster and the outer fullerene cage is the source of various novel properties of endohedral metallofullerenes. Herein, we introduce an adatom-type spin polarization defect on the surface of a typical endohedral stable U2@C60 to predict the associated structure and electronic properties of U2@C61 based on the density functional theory method. We found that defect induces obvious changes in the electronic structure of this metallofullerene. More interestingly, the ground state of U2@C61 is nonet spin in contrast to the septet of U2@C60. Electronic structure analysis shows that the inner U atoms and the C ad-atom on the surface of the cage contribute together to this spin state, which is brought about by a ferromagnetic coupling between the spin of the unpaired electrons of the U atoms and the C ad-atom. This discovery may provide a possible approach to adapt the electronic structure properties of endohedral metallofullerenes. PMID:23439318

  18. Extensive electron transport and energization via multiple, localized dipolarizing flux bundles

    NASA Astrophysics Data System (ADS)

    Gabrielse, Christine; Angelopoulos, Vassilis; Harris, Camilla; Artemyev, Anton; Kepko, Larry; Runov, Andrei

    2017-05-01

    Using an analytical model of multiple dipolarizing flux bundles (DFBs) embedded in earthward traveling bursty bulk flows, we demonstrate how equatorially mirroring electrons can travel long distances and gain hundreds of keV from betatron acceleration. The model parameters are constrained by four Time History of Events and Macroscale Interactions during Substorms satellite observations, putting limits on the DFBs' speed, location, and magnetic and electric field magnitudes. We find that the sharp, localized peaks in magnetic field have such strong spatial gradients that energetic electrons ∇B drift in closed paths around the peaks as those peaks travel earthward. This is understood in terms of the third adiabatic invariant, which remains constant when the field changes on timescales longer than the electron's drift timescale: An energetic electron encircles a sharp peak in magnetic field in a closed path subtending an area of approximately constant flux. As the flux bundle magnetic field increases the electron's drift path area shrinks and the electron is prevented from escaping to the ambient plasma sheet, while it continues to gain energy via betatron acceleration. When the flux bundles arrive at and merge with the inner magnetosphere, where the background field is strong, the electrons suddenly gain access to previously closed drift paths around the Earth. DFBs are therefore instrumental in transporting and energizing energetic electrons over long distances along the magnetotail, bringing them to the inner magnetosphere and energizing them by hundreds of keV.Plain Language SummaryScientists have wondered how narrow flow channels in space could transport and energize <span class="hlt">electrons</span> enough before the <span class="hlt">electrons</span> escape the channel. They also wondered how narrow, <span class="hlt">localized</span> magnetic field peaks (and their electric fields) contribute to <span class="hlt">electron</span> energization in comparison to wide, large-scale electromagnetic fields. We show</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhRvB..94e4303W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhRvB..94e4303W"><span>Effect of spin-orbit and on-site Coulomb interactions on the <span class="hlt">electronic</span> <span class="hlt">structure</span> and lattice dynamics of uranium monocarbide</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wdowik, U. D.; Piekarz, P.; Legut, D.; Jagło, G.</p> <p>2016-08-01</p> <p>Uranium monocarbide, a potential fuel material for the generation IV reactors, is investigated within density functional theory. Its <span class="hlt">electronic</span>, magnetic, elastic, and phonon properties are analyzed and discussed in terms of spin-orbit interaction and <span class="hlt">localized</span> versus itinerant behavior of the 5 f <span class="hlt">electrons</span>. The <span class="hlt">localization</span> of the 5 f states is tuned by varying the <span class="hlt">local</span> Coulomb repulsion interaction parameter. We demonstrate that the theoretical <span class="hlt">electronic</span> <span class="hlt">structure</span>, elastic constants, phonon dispersions, and their densities of states can reproduce accurately the results of x-ray photoemission and bremsstrahlung isochromat measurements as well as inelastic neutron scattering experiments only when the 5 f states experience the spin-orbit interaction and simultaneously remain partially <span class="hlt">localized</span>. The partial <span class="hlt">localization</span> of the 5 f <span class="hlt">electrons</span> could be represented by a moderate value of the on-site Coulomb interaction parameter of about 2 eV. The results of the present studies indicate that both strong <span class="hlt">electron</span> correlations and spin-orbit effects are crucial for realistic theoretical description of the ground-state properties of uranium carbide.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1324570-time-dependent-local-average-structural-evolution-phase-ga-alloys','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1324570-time-dependent-local-average-structural-evolution-phase-ga-alloys"><span>Time-dependent <span class="hlt">local</span> and average <span class="hlt">structural</span> evolution of δ-phase 239Pu-Ga alloys</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Smith, Alice I.; Page, Katharine L.; Siewenie, Joan E.; ...</p> <p>2016-08-05</p> <p>Here, plutonium metal is a very unusual element, exhibiting six allotropes at ambient pressure, between room temperature and its melting point, a complicated phase diagram, and a complex <span class="hlt">electronic</span> <span class="hlt">structure</span>. Many phases of plutonium metal are unstable with changes in temperature, pressure, chemical additions, or time. This strongly affects <span class="hlt">structure</span> and properties, and becomes of high importance, particularly when considering effects on <span class="hlt">structural</span> integrity over long periods of time [1]. This paper presents a time-dependent neutron total scattering study of the <span class="hlt">local</span> and average <span class="hlt">structure</span> of naturally aging δ-phase 239Pu-Ga alloys, together with preliminary results on neutron tomography characterization.</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/2007APS..MARJ20005S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007APS..MARJ20005S"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of lead pyrophosphate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Suewattana, Malliga; Singh, David</p> <p>2007-03-01</p> <p>Lead Pyrophosphate Pb2P2O7 is of interest for potential radiation detection applications and use in long term waste storage. It forms in triclinic P1 crystals and can also be grown as glasses. We performed <span class="hlt">electronic</span> <span class="hlt">structure</span> calculations using the crystal <span class="hlt">structure</span> which determined by Mullica et. al (J. Solid State Chem (1986)) using x-ray diffraction and found large forces on atoms suggesting that the refined atomic positions were not fully correct. Here we report first principles <span class="hlt">structure</span> relaxation and a revised crystal <span class="hlt">structure</span> for this compound. We analyze the resulting <span class="hlt">structure</span> using pair distribution functions and discuss the implications for the <span class="hlt">electronic</span> properties. This work was supported by DOE NA22 and the Office of Naval Research.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MARP14004O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MARP14004O"><span>The CECAM <span class="hlt">Electronic</span> <span class="hlt">Structure</span> Library: community-driven development of software libraries for <span class="hlt">electronic</span> <span class="hlt">structure</span> simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Oliveira, Micael</p> <p></p> <p>The CECAM <span class="hlt">Electronic</span> <span class="hlt">Structure</span> Library (ESL) is a community-driven effort to segregate shared pieces of software as libraries that could be contributed and used by the community. Besides allowing to share the burden of developing and maintaining complex pieces of software, these can also become a target for re-coding by software engineers as hardware evolves, ensuring that <span class="hlt">electronic</span> <span class="hlt">structure</span> codes remain at the forefront of HPC trends. In a series of workshops hosted at the CECAM HQ in Lausanne, the tools and infrastructure for the project were prepared, and the first contributions were included and made available online (http://esl.cecam.org). In this talk I will present the different aspects and aims of the ESL and how these can be useful for the <span class="hlt">electronic</span> <span class="hlt">structure</span> community.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/942230-first-principles-electronic-structure-mn-doped-gaas-gap-gan-semiconductors','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/942230-first-principles-electronic-structure-mn-doped-gaas-gap-gan-semiconductors"><span>First Principles <span class="hlt">Electronic</span> <span class="hlt">Structure</span> of Mn doped GaAs, GaP, and GaN Semiconductors</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>Schulthess, Thomas C; Temmerman, Walter M; Szotek, Zdzislawa</p> <p></p> <p>We present first-principles <span class="hlt">electronic</span> <span class="hlt">structure</span> calculations of Mn doped III-V semiconductors based on the <span class="hlt">local</span> spin-density approximation (LSDA) as well as the self-interaction corrected <span class="hlt">local</span> spin density method (SIC-LSD). We find that it is crucial to use a self-interaction free approach to properly describe the <span class="hlt">electronic</span> ground state. The SIC-LSD calculations predict the proper <span class="hlt">electronic</span> ground state configuration for Mn in GaAs, GaP, and GaN. Excellent quantitative agreement with experiment is found for magnetic moment and p-d exchange in (GaMn)As. These results allow us to validate commonly used models for magnetic semiconductors. Furthermore, we discuss the delicate problem of extractingmore » binding energies of <span class="hlt">localized</span> levels from density functional theory calculations. We propose three approaches to take into account final state effects to estimate the binding energies of the Mn-d levels in GaAs. We find good agreement between computed values and estimates from photoemisison experiments.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFD.L1002R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFD.L1002R"><span>Discovering Coherent <span class="hlt">Structures</span> Using <span class="hlt">Local</span> Causal States</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rupe, Adam; Crutchfield, James P.; Kashinath, Karthik; Prabhat, Mr.</p> <p>2017-11-01</p> <p>Coherent <span class="hlt">structures</span> were introduced in the study of fluid dynamics and were initially defined as regions characterized by high levels of coherent vorticity, i.e. regions where instantaneously space and phase correlated vorticity are high. In a more general spatiotemporal setting, coherent <span class="hlt">structures</span> can be seen as <span class="hlt">localized</span> broken symmetries which persist in time. Building off the computational mechanics framework, which integrates tools from computation and information theory to capture pattern and <span class="hlt">structure</span> in nonlinear dynamical systems, we introduce a theory of coherent <span class="hlt">structures</span>, in the more general sense. Central to computational mechanics is the causal equivalence relation, and a <span class="hlt">local</span> spatiotemporal generalization of it is used to construct the <span class="hlt">local</span> causal states, which are utilized to uncover a system's spatiotemporal symmetries. Coherent <span class="hlt">structures</span> are then identified as persistent, <span class="hlt">localized</span> deviations from these symmetries. We illustrate how novel patterns and <span class="hlt">structures</span> can be discovered in cellular automata and outline the path from them to laminar, transitional and turbulent flows. Funded by Intel through the Big Data Center at LBNL and the IPCC at UC Davis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvB..95f4309B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvB..95f4309B"><span>Scattering of an <span class="hlt">electronic</span> wave packet by a one-dimensional <span class="hlt">electron</span>-phonon-coupled <span class="hlt">structure</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brockt, C.; Jeckelmann, E.</p> <p>2017-02-01</p> <p>We investigate the scattering of an <span class="hlt">electron</span> by phonons in a small <span class="hlt">structure</span> between two one-dimensional tight-binding leads. This model mimics the quantum <span class="hlt">electron</span> transport through atomic wires or molecular junctions coupled to metallic leads. The <span class="hlt">electron</span>-phonon-coupled <span class="hlt">structure</span> is represented by the Holstein model. We observe permanent energy transfer from the <span class="hlt">electron</span> to the phonon system (dissipation), transient self-trapping of the <span class="hlt">electron</span> in the <span class="hlt">electron</span>-phonon-coupled <span class="hlt">structure</span> (due to polaron formation and multiple reflections at the <span class="hlt">structure</span> edges), and transmission resonances that depend strongly on the strength of the <span class="hlt">electron</span>-phonon coupling and the adiabaticity ratio. A recently developed TEBD algorithm, optimized for bosonic degrees of freedom, is used to simulate the quantum dynamics of a wave packet launched against the <span class="hlt">electron</span>-phonon-coupled <span class="hlt">structure</span>. Exact results are calculated for a single <span class="hlt">electron</span>-phonon site using scattering theory and analytical approximations are obtained for limiting cases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..MAR.D7010A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..MAR.D7010A"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> and magnetic anisotropy of Sm2Fe17Nx</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Akai, Hisazumi; Ogura, Masako</p> <p>2014-03-01</p> <p><span class="hlt">Electronic</span> <span class="hlt">structure</span> and magnetic properties of Sm2Fe17Nx are studies on the basis of the first-principles <span class="hlt">electronic</span> <span class="hlt">structure</span> calculation in the framework of the density functional theory within the <span class="hlt">local</span> density and coherent potential approximations. The magnetic anisotropy of the system as a function of nitrogen concentration x is discussed by taking account not only of the crystal field effects but also of the effects of the f-<span class="hlt">electron</span> transfer from Sm to the neighboring sites. Also discussed is the magnetic transition temperature that is estimated by mapping the system into a Heisenberg model. The results show the crystalline magnetic anisotropy changes its direction from in-plane to uniaxial ones as x increases. It takes the maximum value near x ~ 2 . 8 and then decreases slightly towards x = 3 . The mechanism for these behaviors is discussed in the light of the results of detailed calculations on the bonding properties between Sm and its neighboring N. This work was partly supported by Elements Strategy Initiative Center for Magnetic Materials Project, the Ministry of Education, Culture, Sports, Science and Technology, Japan.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25181032','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25181032"><span>Crossed Ga2O3/SnO2 multiwire architecture: a <span class="hlt">local</span> <span class="hlt">structure</span> study with nanometer resolution.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Martínez-Criado, Gema; Segura-Ruiz, Jaime; Chu, Manh-Hung; Tucoulou, Remi; López, Iñaki; Nogales, Emilio; Mendez, Bianchi; Piqueras, Javier</p> <p>2014-10-08</p> <p>Crossed nanowire <span class="hlt">structures</span> are the basis for high-density integration of a variety of nanodevices. Owing to the critical role of nanowires intersections in creating hybrid architectures, it has become a challenge to investigate the <span class="hlt">local</span> <span class="hlt">structure</span> in crossing points in metal oxide nanowires. Thus, if intentionally grown crossed nanowires are well-patterned, an ideal model to study the junction is formed. By combining <span class="hlt">electron</span> and synchrotron beam nanoprobes, we show here experimental evidence of the role of impurities in the coupling formation, <span class="hlt">structural</span> modifications, and atomic site configuration based on crossed Ga2O3/SnO2 nanowires. Our experiment opens new avenues for further <span class="hlt">local</span> <span class="hlt">structure</span> studies with both nanometer resolution and elemental sensitivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22658290-local-average-structure-mn-la-substituted-bifeo-sub','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22658290-local-average-structure-mn-la-substituted-bifeo-sub"><span><span class="hlt">Local</span> and average <span class="hlt">structure</span> of Mn- and La-substituted BiFeO{sub 3}</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>Jiang, Bo; Selbach, Sverre M., E-mail: selbach@ntnu.no</p> <p>2017-06-15</p> <p>The <span class="hlt">local</span> and average <span class="hlt">structure</span> of solid solutions of the multiferroic perovskite BiFeO{sub 3} is investigated by synchrotron X-ray diffraction (XRD) and <span class="hlt">electron</span> density functional theory (DFT) calculations. The average experimental <span class="hlt">structure</span> is determined by Rietveld refinement and the <span class="hlt">local</span> <span class="hlt">structure</span> by total scattering data analyzed in real space with the pair distribution function (PDF) method. With equal concentrations of La on the Bi site or Mn on the Fe site, La causes larger <span class="hlt">structural</span> distortions than Mn. <span class="hlt">Structural</span> models based on DFT relaxed geometry give an improved fit to experimental PDFs compared to models constrained by the space groupmore » symmetry. Berry phase calculations predict a higher ferroelectric polarization than the experimental literature values, reflecting that <span class="hlt">structural</span> disorder is not captured in either average <span class="hlt">structure</span> space group models or DFT calculations with artificial long range order imposed by periodic boundary conditions. Only by including point defects in a supercell, here Bi vacancies, can DFT calculations reproduce the literature results on the <span class="hlt">structure</span> and ferroelectric polarization of Mn-substituted BiFeO{sub 3}. The combination of <span class="hlt">local</span> and average <span class="hlt">structure</span> sensitive experimental methods with DFT calculations is useful for illuminating the <span class="hlt">structure</span>-property-composition relationships in complex functional oxides with <span class="hlt">local</span> <span class="hlt">structural</span> distortions. - Graphical abstract: The experimental and simulated partial pair distribution functions (PDF) for BiFeO{sub 3}, BiFe{sub 0.875}Mn{sub 0.125}O{sub 3}, BiFe{sub 0.75}Mn{sub 0.25}O{sub 3} and Bi{sub 0.9}La{sub 0.1}FeO{sub 3}.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1259300-local-structural-distortion-electrical-transport-properties-bi-ni1-o3-perovskite-under-high-pressure','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1259300-local-structural-distortion-electrical-transport-properties-bi-ni1-o3-perovskite-under-high-pressure"><span><span class="hlt">Local</span> <span class="hlt">structural</span> distortion and electrical transport properties of Bi(Ni 1/2Ti 1/2)O 3 perovskite under high pressure</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Zhu, Jinlong; Yang, Liuxiang; Wang, Hsiu -Wen; ...</p> <p>2015-12-16</p> <p>Perovskite-<span class="hlt">structure</span> materials generally exhibit <span class="hlt">local</span> <span class="hlt">structural</span> distortions that are distinct from long-range, average crystal <span class="hlt">structure</span>. The characterization of such distortion is critical to understanding the <span class="hlt">structural</span> and physical properties of materials. In this work, we combined Pair Distribution Function (PDF) technique with Raman spectroscopy and electrical resistivity measurement to study Bi(Ni 1/2Ti 1/2)O 3 perovskite under high pressure. PDF analysis reveals strong <span class="hlt">local</span> <span class="hlt">structural</span> distortion at ambient conditions. As pressure increases, the <span class="hlt">local</span> <span class="hlt">structure</span> distortions are substantially suppressed and eventually vanish around 4 GPa, leading to concurrent changes in the <span class="hlt">electronic</span> band <span class="hlt">structure</span> and anomalies in the electrical resistivity. Wemore » find, consistent with PDF analysis, Raman spectroscopy data suggest that the <span class="hlt">local</span> <span class="hlt">structure</span> changes to a higher ordered state at pressures above 4 GPa.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17125324','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17125324"><span><span class="hlt">Electron</span>-beam-induced topographical, chemical, and <span class="hlt">structural</span> patterning of amorphous titanium oxide films.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kern, P; Müller, Y; Patscheider, J; Michler, J</p> <p>2006-11-30</p> <p>Electrolytically deposited amorphous TiO2 films on steel are remarkably sensitive to <span class="hlt">electron</span> beam (e-beam) irradiation at moderate energies at 20 keV, resulting in controlled <span class="hlt">local</span> oxide reduction and crystallization, opening the possibility for <span class="hlt">local</span> topographical, chemical, and <span class="hlt">structural</span> modifications within a biocompatible, amorphous, and semiconducting matrix. The sensitivity is shown to vary significantly with the annealing temperature of as-deposited films. Well-defined irradiation conditions in terms of probe current IP (5 microA) and beam size were achieved with an <span class="hlt">electron</span> probe microanalyzer. As shown by atomic force and optical microscopy, micro-Raman spectroscopy, wavelength-dispersive X-ray (WDX), and Auger analyses, e-beam exposure below 1 Acm-2 immediately leads to <span class="hlt">electron</span>-stimulated oxygen desorption, resulting in a well-defined volume loss primarily limited to the irradiated zone under the <span class="hlt">electron</span> probe and in a blue color shift in this zone because of the presence of Ti2O3. Irradiation at 5 Acm(-2) (IP = 5 microA) results in <span class="hlt">local</span> crystallization into anatase phase within 1 s of exposure and in reduction to TiO after an extended exposure of 60 s. Further reduction to the metallic state could be observed after 60 s of exposure at approximately 160 Acm(-2). The <span class="hlt">local</span> reduction could be qualitatively sensed with WDX analysis and Auger line scans. An estimation of the film temperature in the beam center indicates that crystallization occurs at less than 150 degrees C, well below the atmospheric crystallization temperature of the present films. The high e-beam sensitivity in combination with the well-defined volume loss from oxygen desorption allows for precise <span class="hlt">electron</span> lithographic topographical patterning of the present oxides. Irradiation effects leading to the observed reduction and crystallization phenomena under moderate <span class="hlt">electron</span> energies are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRA..123.1900R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRA..123.1900R"><span>The Role of <span class="hlt">Localized</span> Compressional Ultra-low Frequency Waves in Energetic <span class="hlt">Electron</span> Precipitation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rae, I. Jonathan; Murphy, Kyle R.; Watt, Clare E. J.; Halford, Alexa J.; Mann, Ian R.; Ozeke, Louis G.; Sibeck, David G.; Clilverd, Mark A.; Rodger, Craig J.; Degeling, Alex W.; Forsyth, Colin; Singer, Howard J.</p> <p>2018-03-01</p> <p>Typically, ultra-low frequency (ULF) waves have historically been invoked for radial diffusive transport leading to acceleration and loss of outer radiation belt <span class="hlt">electrons</span>. At higher frequencies, very low frequency waves are generally thought to provide a mechanism for <span class="hlt">localized</span> acceleration and loss through precipitation into the ionosphere of radiation belt <span class="hlt">electrons</span>. In this study we present a new mechanism for <span class="hlt">electron</span> loss through precipitation into the ionosphere due to a direct modulation of the loss cone via <span class="hlt">localized</span> compressional ULF waves. We present a case study of compressional wave activity in tandem with riometer and balloon-borne <span class="hlt">electron</span> precipitation across keV-MeV energies to demonstrate that the experimental measurements can be explained by our new enhanced loss cone mechanism. Observational evidence is presented demonstrating that modulation of the equatorial loss cone can occur via <span class="hlt">localized</span> compressional wave activity, which greatly exceeds the change in pitch angle through conservation of the first and second adiabatic invariants. The precipitation response can be a complex interplay between <span class="hlt">electron</span> energy, the <span class="hlt">localization</span> of the waves, the shape of the phase space density profile at low pitch angles, ionospheric decay time scales, and the time dependence of the <span class="hlt">electron</span> source; we show that two pivotal components not usually considered are <span class="hlt">localized</span> ULF wave fields and ionospheric decay time scales. We conclude that enhanced precipitation driven by compressional ULF wave modulation of the loss cone is a viable candidate for direct precipitation of radiation belt <span class="hlt">electrons</span> without any additional requirement for gyroresonant wave-particle interaction. Additional mechanisms would be complementary and additive in providing means to precipitate <span class="hlt">electrons</span> from the radiation belts during storm times.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18298141','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18298141"><span><span class="hlt">Localized</span> basis sets for unbound <span class="hlt">electrons</span> in nanoelectronics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Soriano, D; Jacob, D; Palacios, J J</p> <p>2008-02-21</p> <p>It is shown how unbound <span class="hlt">electron</span> wave functions can be expanded in a suitably chosen <span class="hlt">localized</span> basis sets for any desired range of energies. In particular, we focus on the use of Gaussian basis sets, commonly used in first-principles codes. The possible usefulness of these basis sets in a first-principles description of field emission or scanning tunneling microscopy at large bias is illustrated by studying a simpler related phenomenon: The lifetime of an <span class="hlt">electron</span> in a H atom subjected to a strong electric field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930049945&hterms=millwater&qs=N%3D0%26Ntk%3DAuthor-Name%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dmillwater','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930049945&hterms=millwater&qs=N%3D0%26Ntk%3DAuthor-Name%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dmillwater"><span>Global/<span class="hlt">local</span> methods for probabilistic <span class="hlt">structural</span> analysis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Millwater, H. R.; Wu, Y.-T.</p> <p>1993-01-01</p> <p>A probabilistic global/<span class="hlt">local</span> method is proposed to reduce the computational requirements of probabilistic <span class="hlt">structural</span> analysis. A coarser global model is used for most of the computations with a <span class="hlt">local</span> more refined model used only at key probabilistic conditions. The global model is used to establish the cumulative distribution function (cdf) and the Most Probable Point (MPP). The <span class="hlt">local</span> model then uses the predicted MPP to adjust the cdf value. The global/<span class="hlt">local</span> method is used within the advanced mean value probabilistic algorithm. The <span class="hlt">local</span> model can be more refined with respect to the g1obal model in terms of finer mesh, smaller time step, tighter tolerances, etc. and can be used with linear or nonlinear models. The basis for this approach is described in terms of the correlation between the global and <span class="hlt">local</span> models which can be estimated from the global and <span class="hlt">local</span> MPPs. A numerical example is presented using the NESSUS probabilistic <span class="hlt">structural</span> analysis program with the finite element method used for the <span class="hlt">structural</span> modeling. The results clearly indicate a significant computer savings with minimal loss in accuracy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993ssdm.conf..701M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993ssdm.conf..701M"><span>Global/<span class="hlt">local</span> methods for probabilistic <span class="hlt">structural</span> analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Millwater, H. R.; Wu, Y.-T.</p> <p>1993-04-01</p> <p>A probabilistic global/<span class="hlt">local</span> method is proposed to reduce the computational requirements of probabilistic <span class="hlt">structural</span> analysis. A coarser global model is used for most of the computations with a <span class="hlt">local</span> more refined model used only at key probabilistic conditions. The global model is used to establish the cumulative distribution function (cdf) and the Most Probable Point (MPP). The <span class="hlt">local</span> model then uses the predicted MPP to adjust the cdf value. The global/<span class="hlt">local</span> method is used within the advanced mean value probabilistic algorithm. The <span class="hlt">local</span> model can be more refined with respect to the g1obal model in terms of finer mesh, smaller time step, tighter tolerances, etc. and can be used with linear or nonlinear models. The basis for this approach is described in terms of the correlation between the global and <span class="hlt">local</span> models which can be estimated from the global and <span class="hlt">local</span> MPPs. A numerical example is presented using the NESSUS probabilistic <span class="hlt">structural</span> analysis program with the finite element method used for the <span class="hlt">structural</span> modeling. The results clearly indicate a significant computer savings with minimal loss in accuracy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT.........3J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT.........3J"><span><span class="hlt">Electronic</span> <span class="hlt">Structure</span> and Surface Physics of Two-dimensional Material Molybdenum Disulfide</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jin, Wencan</p> <p></p> <p>The interest in two-dimensional materials and materials physics has grown dramatically over the past decade. The family of two-dimensional materials, which includes graphene, transition metal dichalcogenides, phosphorene, hexagonal boron nitride, etc., can be fabricated into atomically thin films since the intralayer bonding arises from their strong covalent character, while the interlayer interaction is mediated by weak van der Waals forces. Among them, molybdenum disulfide (MoS2) has attracted much interest for its potential applications in opto-<span class="hlt">electronic</span> and valleytronics devices. Previously, much of the experimental studies have concentrated on optical and transport measurements while neglecting direct experimental determination of the <span class="hlt">electronic</span> <span class="hlt">structure</span> of MoS2, which is crucial to the full understanding of its distinctive properties. In particular, like other atomically thin materials, the interactions with substrate impact the surface <span class="hlt">structure</span> and morphology of MoS2, and as a result, its <span class="hlt">structural</span> and physical properties can be affected. In this dissertation, the <span class="hlt">electronic</span> <span class="hlt">structure</span> and surface <span class="hlt">structure</span> of MoS2 are directly investigated using angle-resolved photoemission spectroscopy and cathode lens microscopy. <span class="hlt">Local</span>-probe angle-resolved photoemission spectroscopy measurements of monolayer, bilayer, trilayer, and bulk MoS 2 directly demonstrate the indirect-to-direct bandgap transition due to quantum confinement as the MoS2 thickness is decreased from multilayer to monolayer. The evolution of the interlayer coupling in this transition is also investigated using density functional theory calculations. Also, the thickness-dependent surface roughness is characterized using selected-area low energy <span class="hlt">electron</span> diffraction (LEED) and the surface <span class="hlt">structural</span> relaxation is investigated using LEED I-V measurements combined with dynamical LEED calculations. Finally, bandgap engineering is demonstrated via tuning of the interlayer interactions in van der Waals</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApPhL.106m3109K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApPhL.106m3109K"><span><span class="hlt">Localized</span> conductive patterning via focused <span class="hlt">electron</span> beam reduction of graphene oxide</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, Songkil; Kulkarni, Dhaval D.; Henry, Mathias; Zackowski, Paul; Jang, Seung Soon; Tsukruk, Vladimir V.; Fedorov, Andrei G.</p> <p>2015-03-01</p> <p>We report on a method for "direct-write" conductive patterning via reduction of graphene oxide (GO) sheets using focused <span class="hlt">electron</span> beam induced deposition (FEBID) of carbon. FEBID treatment of the intrinsically dielectric graphene oxide between two metal terminals opens up the conduction channel, thus enabling a unique capability for nanoscale conductive domain patterning in GO. An increase in FEBID <span class="hlt">electron</span> dose results in a significant increase of the domain electrical conductivity with improving linearity of drain-source current vs. voltage dependence, indicative of a change of graphene oxide <span class="hlt">electronic</span> properties from insulating to semiconducting. Density functional theory calculations suggest a possible mechanism underlying this experimentally observed phenomenon, as <span class="hlt">localized</span> reduction of graphene oxide layers via interactions with highly reactive intermediates of <span class="hlt">electron</span>-beam-assisted dissociation of surface-adsorbed hydrocarbon molecules. These findings establish an unusual route for using FEBID as nanoscale lithography and patterning technique for engineering carbon-based nanomaterials and devices with <span class="hlt">locally</span> tailored <span class="hlt">electronic</span> properties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JPhCS.377a2093S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JPhCS.377a2093S"><span><span class="hlt">Electron</span> band <span class="hlt">structure</span> of the high pressure cubic phase of AlH3</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shi, Hongliang; Zarifi, Niliffar; Yim, Wai-Leung; Tse, J. S.</p> <p>2012-07-01</p> <p>The <span class="hlt">electronic</span> band <span class="hlt">structure</span> of the cubic Pm3n phase of AlH3 stable above 100 GPa is examined with semi-<span class="hlt">local</span>, Tran-Blaha modified Becke-Johnson <span class="hlt">local</span> density approximation (TB-mBJLDA), screened hybrid density functionals and GW methods. The shift of the conduction band to higher energy with increasing pressure is predicted by all methods. However, there are significant differences in detail band <span class="hlt">structure</span>. In the pressure range from 90 to160 GPa, semi-<span class="hlt">local</span>, hybrid functional and TB-mBJLDA calculations predicted that AlH3 is a poor metal. In comparison, GW calculations show a gap opening at 160 GPa and AlH3 becomes a small gap semi-conductor. From the trends of the calculated band shifts, it can be concluded that the favourable conditions leading to the nesting of Fermi surfaces predicted by semi-<span class="hlt">local</span> calculation have disappeared if the exchange term is included. The results highlight the importance of the correction to the exchange energy on the band <span class="hlt">structure</span> of hydrogen dominant dense metal hydrides at high pressure hydrides and may help to rationalize the absence of superconductivity in AlH3 from experimental measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012APS..MAR.J1009P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012APS..MAR.J1009P"><span><span class="hlt">Local</span> 2D-2D tunneling in high mobility <span class="hlt">electron</span> systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pelliccione, Matthew; Sciambi, Adam; Bartel, John; Goldhaber-Gordon, David; Pfeiffer, Loren; West, Ken; Lilly, Michael; Bank, Seth; Gossard, Arthur</p> <p>2012-02-01</p> <p>Many scanning probe techniques have been utilized in recent years to measure <span class="hlt">local</span> properties of high mobility two-dimensional (2D) <span class="hlt">electron</span> systems in GaAs. However, most techniques lack the ability to tunnel into the buried 2D system and measure <span class="hlt">local</span> spectroscopic information. We report scanning gate measurements on a bilayer GaAs/AlGaAs heterostructure that allows for a <span class="hlt">local</span> modulation of tunneling between two 2D <span class="hlt">electron</span> layers. We call this technique Virtual Scanning Tunneling Microscopy (VSTM) [1,2] as the influence of the scanning gate is analogous to an STM tip, except at a GaAs/AlGaAs interface instead of a surface. We will discuss the spectroscopic capabilities of the technique, and show preliminary results of measurements on a high mobility 2D <span class="hlt">electron</span> system.[1] A. Sciambi, M. Pelliccione et al., Appl. Phys. Lett. 97, 132103 (2010).[2] A. Sciambi, M. Pelliccione et al., Phys. Rev. B 84, 085301 (2011).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1183094-studying-localized-corrosion-using-liquid-cell-transmission-electron-microscopy','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1183094-studying-localized-corrosion-using-liquid-cell-transmission-electron-microscopy"><span>Studying <span class="hlt">localized</span> corrosion using liquid cell transmission <span class="hlt">electron</span> microscopy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Chee, See Wee; Pratt, Sarah H.; Hattar, Khalid; ...</p> <p>2014-11-07</p> <p>Using liquid cell transmission <span class="hlt">electron</span> microscopy (LCTEM), <span class="hlt">localized</span> corrosion of Cu and Al thin films immersed in aqueous NaCl solutions was studied. We demonstrate that potentiostatic control can be used to initiate pitting and that <span class="hlt">local</span> compositional changes, due to focused ion beam implantation of Au + ions, can modify the corrosion susceptibility of Al films. Likewise, a discussion on strategies to control the onset of pitting is also presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29617017','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29617017"><span>Study of the <span class="hlt">electronic</span> <span class="hlt">structure</span> of <span class="hlt">electron</span> accepting cyano-films: TCNQversusTCNE.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Capitán, Maria J; Álvarez, Jesús; Navio, Cristina</p> <p>2018-04-18</p> <p>In this article, we perform systematic research on the <span class="hlt">electronic</span> <span class="hlt">structure</span> of two closely related organic <span class="hlt">electron</span> acceptor molecules (TCNQ and TCNE), which are of technological interest due to their outstanding <span class="hlt">electronic</span> properties. These studies have been performed from the experimental point of view by the use <span class="hlt">electron</span> spectroscopies (XPS and UPS) and supported theoretically by the use of ab-initio DFT calculations. The cross-check between both molecules allows us to identify the characteristic <span class="hlt">electronic</span> features of each part of the molecules and their contribution to the final <span class="hlt">electronic</span> <span class="hlt">structure</span>. We can describe the nature of the band gap of these materials, and we relate this with the appearance of the shake-up features in the core level spectra. A band bending and energy gap reduction of the aforementioned <span class="hlt">electronic</span> <span class="hlt">structure</span> in contact with a metal surface are seen in the experimental results as well in the theoretical calculations. This behavior implies that the TCNQ thin film accepts <span class="hlt">electrons</span> from the metal substrate becoming a Schottky n-junction.</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.ncbi.nlm.nih.gov/pubmed/27334148','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27334148"><span>Graph-based linear scaling <span class="hlt">electronic</span> <span class="hlt">structure</span> theory.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Niklasson, Anders M N; Mniszewski, Susan M; Negre, Christian F A; Cawkwell, Marc J; Swart, Pieter J; Mohd-Yusof, Jamal; Germann, Timothy C; Wall, Michael E; Bock, Nicolas; Rubensson, Emanuel H; Djidjev, Hristo</p> <p>2016-06-21</p> <p>We show how graph theory can be combined with quantum theory to calculate the <span class="hlt">electronic</span> <span class="hlt">structure</span> of large complex systems. The graph formalism is general and applicable to a broad range of <span class="hlt">electronic</span> <span class="hlt">structure</span> methods and materials, including challenging systems such as biomolecules. The methodology combines well-controlled accuracy, low computational cost, and natural low-communication parallelism. This combination addresses substantial shortcomings of linear scaling <span class="hlt">electronic</span> <span class="hlt">structure</span> theory, in particular with respect to quantum-based molecular dynamics simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22660738-graph-based-linear-scaling-electronic-structure-theory','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22660738-graph-based-linear-scaling-electronic-structure-theory"><span>Graph-based linear scaling <span class="hlt">electronic</span> <span class="hlt">structure</span> theory</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>Niklasson, Anders M. N., E-mail: amn@lanl.gov; Negre, Christian F. A.; Cawkwell, Marc J.</p> <p>2016-06-21</p> <p>We show how graph theory can be combined with quantum theory to calculate the <span class="hlt">electronic</span> <span class="hlt">structure</span> of large complex systems. The graph formalism is general and applicable to a broad range of <span class="hlt">electronic</span> <span class="hlt">structure</span> methods and materials, including challenging systems such as biomolecules. The methodology combines well-controlled accuracy, low computational cost, and natural low-communication parallelism. This combination addresses substantial shortcomings of linear scaling <span class="hlt">electronic</span> <span class="hlt">structure</span> theory, in particular with respect to quantum-based molecular dynamics simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH41B2764B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH41B2764B"><span>Non-<span class="hlt">Local</span> Diffusion of Energetic <span class="hlt">Electrons</span> during Solar Flares</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bian, N. H.; Emslie, G.; Kontar, E.</p> <p>2017-12-01</p> <p>The transport of the energy contained in suprathermal <span class="hlt">electrons</span> in solar flares plays a key role in our understanding of many aspects of flare physics, from the spatial distributions of hard X-ray emission and energy deposition in the ambient atmosphere to global energetics. Historically the transport of these particles has been largely treated through a deterministic approach, in which first-order secular energy loss to <span class="hlt">electrons</span> in the ambient target is treated as the dominant effect, with second-order diffusive terms (in both energy and angle) generally being either treated as a small correction or even neglected. Here, we critically analyze this approach, and we show that spatial diffusion through pitch-angle scattering necessarily plays a very significant role in the transport of <span class="hlt">electrons</span>. We further show that a satisfactory treatment of the diffusion process requires consideration of non-<span class="hlt">local</span> effects, so that the <span class="hlt">electron</span> flux depends not just on the <span class="hlt">local</span> gradient of the <span class="hlt">electron</span> distribution function but on the value of this gradient within an extended region encompassing a significant fraction of a mean free path. Our analysis applies generally to pitch-angle scattering by a variety of mechanisms, from Coulomb collisions to turbulent scattering. We further show that the spatial transport of <span class="hlt">electrons</span> along the magnetic field of a flaring loop can be modeled as a Continuous Time Random Walk with velocity-dependent probability distribution functions of jump sizes and occurrences, both of which can be expressed in terms of the scattering mean free path.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/603471','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/603471"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of barium strontium titanate by soft-x-ray absorption spectroscopy</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>Uehara, Y.; Underwood, J.H.; Gullikson, E.M.</p> <p>1997-04-01</p> <p>Perovskite-type titanates, such as Strontium Titanate (STO), Barium Titanate (BTO), and Lead Titanate (PTO) have been widely studied because they show good electric and optical properties. In recent years, thin films of Barium Strontium Titanate (BST) have been paid much attention as dielectrics of dynamic random access memory (DRAM) capacitors. BST is a better insulator with a higher dielectric constant than STO and can be controlled in a paraelectric phase with an appropriate ratio of Ba/Sr composition, however, few studies have been done on the <span class="hlt">electronic</span> <span class="hlt">structure</span> of the material. Studies of the <span class="hlt">electronic</span> <span class="hlt">structure</span> of such materials can bemore » beneficial, both for fundamental physics research and for improving technological applications. BTO is a famous ferroelectric material with a tetragonal <span class="hlt">structure</span>, in which Ti and Ba atoms are slightly displaced from the lattice points. On the other hand, BST keeps a paraelectric phase, which means that the atoms are still at the cubic lattice points. It should be of great interest to see how this difference of the <span class="hlt">local</span> <span class="hlt">structure</span> around Ti atoms between BTO and BST effects the <span class="hlt">electronic</span> <span class="hlt">structure</span> of these two materials. In this report, the authors present the Ti L{sub 2,3} absorption spectra of STO, BTO, and BST measured with very high accuracy in energy of the absorption features.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1409191','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1409191"><span>Study of rare earth <span class="hlt">local</span> moment magnetism and strongly correlated phenomena in various crystal <span class="hlt">structures</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>Kong, Tai</p> <p></p> <p>Benefiting from unique properties of 4f <span class="hlt">electrons</span>, rare earth based compounds are known for offering a versatile playground for condensed matter physics research as well as industrial applications. This thesis focuses on three specific examples that further explore the rare earth <span class="hlt">local</span> moment magnetism and strongly correlated phenomena in various crystal <span class="hlt">structures</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhRvB..92j0101L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhRvB..92j0101L"><span><span class="hlt">Local</span> atomic and <span class="hlt">electronic</span> <span class="hlt">structures</span> in ferromagnetic topological insulator Cr-doped (BixSb1-x) 2Te3 studied by XAFS and ab initio calculations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Zhen; Wei, Xinyuan; Wang, Jiajia; Pan, Hong; Ji, Fuhao; Ye, Mao; Yang, Zhongqin; Qiao, Shan</p> <p>2015-09-01</p> <p>The <span class="hlt">local</span> atomic and <span class="hlt">electronic</span> <span class="hlt">structures</span> around the dopants in Cr-doped (BixSb1 -x )2Te3 are studied by x-ray absorption fine <span class="hlt">structure</span> (XAFS) measurements and first-principles calculations. Both Cr and Bi are confirmed substituting Sb sites (CrSb and BiSb). The six nearest Te atoms around Cr move towards Cr and shorten the Cr-Te bond lengths to 2.76 Å and 2.77 Å for x =0.1 and x =0.2 , respectively. Importantly, we reveal the hybridization between the Sb/Te p states and Cr d states by the presence of a pre-edge peak at Cr K -absorption edge, which is also supported by our ab initio calculations. These findings provide important clues to understand the mechanism of ferromagnetic order in this system with quantum anomalous Hall effect.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24002904','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24002904"><span>Geometry motivated alternative view on <span class="hlt">local</span> protein backbone <span class="hlt">structures</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zacharias, Jan; Knapp, Ernst Walter</p> <p>2013-11-01</p> <p>We present an alternative to the classical Ramachandran plot (R-plot) to display <span class="hlt">local</span> protein backbone <span class="hlt">structure</span>. Instead of the (φ, ψ)-backbone angles relating to the chemical architecture of polypeptides generic helical parameters are used. These are the rotation or twist angle ϑ and the helical rise parameter d. Plots with these parameters provide a different view on the nature of <span class="hlt">local</span> protein backbone <span class="hlt">structures</span>. It allows to display the <span class="hlt">local</span> <span class="hlt">structures</span> in polar (d, ϑ)-coordinates, which is not possible for an R-plot, where <span class="hlt">structural</span> regimes connected by periodicity appear disconnected. But there are other advantages, like a clear discrimination of the handedness of a <span class="hlt">local</span> <span class="hlt">structure</span>, a larger spread of the different <span class="hlt">local</span> <span class="hlt">structure</span> domains--the latter can yield a better separation of different <span class="hlt">local</span> secondary <span class="hlt">structure</span> motives--and many more. Compared to the R-plot we are not aware of any major disadvantage to classify <span class="hlt">local</span> polypeptide <span class="hlt">structures</span> with the (d, ϑ)-plot, except that it requires some elementary computations. To facilitate usage of the new (d, ϑ)-plot for protein <span class="hlt">structures</span> we provide a web application (http://agknapp.chemie.fu-berlin.de/secsass), which shows the (d, ϑ)-plot side-by-side with the R-plot. © 2013 The Protein Society.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JChPh.137s4112K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JChPh.137s4112K"><span><span class="hlt">Electronic</span> energy transfer: <span class="hlt">Localized</span> operator partitioning of <span class="hlt">electronic</span> energy in composite quantum systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Khan, Yaser; Brumer, Paul</p> <p>2012-11-01</p> <p>A Hamiltonian based approach using spatially <span class="hlt">localized</span> projection operators is introduced to give precise meaning to the chemically intuitive idea of the <span class="hlt">electronic</span> energy on a quantum subsystem. This definition facilitates the study of <span class="hlt">electronic</span> energy transfer in arbitrarily coupled quantum systems. In particular, the decomposition scheme can be applied to molecular components that are strongly interacting (with significant orbital overlap) as well as to isolated fragments. The result defines a consistent <span class="hlt">electronic</span> energy at all internuclear distances, including the case of separated fragments, and reduces to the well-known Förster and Dexter results in their respective limits. Numerical calculations of coherent energy and charge transfer dynamics in simple model systems are presented and the effect of collisionally induced decoherence is examined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1988suco.conf.....F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1988suco.conf.....F"><span>Probing the <span class="hlt">electronic</span> and defect <span class="hlt">structure</span> of perovskite superconductors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fluss, M. J.; Wachs, A. L.; Turchi, P. E. A.; Howell, R. H.; Jean, Y. C.; Kyle, J.; Nakanishi, H.; Chu, C. W.; Meng, R. L.; Hor, H. P.</p> <p>1988-02-01</p> <p>Positrons, either <span class="hlt">localized</span> or delocalized, in the perovskite superconductors are sensitive to changes in <span class="hlt">electron</span> density accompanying the normal-to-superconducting transition. We have been using this probe in our laboratory to study the nature of this new phenomena. Our work to date, which is briefly reviewed here, has consisted of a series of lifetime studies on La(sub 1.85)Sr(sub 0.15)CuO4 and YBa2Cu3O(sub 7-d) superconducting samples, the determination of the positron wave function in the perfect crystal, and a direct measurement of the <span class="hlt">electron</span> momentum density in single crystal La2CuO4. Several important observations have resulted from this early work: the similar response of the positron annihilation lifetime to superconductivity in both La(sub 1.85)Sr(sub 0.15)CuO4 and YBa2Cu3O7, and a quantitative description of the <span class="hlt">electronic</span> <span class="hlt">structure</span> for La(sub 1.85)Sr(sub 0.15)CuO4 in terms of a linear combination of atomic orbital-molecular orbital (LCAO-MO) model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JChPh.134t5102B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JChPh.134t5102B"><span>Combined effects of metal complexation and size expansion in the <span class="hlt">electronic</span> <span class="hlt">structure</span> of DNA base pairs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brancolini, Giorgia; Di Felice, Rosa</p> <p>2011-05-01</p> <p>Novel DNA derivatives have been recently investigated in the pursuit of modified DNA duplexes to tune the <span class="hlt">electronic</span> <span class="hlt">structure</span> of DNA-based assemblies for nanotechnology applications. Size-expanded DNAs (e.g., xDNA) and metalated DNAs (M-DNA) may enhance stacking interactions and induce metallic conductivity, respectively. Here we explore possible ways of tailoring the DNA <span class="hlt">electronic</span> <span class="hlt">structure</span> by combining the aromatic size expansion with the metal-doping. We select the salient <span class="hlt">structures</span> from our recent study on natural DNA pairs complexed with transition metal ions and consider the equivalent model configurations for xDNA pairs. We present the results of density functional theory <span class="hlt">electronic</span> <span class="hlt">structure</span> calculations of the metalated expanded base-pairs with various <span class="hlt">localized</span> basis sets and exchange-correlation functionals. Implicit solvent and coordination water molecules are also included. Our results indicate that the effect of base expansion is largest in Ag-xGC complexes, while Cu-xGC complexes are the most promising candidates for nanowires with enhanced <span class="hlt">electron</span> transfer and also for on-purpose modification of the DNA double-helix for signal detection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1991ssdm.conf.1322W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1991ssdm.conf.1322W"><span>Embedded <span class="hlt">electronics</span> for intelligent <span class="hlt">structures</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Warkentin, David J.; Crawley, Edward F.</p> <p></p> <p>The signal, power, and communications provisions for the distributed control processing, sensing, and actuation of an intelligent <span class="hlt">structure</span> could benefit from a method of physically embedding some <span class="hlt">electronic</span> components. The preliminary feasibility of embedding <span class="hlt">electronic</span> components in load-bearing intelligent composite <span class="hlt">structures</span> is addressed. A technique for embedding integrated circuits on silicon chips within graphite/epoxy composite <span class="hlt">structures</span> is presented which addresses the problems of electrical, mechanical, and chemical isolation. The mechanical and chemical isolation of test articles manufactured by this technique are tested by subjecting them to static and cyclic mechanical loads and a temperature/humidity/bias environment. The likely failure modes under these conditions are identified, and suggestions for further improvements in the technique are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26912363','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26912363"><span>Negative <span class="hlt">local</span> resistance caused by viscous <span class="hlt">electron</span> backflow in graphene.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bandurin, D A; Torre, I; Krishna Kumar, R; Ben Shalom, M; Tomadin, A; Principi, A; Auton, G H; Khestanova, E; Novoselov, K S; Grigorieva, I V; Ponomarenko, L A; Geim, A K; Polini, M</p> <p>2016-03-04</p> <p>Graphene hosts a unique <span class="hlt">electron</span> system in which <span class="hlt">electron</span>-phonon scattering is extremely weak but <span class="hlt">electron-electron</span> collisions are sufficiently frequent to provide <span class="hlt">local</span> equilibrium above the temperature of liquid nitrogen. Under these conditions, <span class="hlt">electrons</span> can behave as a viscous liquid and exhibit hydrodynamic phenomena similar to classical liquids. Here we report strong evidence for this transport regime. We found that doped graphene exhibits an anomalous (negative) voltage drop near current-injection contacts, which is attributed to the formation of submicrometer-size whirlpools in the <span class="hlt">electron</span> flow. The viscosity of graphene's <span class="hlt">electron</span> liquid is found to be ~0.1 square meters per second, an order of magnitude higher than that of honey, in agreement with many-body theory. Our work demonstrates the possibility of studying <span class="hlt">electron</span> hydrodynamics using high-quality graphene. Copyright © 2016, American Association for the Advancement of Science.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16120979','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16120979"><span><span class="hlt">Structural</span> changes induced by lattice-<span class="hlt">electron</span> interactions: SiO2 stishovite and FeTiO3 ilmenite.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yamanaka, Takamitsu</p> <p>2005-09-01</p> <p>The bright source and highly collimated beam of synchrotron radiation offers many advantages for single-crystal <span class="hlt">structure</span> analysis under non-ambient conditions. The <span class="hlt">structure</span> changes induced by the lattice-<span class="hlt">electron</span> interaction under high pressure have been investigated using a diamond anvil pressure cell. The pressure dependence of <span class="hlt">electron</span> density distributions around atoms is elucidated by a single-crystal diffraction study using deformation <span class="hlt">electron</span> density analysis and the maximum entropy method. In order to understand the bonding <span class="hlt">electrons</span> under pressure, diffraction intensity measurements of FeTiO3 ilmenite and gamma-SiO2 stishovite single crystals at high pressures were made using synchrotron radiation. Both diffraction studies describe the <span class="hlt">electron</span> density distribution including bonding <span class="hlt">electrons</span> and provide the effective charge of the cations. In both cases the valence <span class="hlt">electrons</span> are more <span class="hlt">localized</span> around the cations with increasing pressure. This is consistent with molecular orbital calculations, proving that the bonding <span class="hlt">electron</span> density becomes smaller with pressure. The thermal displacement parameters of both samples are reduced with increasing pressure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009A%26A...508..993B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009A%26A...508..993B"><span><span class="hlt">Local</span> re-acceleration and a modified thick target model of solar flare <span class="hlt">electrons</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brown, J. C.; Turkmani, R.; Kontar, E. P.; MacKinnon, A. L.; Vlahos, L.</p> <p>2009-12-01</p> <p>Context: The collisional thick target model (CTTM) of solar hard X-ray (HXR) bursts has become an almost “standard model” of flare impulsive phase energy transport and radiation. However, it faces various problems in the light of recent data, particularly the high <span class="hlt">electron</span> beam density and anisotropy it involves. Aims: We consider how photon yield per <span class="hlt">electron</span> can be increased, and hence fast <span class="hlt">electron</span> beam intensity requirements reduced, by <span class="hlt">local</span> re-acceleration of fast <span class="hlt">electrons</span> throughout the HXR source itself, after injection. Methods: We show parametrically that, if net re-acceleration rates due to e.g. waves or <span class="hlt">local</span> current sheet electric (E) fields are a significant fraction of collisional loss rates, <span class="hlt">electron</span> lifetimes, and hence the net radiative HXR output per <span class="hlt">electron</span> can be substantially increased over the CTTM values. In this <span class="hlt">local</span> re-acceleration thick target model (LRTTM) fast <span class="hlt">electron</span> number requirements and anisotropy are thus reduced. One specific possible scenario involving such re-acceleration is discussed, viz, a current sheet cascade (CSC) in a randomly stressed magnetic loop. Results: Combined MHD and test particle simulations show that <span class="hlt">local</span> E fields in CSCs can efficiently accelerate <span class="hlt">electrons</span> in the corona and and re-accelerate them after injection into the chromosphere. In this HXR source scenario, rapid synchronisation and variability of impulsive footpoint emissions can still occur since primary <span class="hlt">electron</span> acceleration is in the high Alfvén speed corona with fast re-acceleration in chromospheric CSCs. It is also consistent with the energy-dependent time-of-flight delays in HXR features. Conclusions: Including <span class="hlt">electron</span> re-acceleration in the HXR source allows an LRTTM modification of the CTTM in which beam density and anisotropy are much reduced, and alleviates theoretical problems with the CTTM, while making it more compatible with radio and interplanetary <span class="hlt">electron</span> numbers. The LRTTM is, however, different in some respects such as</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25481158','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25481158"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> and aromaticity of large-scale hexagonal graphene nanoflakes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hu, Wei; Lin, Lin; Yang, Chao; Yang, Jinlong</p> <p>2014-12-07</p> <p>With the help of the recently developed SIESTA-pole (Spanish Initiative for <span class="hlt">Electronic</span> Simulations with Thousands of Atoms) - PEXSI (pole expansion and selected inversion) method [L. Lin, A. García, G. Huhs, and C. Yang, J. Phys.: Condens. Matter 26, 305503 (2014)], we perform Kohn-Sham density functional theory calculations to study the stability and <span class="hlt">electronic</span> <span class="hlt">structure</span> of hydrogen passivated hexagonal graphene nanoflakes (GNFs) with up to 11,700 atoms. We find the <span class="hlt">electronic</span> properties of GNFs, including their cohesive energy, edge formation energy, highest occupied molecular orbital-lowest unoccupied molecular orbital energy gap, edge states, and aromaticity, depend sensitively on the type of edges (armchair graphene nanoflakes (ACGNFs) and zigzag graphene nanoflakes (ZZGNFs)), size and the number of <span class="hlt">electrons</span>. We observe that, due to the edge-induced strain effect in ACGNFs, large-scale ACGNFs' edge formation energy decreases as their size increases. This trend does not hold for ZZGNFs due to the presence of many edge states in ZZGNFs. We find that the energy gaps E(g) of GNFs all decay with respect to 1/L, where L is the size of the GNF, in a linear fashion. But as their size increases, ZZGNFs exhibit more <span class="hlt">localized</span> edge states. We believe the presence of these states makes their gap decrease more rapidly. In particular, when L is larger than 6.40 nm, we find that ZZGNFs exhibit metallic characteristics. Furthermore, we find that the aromatic <span class="hlt">structures</span> of GNFs appear to depend only on whether the system has 4N or 4N + 2 <span class="hlt">electrons</span>, where N is an integer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22658104-structural-electronic-magnetic-properties-carbon-doped-boron-nitride-nanowire-ab-initio-study','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22658104-structural-electronic-magnetic-properties-carbon-doped-boron-nitride-nanowire-ab-initio-study"><span><span class="hlt">Structural</span>, <span class="hlt">electronic</span> and magnetic properties of carbon doped boron nitride nanowire: Ab initio study</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>Jalilian, Jaafar, E-mail: JaafarJalilian@gmail.com; Kanjouri, Faramarz, E-mail: kanjouri@khu.ac.ir</p> <p>2016-11-15</p> <p>Using spin-polarized density functional theory calculations, we demonstrated that carbon doped boron nitride nanowire (C-doped BNNW) has diverse <span class="hlt">electronic</span> and magnetic properties depending on position of carbon atoms and their percentages. Our results show that only when one carbon atom is situated on the edge of the nanowire, C-doped BNNW is transformed into half-metal. The calculated <span class="hlt">electronic</span> <span class="hlt">structure</span> of the C-doped BNNW suggests that doping carbon can induce <span class="hlt">localized</span> edge states around the Fermi level, and the interaction among <span class="hlt">localized</span> edge states leads to semiconductor to half-metal transition. Overall, the bond reconstruction causes of appearance of different <span class="hlt">electronic</span> behavior suchmore » as semiconducting, half-metallicity, nonmagnetic metallic, and ferromagnetic metallic characters. The formation energy of the system shows that when a C atom is doped on surface boron site, system is more stable than the other positions of carbon impurity. Our calculations show that C-doped BNNW may offer unique opportunities for developing nanoscale spintronic materials.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvM...2a5002R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvM...2a5002R"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of negative charge transfer CaFeO3 across the metal-insulator transition</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rogge, Paul C.; Chandrasena, Ravini U.; Cammarata, Antonio; Green, Robert J.; Shafer, Padraic; Lefler, Benjamin M.; Huon, Amanda; Arab, Arian; Arenholz, Elke; Lee, Ho Nyung; Lee, Tien-Lin; Nemšák, Slavomír; Rondinelli, James M.; Gray, Alexander X.; May, Steven J.</p> <p>2018-01-01</p> <p>We investigated the metal-insulator transition for epitaxial thin films of the perovskite CaFeO3, a material with a significant oxygen ligand hole contribution to its <span class="hlt">electronic</span> <span class="hlt">structure</span>. We find that biaxial tensile and compressive strain suppress the metal-insulator transition temperature. By combining hard x-ray photoelectron spectroscopy, soft x-ray absorption spectroscopy, and density functional calculations, we resolve the element-specific changes to the <span class="hlt">electronic</span> <span class="hlt">structure</span> across the metal-insulator transition. We demonstrate that the Fe sites undergo no observable spectroscopic change between the metallic and insulating states, whereas the O <span class="hlt">electronic</span> configuration undergoes significant changes. This strongly supports the bond-disproportionation model of the metal-insulator transition for CaFeO3 and highlights the importance of ligand holes in its <span class="hlt">electronic</span> <span class="hlt">structure</span>. By sensitively measuring the ligand hole density, however, we find that it increases by ˜5 -10 % in the insulating state, which we ascribe to a further <span class="hlt">localization</span> of <span class="hlt">electron</span> charge on the Fe sites. These results provide detailed insight into the metal-insulator transition of negative charge transfer compounds and should prove instructive for understanding metal-insulator transitions in other late transition metal compounds such as the nickelates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS.953a2160P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS.953a2160P"><span>Intranet and village community: optimization of public service based on <span class="hlt">electronic</span> government at the <span class="hlt">local</span> level</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pradana, G. W.; Fanida, E. H.; Niswah, F.</p> <p>2018-01-01</p> <p>The demand for good governance is directed towards the realization of efficiency, effectiveness, and clean government. The move is demonstrated through national and regional levels to develop and implement <span class="hlt">electronic</span> government concepts. Through the development of <span class="hlt">electronic</span> government is done <span class="hlt">structuring</span> management systems and work processes in the government environment by optimizing the utilization of information technology. One of the real forms of <span class="hlt">electronic</span> government (e-Gov) implementation at the <span class="hlt">local</span> level is the Intranet Sub-District program in Sukodono Sub-District, Sidoarjo. Intranet Sub-District is an innovation whose purpose is to realize the availability of information on the utilization of management, distribution, and storage of official scripts, and also the optimal delivery of information and communication in the implementation of guidance and supervision of <span class="hlt">local</span> administration. The type of this paper is descriptive with a qualitative approach and focus on the implementation of the Intranet District Program in Sukodono District, Sidoarjo. The findings of the study are the limited number of human resources who have mastered ICT, the uneven network, the adequacy of institutional needs and the existence of budget support from the authorized institution and the information system has not accommodated all the service needs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26726677','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26726677"><span><span class="hlt">Local</span> <span class="hlt">Structure</span> Determination of Carbon/Nickel Ferrite Composite Nanofibers Probed by X-ray 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>Nilmoung, Sukunya; Kidkhunthod, Pinit; Maensiri, Santi</p> <p>2015-11-01</p> <p>Carbon/NiFe2O4 composite nanofibers have been successfully prepared by electrospinning method using a various concentration solution of Ni and Fe nitrates dispersed into polyacrylonitride (PAN) solution in N,N' dimethylformamide. The phase and mophology of PAN/NiFe2O4 composite samples were characterized and investigated by X-ray diffraction and scanning <span class="hlt">electron</span> microscopy. The magnetic properties of the prepared samples were measured at ambient temperature by a vibrating sample magnetometer. It is found that all composite samples exhibit ferromagnetism. This could be <span class="hlt">local-structurally</span> explained by the existed oxidation states of Ni2+ and Fe3+ in the samples. Moreover, <span class="hlt">local</span> environments around Ni and Fe ions could be revealed by X-ray absorption spectroscopy (XAS) measurement including X-ray absorption near edge <span class="hlt">structure</span> (XANES) and Extended X-ray absorption fine <span class="hlt">structure</span> (EXAFS).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24081041','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24081041"><span>Femtosecond laser-induced periodic <span class="hlt">structure</span> adjustments based on <span class="hlt">electron</span> dynamics control: from subwavelength ripples to double-grating <span class="hlt">structures</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shi, Xuesong; Jiang, Lan; Li, Xin; Wang, Sumei; Yuan, Yanping; Lu, Yongfeng</p> <p>2013-10-01</p> <p>This study proposes a method for adjusting subwavelength ripple periods and the corresponding double-grating <span class="hlt">structures</span> formed on fused silica by designing femtosecond laser pulse trains based on <span class="hlt">localized</span> transient <span class="hlt">electron</span> density control. Four near-constant period ranges of 190-490 nm of ripples perpendicular to the polarization are obtained by designing pulse trains to excite and modulate the surface plasmon waves. In the period range of 350-490 nm, the double-grating <span class="hlt">structure</span> is fabricated in one step, which is probably attributable to the grating-assisted enhanced energy deposition and subsequent thermal effects.</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('http://adsabs.harvard.edu/abs/2018IJMPB..3250060K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018IJMPB..3250060K"><span>InN/GaN quantum dot superlattices: Charge-carrier states and surface <span class="hlt">electronic</span> <span class="hlt">structure</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kanouni, F.; Brezini, A.; Djenane, M.; Zou, Q.</p> <p>2018-03-01</p> <p>We have theoretically investigated the <span class="hlt">electron</span> energy spectra and surface states energy in the three dimensionally ordered quantum dot superlattices (QDSLs) made of InN and GaN semiconductors. The QDSL is assumed in this model to be a matrix of GaN containing cubic dots of InN of the same size and uniformly distributed. For the miniband’s <span class="hlt">structure</span> calculation, the resolution of the effective mass Schrödinger equation is done by decoupling it in the three directions within the framework of Kronig-Penney model. We found that the <span class="hlt">electrons</span> minibands in infinite ODSLs are clearly different from those in the conventional quantum-well superlattices. The <span class="hlt">electrons</span> <span class="hlt">localization</span> and charge-carrier states are very dependent on the quasicrystallographic directions, the size and the shape of the dots which play a role of the artificial atoms in such QD supracrystal. The energy spectrum of the <span class="hlt">electron</span> states <span class="hlt">localized</span> at the surface of InN/GaN QDSL is represented by Kronig-Penney like-model, calculated via direct matching procedure. The calculation results show that the substrate breaks symmetrical shape of QDSL on which some <span class="hlt">localized</span> <span class="hlt">electronic</span> surface states can be produced in minigap regions. Furthermore, we have noticed that the surface states degeneracy is achieved in like very thin bands located in the minigaps, identified by different quantum numbers nx, ny, nz. Moreover, the surface energy bands split due to the reduction of the symmetry of the QDSL in z-direction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhDT.......278D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhDT.......278D"><span><span class="hlt">Local</span> <span class="hlt">structure</span> and <span class="hlt">structural</span> signature underlying properties in metallic glasses and supercooled liquids</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ding, Jun</p> <p></p> <p>Metallic glasses (MGs), discovered five decades ago as a newcomer in the family of glasses, are of current interest because of their unique <span class="hlt">structures</span> and properties. There are also many fundamental materials science issues that remain unresolved for metallic glasses, as well as their predecessor above glass transition temperature, the supercooled liquids. In particular, it is a major challenge to characterize the <span class="hlt">local</span> <span class="hlt">structure</span> and unveil the <span class="hlt">structure</span>-property relationship for these amorphous materials. This thesis presents a systematic study of the <span class="hlt">local</span> <span class="hlt">structure</span> of metallic glasses as well as supercooled liquids via classical and ab initio molecular dynamics simulations. Three typical MG models are chosen as representative candidate, Cu64 Zr36, Pd82Si18 and Mg65Cu 25Y10 systems, while the former is dominant with full icosahedra short-range order and the prism-type short-range order dominate for latter two. Furthermore, we move to unravel the underlying <span class="hlt">structural</span> signature among several properties in metallic glasses. Firstly, the temperature dependence of specific heat and liquid fragility between Cu-Zr and Mg-Cu-Y (also Pd-Si) in supercooled liquids are quite distinct: gradual versus fast evolution of specific heat and viscosity/relaxation time with undercooling. Their <span class="hlt">local</span> <span class="hlt">structural</span> ordering are found to relate with the temperature dependence of specific heat and relaxation time. Then elastic heterogeneity has been studied to correlate with <span class="hlt">local</span> <span class="hlt">structure</span> in Cu-Zr MGs. Specifically, this part covers how the degree of elastic deformation correlates with the internal <span class="hlt">structure</span> at the atomic level, how to quantitatively evaluate the <span class="hlt">local</span> solidity/liquidity in MGs and how the network of interpenetrating connection of icosahedra determine the corresponding shear modulus. Finally, we have illustrated the <span class="hlt">structure</span> signature of quasi-<span class="hlt">localized</span> low-frequency vibrational normal modes, which resides the intriguing vibrational properties in MGs. Specifically, the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1025333','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1025333"><span>Final report: ES11: The 23rd Annual Workshop on <span class="hlt">Electronic</span> <span class="hlt">Structure</span> Methods</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>Rappe, Andrew M.</p> <p>2011-08-31</p> <p>ES11: the 23rd Annual Workshop on <span class="hlt">Electronic</span> <span class="hlt">Structure</span> Methods was held from June 6-9, 2011 at the University of Pennsylvania. The <span class="hlt">local</span> organizing committee (see Section II) led by PI Andrew M. Rappe supervised the organization of the conference, before, during, and after the meeting itself. The national organizing committee set the technical program of talks, and provided support and advice in various ways. The conference was well-attended (see Section III). An important feature of this conference was a series of panel discussions (see Section IV) to discuss the field of <span class="hlt">electronic</span> <span class="hlt">structure</span> and to set new directions. The technicalmore » program was of extraordinarily high quality (see Section V). The host institution, the University of Pennsylvania, provided a supportive environment for this meeting (see Section VI).« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Nanos...714946K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Nanos...714946K"><span>Dynamic modulation of <span class="hlt">electronic</span> properties of graphene by <span class="hlt">localized</span> carbon doping using focused <span class="hlt">electron</span> beam induced deposition</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, S.; Russell, M.; Henry, M.; Kim, S. S.; Naik, R. R.; Voevodin, A. A.; Jang, S. S.; Tsukruk, V. V.; Fedorov, A. G.</p> <p>2015-09-01</p> <p>We report on the first demonstration of controllable carbon doping of graphene to engineer <span class="hlt">local</span> <span class="hlt">electronic</span> properties of a graphene conduction channel using focused <span class="hlt">electron</span> beam induced deposition (FEBID). Electrical measurements indicate that an ``n-p-n'' junction on graphene conduction channel is formed by partial carbon deposition near the source and drain metal contacts by low energy (<50 eV) secondary <span class="hlt">electrons</span> due to inelastic collisions of long range backscattered primary <span class="hlt">electrons</span> generated from a low dose of high energy (25 keV) <span class="hlt">electron</span> beam (1 × 1018 e- per cm2). Detailed AFM imaging provides direct evidence of the new mechanism responsible for dynamic evolution of the <span class="hlt">locally</span> varying graphene doping. The FEBID carbon atoms, which are physisorbed and weakly bound to graphene, diffuse towards the middle of graphene conduction channel due to their surface chemical potential gradient, resulting in negative shift of Dirac voltage. Increasing a primary <span class="hlt">electron</span> dose to 1 × 1019 e- per cm2 results in a significant increase of carbon deposition, such that it covers the entire graphene conduction channel at high surface density, leading to n-doping of graphene channel. Collectively, these findings establish a unique capability of FEBID technique to dynamically modulate the doping state of graphene, thus enabling a new route to resist-free, ``direct-write'' functional patterning of graphene-based <span class="hlt">electronic</span> devices with potential for on-demand re-configurability.We report on the first demonstration of controllable carbon doping of graphene to engineer <span class="hlt">local</span> <span class="hlt">electronic</span> properties of a graphene conduction channel using focused <span class="hlt">electron</span> beam induced deposition (FEBID). Electrical measurements indicate that an ``n-p-n'' junction on graphene conduction channel is formed by partial carbon deposition near the source and drain metal contacts by low energy (<50 eV) secondary <span class="hlt">electrons</span> due to inelastic collisions of long range backscattered primary <span class="hlt">electrons</span> generated</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005PhRvB..72q4104M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005PhRvB..72q4104M"><span><span class="hlt">Local</span> <span class="hlt">structure</span> in LaMnO3 and CaMnO3 perovskites: A quantitative <span class="hlt">structural</span> refinement of Mn K -edge XANES data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Monesi, C.; Meneghini, C.; Bardelli, F.; Benfatto, M.; Mobilio, S.; Manju, U.; Sarma, D. D.</p> <p>2005-11-01</p> <p>Hole-doped perovskites such as La1-xCaxMnO3 present special magnetic and magnetotransport properties, and it is commonly accepted that the <span class="hlt">local</span> atomic <span class="hlt">structure</span> around Mn ions plays a crucial role in determining these peculiar features. Therefore experimental techniques directly probing the <span class="hlt">local</span> atomic <span class="hlt">structure</span>, like x-ray absorption spectroscopy (XAS), have been widely exploited to deeply understand the physics of these compounds. Quantitative XAS analysis usually concerns the extended region [extended x-ray absorption fine <span class="hlt">structure</span> (EXAFS)] of the absorption spectra. The near-edge region [x-ray absorption near-edge spectroscopy (XANES)] of XAS spectra can provide detailed complementary information on the <span class="hlt">electronic</span> <span class="hlt">structure</span> and <span class="hlt">local</span> atomic topology around the absorber. However, the complexity of the XANES analysis usually prevents a quantitative understanding of the data. This work exploits the recently developed MXAN code to achieve a quantitative <span class="hlt">structural</span> refinement of the Mn K -edge XANES of LaMnO3 and CaMnO3 compounds; they are the end compounds of the doped manganite series LaxCa1-xMnO3 . The results derived from the EXAFS and XANES analyses are in good agreement, demonstrating that a quantitative picture of the <span class="hlt">local</span> <span class="hlt">structure</span> can be obtained from XANES in these crystalline compounds. Moreover, the quantitative XANES analysis provides topological information not directly achievable from EXAFS data analysis. This work demonstrates that combining the analysis of extended and near-edge regions of Mn K -edge XAS spectra could provide a complete and accurate description of Mn <span class="hlt">local</span> atomic environment in these compounds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22597888-size-effects-structural-electronic-optical-properties-finite-length-carbon-nanotube-ab-initio-electronic-structure-study','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22597888-size-effects-structural-electronic-optical-properties-finite-length-carbon-nanotube-ab-initio-electronic-structure-study"><span>Size effects on the <span class="hlt">structural</span>, <span class="hlt">electronic</span>, and optical properties of (5,0) finite-length carbon nanotube: An ab-initio <span class="hlt">electronic</span> <span class="hlt">structure</span> study</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>Tarighi Ahmadpour, Mahdi; Rostamnejadi, Ali; Hashemifar, S. Javad</p> <p>2016-07-07</p> <p>We use density functional computations to study the zero temperature <span class="hlt">structural</span>, <span class="hlt">electronic</span>, magnetic, and optical properties of (5,0) finite carbon nanotubes (FCNT), with length in the range of 4–44 Å. It is found that the <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties of (5,0) FCNTs, in the ground state, converge at a length of about 30 Å, while the excited state properties exhibit long-range edge effects. We discuss that curvature effects enhance energy gap of FCNTs, in contrast to the known trend in the periodic limit. It is seen that compensation of curvature effects in two special small sizes may give rise to spontaneous magnetization.more » The obtained cohesive energies provide some insights into the effects of environment on the growth of FCNTs. The second-order difference of the total energies reveals an important magic size of about 15 Å. The optical and dynamical magnetic responses of the FCNTs to polarized electromagnetic pulses are studied by time dependent density functional theory. The results show that the static and dynamic magnetic properties mainly come from the edge carbon atoms. The optical absorption properties are described in terms of <span class="hlt">local</span> field effects and characterized by Casida linear response method.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/15017432-mapping-electron-localization-function-earth-materials','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/15017432-mapping-electron-localization-function-earth-materials"><span>A Mapping of the <span class="hlt">Electron</span> <span class="hlt">Localization</span> Function for Earth Materials</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>Gibbs, Gerald V.; Cox, David F.; Ross, Nancy</p> <p>2005-06-01</p> <p>The <span class="hlt">electron</span> <span class="hlt">localization</span> function, ELF, generated for a number of geometry-optimized earth materials, provides a graphical representation of the spatial <span class="hlt">localization</span> of the probability <span class="hlt">electron</span> density distribution as embodied in domains ascribed to <span class="hlt">localized</span> bond and lone pair <span class="hlt">electrons</span>. The lone pair domains, displayed by the silica polymorphs quartz, coesite and cristobalite, are typically banana-shaped and oriented perpendicular to the plane of the SiOSi angle at ~0.60 Å from the O atom on the reflex side of the angle. With decreasing angle, the domains increase in magnitude, indicating an increase in the nucleophilic character of the O atom, rendering itmore » more susceptible to potential electrophilic attack. The Laplacian isosurface maps of the experimental and theoretical <span class="hlt">electron</span> density distribution for coesite substantiates the increase in the size of the domain with decreasing angle. Bond pair domains are displayed along each of the SiO bond vectors as discrete concave hemispherically-shaped domains at ~0.70 Å from the O atom. For more closed-shell ionic bonded interactions, the bond and lone pair domains are often coalesced, resulting in concave hemispherical toroidal-shaped domains with <span class="hlt">local</span> maxima centered along the bond vectors. As the shared covalent character of the bonded interactions increases, the bond and lone pair domains are better developed as discrete domains. ELF isosurface maps generated for the earth materials tremolite, diopside, talc and dickite display banana-shaped lone pair domains associated with the bridging O atoms of SiOSi angles and concave hemispherical toroidal bond pair domains associated with the nonbridging ones. The lone pair domains in dickite and talc provide a basis for understanding the bonded interactions between the adjacent neutral layers. Maps were also generated for beryl, cordierite, quartz, low albite, forsterite, wadeite, åkermanite, pectolite, periclase, hurlbutite, thortveitite and vanthoffite</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT.......126D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT.......126D"><span><span class="hlt">Local</span> Magnetism in Strongly Correlated <span class="hlt">Electron</span> Systems with Orbital Degrees of Freedom</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ducatman, Samuel Charles</p> <p></p> <p>The central aim of my research is to explain the connection between the macroscopic behavior and the microscopic physics of strongly correlated <span class="hlt">electron</span> systems with orbital degrees of freedom through the use of effective models. My dissertation focuses on the sub-class of these materials where <span class="hlt">electrons</span> appear to be <span class="hlt">localized</span> by interactions, and magnetic ions have well measured magnetic moments. This suggests that we can capture the low-energy physics of the material by employing a minimal model featuring <span class="hlt">localized</span> spins which interact with each other through exchange couplings. I describe Fe1+y Te and beta-Li2IrO3 with effective models primarily focusing on the spins of the magnetic ions, in this case Fe and Ir, respectively. The goal with both materials is to gain insight and make predictions for experimentalists. In chapter 2, I focus on Fe1+yTe. I describe why we believe the magnetic ground state of this material, with an observed Bragg peak at Q +/- pi/2, pi/2), can be described by a Heisenberg model with 1st, 2nd, and 3rd neighbor interactions. I present two possible ground states of this model in the small J1 limit, the bicollinear and plaquette states. In order to predict which ground state the model prefers, I calculate the spin wave spectrum with 1/S corrections, and I find the model naturally selects the "plaquette state." I give a brief description of the ways this result could be tested using experimental techniques such as polarized neutron scattering. In chapter 3, I extend the model used in chapter 2. This is necessary because the Heisenberg model we employed cannot explain why Fe1+yTe undergoes a phase transition as y is increased. We add an additional elements to our calculation; we assume that <span class="hlt">electrons</span> in some of the Fe 3D orbitals have selectively <span class="hlt">localized</span> while others remain itinerant. We write a new Hamiltonian, where <span class="hlt">localized</span> moments acquire a new long-range RKKY-like interaction from interactions with the itinerant <span class="hlt">electrons</span>. We are</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..MAR.G1308L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..MAR.G1308L"><span>Vacancy effects on the <span class="hlt">electronic</span> and <span class="hlt">structural</span> properties pentacene</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Laraib, Iflah; Janotti, Anderson</p> <p></p> <p>Defects in organic crystals are likely to affect charge transport in organic <span class="hlt">electronic</span> devices. Vacancies can create lattice distortions and modify <span class="hlt">electronic</span> states associated with the molecules in its surrounding. Spectroscopy experiments indicate that molecular vacancies trap charge carriers. Experimental characterization of individual defects is challenging and unambiguous. Here we use density functional calculations including van der Waals interactions in a supercell approach to study the single vacancy in pentacene, a prototype organic semiconductor. We determine formation energies, <span class="hlt">local</span> lattice relaxations, and discuss how vacancies <span class="hlt">locally</span> distort the lattice and affect the <span class="hlt">electronic</span> properties of the host organic semiconductor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997PhyC..282.1283G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997PhyC..282.1283G"><span>Study of photoirradiation for YBa 2Cu 3O 6+ x compounds and the <span class="hlt">electron</span> <span class="hlt">structure</span> by positron experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guosheng, Cheng; Jiaxiang, Shang; Xigui, Li; xianqi, Dai; Xizhong, Wang; Jincang, Zhang</p> <p>1997-08-01</p> <p>We present positron lifetime data of YBa 2Cu 3O 6+ x (x=0.92, 0.43) compounds for different photo-irradiation time. It is given that change of the <span class="hlt">local</span> <span class="hlt">electron</span> density and vacancy concentration with photoirradiation time. It is found that there is transform at the <span class="hlt">electronic</span> <span class="hlt">structure</span> of CuO chains. We also have discussed the effect of photoirradiations time on the <span class="hlt">electronic</span> <span class="hlt">structure</span> of YBa 2Cu 3O 6+ x systems and their charge reservoir layer and CuO 2 plane conduction.layer. The positron experimental results support the model of photoinduced oxygen-diffusion mechanism.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890039491&hterms=electronegativity&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Delectronegativity','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890039491&hterms=electronegativity&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Delectronegativity"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of BaO/W cathode surfaces</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Muller, Wolfgang</p> <p>1989-01-01</p> <p>The <span class="hlt">local</span> <span class="hlt">electronic</span> <span class="hlt">structure</span> of the emissive layer of barium dispenser thermionic cathodes is investigated theoretically using the relativistic scattered-wave approach. The interaction of Ba and O with W, Os, and W-Os alloy surfaces is studied with atomic clusters modeling different absorption environments representative of B- and M-type cathodes. Ba is found to be strongly oxidized, while O and the metal substrate are in a reduced chemical state. The presence of O enhances the surface dipole and Ba binding energy relative to Ba on W. Model results for W-Os alloy substrates show only relatively small changes in Ba and O for identical geometries, but very large charge redistributions inside the substrate, which are attributed to the electronegativity difference between Os and W. If Os is present in the surface layer, the charge transfer from Ba to the substrate and the Ba binding energy increase relative to W. Explanations are offered for the improved <span class="hlt">electron</span> emission from alloy surfaces and the different emission enhancement for different alloy substrates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhRvB..91s5108W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhRvB..91s5108W"><span>Hybrid-exchange density-functional theory study of the <span class="hlt">electronic</span> <span class="hlt">structure</span> of MnV2O4 : Exotic orbital ordering in the cubic <span class="hlt">structure</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, Wei</p> <p>2015-05-01</p> <p>The <span class="hlt">electronic</span> <span class="hlt">structures</span> of cubic and tetragonal MnV2O4 have been studied using hybrid-exchange density-functional theory. The computed <span class="hlt">electronic</span> <span class="hlt">structure</span> of the tetragonal phase shows an antiferro-orbital ordering on V sites and a ferrimagnetic ground state (the spins on V and Mn are antialigned). These results are in good agreement with the previous theoretical result obtained from the <span class="hlt">local</span>-density approximation + U methods [S. Sarkar et al., Phys. Rev. Lett. 102, 216405 (2009), 10.1103/PhysRevLett.102.216405]. Moreover, the <span class="hlt">electronic</span> <span class="hlt">structure</span>, especially the projected density of states of the cubic phase, has been predicted with good agreement with the recent soft x-ray spectroscopy experiment. Similar to the tetragonal phase, the spins on V and Mn in the cubic <span class="hlt">structure</span> favor a ferrimagnetic configuration. Most interesting is that the computed charge densities of the spin-carrying orbitals on V in the cubic phase show an exotic orbital ordering, i.e., a ferro-orbital ordering along [110] but an antiferro-orbital ordering along [1 ¯10 ] .</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/10158790','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/10158790"><span>Atomic scale <span class="hlt">structure</span> and chemistry of interfaces by Z-contrast imaging and <span class="hlt">electron</span> energy loss spectroscopy in the stem</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>McGibbon, M.M.; Browning, N.D.; Chisholm, M.F.</p> <p></p> <p>The macroscopic properties of many materials are controlled by the <span class="hlt">structure</span> and chemistry at grain boundaries. A basic understanding of the <span class="hlt">structure</span>-property relationship requires a technique which probes both composition and chemical bonding on an atomic scale. High-resolution Z-contrast imaging in the scanning transmission <span class="hlt">electron</span> microscope (STEM) forms an incoherent image in which changes in atomic <span class="hlt">structure</span> and composition across an interface can be interpreted directly without the need for preconceived atomic <span class="hlt">structure</span> models. Since the Z-contrast image is formed by <span class="hlt">electrons</span> scattered through high angles, parallel detection <span class="hlt">electron</span> energy loss spectroscopy (PEELS) can be used simultaneously to provide complementarymore » chemical information on an atomic scale. The fine <span class="hlt">structure</span> in the PEEL spectra can be used to investigate the <span class="hlt">local</span> <span class="hlt">electronic</span> <span class="hlt">structure</span> and the nature of the bonding across the interface. In this paper we use the complimentary techniques of high resolution Z-contrast imaging and PEELS to investigate the atomic <span class="hlt">structure</span> and chemistry of a 25{degree} symmetric tilt boundary in a bicrystal of the electroceramic SrTiO{sub 3}.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24093294','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24093294"><span><span class="hlt">Local</span> conservation laws and the <span class="hlt">structure</span> of the many-body <span class="hlt">localized</span> states.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Serbyn, Maksym; Papić, Z; Abanin, Dmitry A</p> <p>2013-09-20</p> <p>We construct a complete set of <span class="hlt">local</span> integrals of motion that characterize the many-body <span class="hlt">localized</span> (MBL) phase. Our approach relies on the assumption that <span class="hlt">local</span> perturbations act <span class="hlt">locally</span> on the eigenstates in the MBL phase, which is supported by numerical simulations of the random-field XXZ spin chain. We describe the <span class="hlt">structure</span> of the eigenstates in the MBL phase and discuss the implications of <span class="hlt">local</span> conservation laws for its nonequilibrium quantum dynamics. We argue that the many-body <span class="hlt">localization</span> can be used to protect coherence in the system by suppressing relaxation between eigenstates with different <span class="hlt">local</span> integrals of motion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1237579-probing-actinide-electronic-structure-through-pu-cluster-calculations','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1237579-probing-actinide-electronic-structure-through-pu-cluster-calculations"><span>Probing Actinide <span class="hlt">Electronic</span> <span class="hlt">Structure</span> through Pu Cluster Calculations</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Ryzhkov, Mickhail V.; Mirmelstein, Alexei; Yu, Sung-Woo; ...</p> <p>2013-02-26</p> <p>The calculations for the <span class="hlt">electronic</span> <span class="hlt">structure</span> of clusters of plutonium have been performed, within the framework of the relativistic discrete-variational method. Moreover, these theoretical results and those calculated earlier for related systems have been compared to spectroscopic data produced in the experimental investigations of bulk systems, including photoelectron spectroscopy. Observation of the changes in the Pu <span class="hlt">electronic</span> <span class="hlt">structure</span> as a function of size provides powerful insight for aspects of bulk Pu <span class="hlt">electronic</span> <span class="hlt">structure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JChPh.148l4707S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JChPh.148l4707S"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of ZrX2 (X = Se, Te)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shkvarin, A. S.; Merentsov, A. I.; Shkvarina, E. G.; Yarmoshenko, Yu. M.; Píš, I.; Nappini, S.; Titov, A. N.</p> <p>2018-03-01</p> <p>The <span class="hlt">electronic</span> <span class="hlt">structure</span> of the ZrX2 (X = Se, Te) compounds has been studied using photoelectron, resonant photoelectron and X-ray absorption spectroscopy, theoretical calculations of the X-ray absorption spectra, and density of <span class="hlt">electronic</span> states. It was found that the absorption spectra and valence band spectra are influenced by the chalcogen type. The results of the multiplet calculation of the Zr4+ atom show that the change in the splitting in the crystal field, which is described by the 10Dq parameter, is due to the change in the ratio of covalent and ionic contributions to the chemical bond. The resonance band near the Fermi level in the valence band spectra is observed for ZrTe2 in the Zr 3p-4d resonant excitation mode. The extent of photon energy indicates the charge <span class="hlt">localization</span> on the Zr atom. Similar resonance band for ZrSe2 is absent; it indicates the presence of a gap at the Fermi level.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29185061','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29185061"><span><span class="hlt">Electronic</span> <span class="hlt">structures</span> of elements according to ionization energies.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zadeh, Dariush H</p> <p>2017-11-28</p> <p>The <span class="hlt">electronic</span> <span class="hlt">structures</span> of elements in the periodic table were analyzed using available experimental ionization energies. Two new parameters were defined to carry out the study. The first parameter-apparent nuclear charge (ANC)-quantified the overall charge of the nucleus and inner <span class="hlt">electrons</span> observed by an outer <span class="hlt">electron</span> during the ionization process. This parameter was utilized to define a second parameter, which presented the shielding ability of an <span class="hlt">electron</span> against the nuclear charge. This second parameter-<span class="hlt">electron</span> shielding effect (ESE)-provided an insight into the <span class="hlt">electronic</span> <span class="hlt">structure</span> of atoms. This article avoids any sort of approximation, interpolation or extrapolation. First experimental ionization energies were used to obtain the two aforementioned parameters. The second parameter (ESE) was then graphed against the <span class="hlt">electron</span> number of each element, and was used to read the corresponding <span class="hlt">electronic</span> <span class="hlt">structure</span>. The ESE showed spikes/peaks at the end of each <span class="hlt">electronic</span> shell, providing insight into when an <span class="hlt">electronic</span> shell closes and a new one starts. The <span class="hlt">electronic</span> <span class="hlt">structures</span> of elements in the periodic table were mapped using this methodology. These graphs did not show complete agreement with the previously known "Aufbau" filling rule. A new filling rule was suggested based on the present observations. Finally, a new way to organize elements in the periodic table is suggested. Two earlier topics of effective nuclear charge, and shielding factor were also briefly discussed and compared numerically to demonstrate the capability of the new approach.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6256226-self-consistent-electronic-structure-disordered-fe-sub-sub-ni-sub-sub','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6256226-self-consistent-electronic-structure-disordered-fe-sub-sub-ni-sub-sub"><span>Self-consistent <span class="hlt">electronic</span> <span class="hlt">structure</span> of disordered Fe/sub 0/ /sub 65/Ni/sub 0/ /sub 35/</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>Johnson, D.D.; Pinski, F.J.; Stocks, G.M.</p> <p>1984-01-01</p> <p>We present the results of the first ab-initio calculation of the <span class="hlt">electronic</span> <span class="hlt">structure</span> of a disordered Fe/sub 0/ /sub 65/Ni/sub 0/ /sub 35/ alloy. The calculation is based on the multiple-scattering coherent-potential approach (KKR-CPA) and is fully self-consistent and spin-polarized. Magnetic effects are included within <span class="hlt">local</span>-spin-density functional theory using the exchange-correlation function of Vosko-Wilk-Nusair. The most striking feature of the calculation is that <span class="hlt">electrons</span> of different spins experience different degrees of disorder. The minority spin <span class="hlt">electrons</span> see a very large disorder; whereas, the majority spin <span class="hlt">electrons</span> see little disorder. Consequently, the minority spin density of states is smooth compared tomore » the very <span class="hlt">structured</span> majority spin density of states. This difference is due to a subtle balance between exchange-splitting and charge neutrality. 15 references, 2 figures.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5379487','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5379487"><span>Atomic <span class="hlt">structure</span> and <span class="hlt">electronic</span> properties of MgO grain boundaries in tunnelling magnetoresistive devices</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Bean, Jonathan J.; Saito, Mitsuhiro; Fukami, Shunsuke; Sato, Hideo; Ikeda, Shoji; Ohno, Hideo; Ikuhara, Yuichi; McKenna, Keith P.</p> <p>2017-01-01</p> <p>Polycrystalline metal oxides find diverse applications in areas such as nanoelectronics, photovoltaics and catalysis. Although grain boundary defects are ubiquitous their <span class="hlt">structure</span> and <span class="hlt">electronic</span> properties are very poorly understood since it is extremely challenging to probe the <span class="hlt">structure</span> of buried interfaces directly. In this paper we combine novel plan-view high-resolution transmission <span class="hlt">electron</span> microscopy and first principles calculations to provide atomic level understanding of the <span class="hlt">structure</span> and properties of grain boundaries in the barrier layer of a magnetic tunnel junction. We show that the highly [001] textured MgO films contain numerous tilt grain boundaries. First principles calculations reveal how these grain boundaries are associated with <span class="hlt">locally</span> reduced band gaps (by up to 3 eV). Using a simple model we show how shunting a proportion of the tunnelling current through grain boundaries imposes limits on the maximum magnetoresistance that can be achieved in devices. PMID:28374755</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1201340-electronic-structure-reconstruction-across-antiferromagnetic-transition-tafete-spin-ladder','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1201340-electronic-structure-reconstruction-across-antiferromagnetic-transition-tafete-spin-ladder"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> reconstruction across the antiferromagnetic transition in TaFe₁̣₂₃Te₃ spin ladder</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Xu, Min; Wang, Li -Min; Peng, Rui; ...</p> <p>2015-02-01</p> <p>With angle-resolved photoemission spectroscopy, we studied the <span class="hlt">electronic</span> <span class="hlt">structure</span> of TaFe₁̣₂₃Te₃, a two-leg spin ladder compound with a novel antiferromagnetic ground state. Quasi-two-dimensional Fermi surface is observed, with sizable inter-ladder hopping. Moreover, instead of observing an energy gap at the Fermi surface in the antiferromagnetic state, we observed the shifts of various bands. Combining these observations with density-functional-theory calculations, we propose that the large scale reconstruction of the <span class="hlt">electronic</span> <span class="hlt">structure</span>, caused by the interactions between coexisting itinerant <span class="hlt">electrons</span> and <span class="hlt">local</span> moments, is most likely the driving force of the magnetic transition. Thus TaFe₁̣₂₃Te₃ serves as a simpler platform that containsmore » similar ingredients as the parent compounds of iron-based superconductors.« 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_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('http://adsabs.harvard.edu/abs/2015REDS..170..894L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015REDS..170..894L"><span>Theoretical studies of the EPR parameters and <span class="hlt">local</span> <span class="hlt">structures</span> for Cu2+-doped cobalt ammonium phosphate hexahydrate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Chao-Ying; Liu, Shi-Fei; Fu, Jin-Xian</p> <p>2015-11-01</p> <p>High-order perturbation formulas for a 3d9 ion in rhombically elongated octahedral was applied to calculate the <span class="hlt">electron</span> paramagnetic resonance (EPR) parameters (the g factors, gi, and the hyperfine <span class="hlt">structure</span> constants Ai, i = x, y, z) of the rhombic Cu2+ center in CoNH4PO4.6H2O. In the calculations, the required crystal-field parameters are estimated from the superposition model which enables correlation of the crystal-field parameters and hence the EPR parameters with the <span class="hlt">local</span> <span class="hlt">structure</span> of the rhombic Cu2+ center. Based on the calculations, the ligand octahedral (i.e. [Cu(H2O)6]2+ cluster) are found to experience the <span class="hlt">local</span> bond length variations ΔZ (≈0.213 Å) and δr (≈0.132 Å) along axial and perpendicular directions due to the Jahn-Teller effect. Theoretical EPR parameters based on the above <span class="hlt">local</span> <span class="hlt">structure</span> are in good agreement with the observed values; the results are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5225986','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5225986"><span>Automatic Segmentation and Quantification of Filamentous <span class="hlt">Structures</span> in <span class="hlt">Electron</span> Tomography</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Loss, Leandro A.; Bebis, George; Chang, Hang; Auer, Manfred; Sarkar, Purbasha; Parvin, Bahram</p> <p>2016-01-01</p> <p><span class="hlt">Electron</span> tomography is a promising technology for imaging ultrastructures at nanoscale resolutions. However, image and quantitative analyses are often hindered by high levels of noise, staining heterogeneity, and material damage either as a result of the <span class="hlt">electron</span> beam or sample preparation. We have developed and built a framework that allows for automatic segmentation and quantification of filamentous objects in 3D <span class="hlt">electron</span> tomography. Our approach consists of three steps: (i) <span class="hlt">local</span> enhancement of filaments by Hessian filtering; (ii) detection and completion (e.g., gap filling) of filamentous <span class="hlt">structures</span> through tensor voting; and (iii) delineation of the filamentous networks. Our approach allows for quantification of filamentous networks in terms of their compositional and morphological features. We first validate our approach using a set of specifically designed synthetic data. We then apply our segmentation framework to tomograms of plant cell walls that have undergone different chemical treatments for polysaccharide extraction. The subsequent compositional and morphological analyses of the plant cell walls reveal their organizational characteristics and the effects of the different chemical protocols on specific polysaccharides. PMID:28090597</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28090597','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28090597"><span>Automatic Segmentation and Quantification of Filamentous <span class="hlt">Structures</span> in <span class="hlt">Electron</span> Tomography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Loss, Leandro A; Bebis, George; Chang, Hang; Auer, Manfred; Sarkar, Purbasha; Parvin, Bahram</p> <p>2012-10-01</p> <p><span class="hlt">Electron</span> tomography is a promising technology for imaging ultrastructures at nanoscale resolutions. However, image and quantitative analyses are often hindered by high levels of noise, staining heterogeneity, and material damage either as a result of the <span class="hlt">electron</span> beam or sample preparation. We have developed and built a framework that allows for automatic segmentation and quantification of filamentous objects in 3D <span class="hlt">electron</span> tomography. Our approach consists of three steps: (i) <span class="hlt">local</span> enhancement of filaments by Hessian filtering; (ii) detection and completion (e.g., gap filling) of filamentous <span class="hlt">structures</span> through tensor voting; and (iii) delineation of the filamentous networks. Our approach allows for quantification of filamentous networks in terms of their compositional and morphological features. We first validate our approach using a set of specifically designed synthetic data. We then apply our segmentation framework to tomograms of plant cell walls that have undergone different chemical treatments for polysaccharide extraction. The subsequent compositional and morphological analyses of the plant cell walls reveal their organizational characteristics and the effects of the different chemical protocols on specific polysaccharides.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvB..96k5126F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvB..96k5126F"><span><span class="hlt">Electronic</span> <span class="hlt">structures</span> of U X3 (X =Al , Ga, and In) studied by photoelectron spectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fujimori, Shin-ichi; Kobata, Masaaki; Takeda, Yukiharu; Okane, Tetsuo; Saitoh, Yuji; Fujimori, Atsushi; Yamagami, Hiroshi; Haga, Yoshinori; Yamamoto, Etsuji; Ōnuki, Yoshichika</p> <p>2017-09-01</p> <p>The <span class="hlt">electronic</span> <span class="hlt">structures</span> of U X3 (X =Al , Ga , and In ) were studied by photoelectron spectroscopy to understand the relationship between their <span class="hlt">electronic</span> <span class="hlt">structures</span> and magnetic properties. The band <span class="hlt">structures</span> and Fermi surfaces of UAl3 and UGa3 were revealed experimentally by angle-resolved photoelectron spectroscopy (ARPES), and they were compared with the result of band-<span class="hlt">structure</span> calculations. The topologies of the Fermi surfaces and the band <span class="hlt">structures</span> of UAl3 and UGa3 were explained reasonably well by the calculation, although bands near the Fermi level (EF) were renormalized owing to the finite <span class="hlt">electron</span> correlation effect. The topologies of the Fermi surfaces of UAl3 and UGa3 are very similar to each other, except for some minor differences. Such minor differences in their Fermi surface or <span class="hlt">electron</span> correlation effect might take an essential role in their different magnetic properties. No significant changes were observed between the ARPES spectra of UGa3 in the paramagnetic and antiferromagnetic phases, suggesting that UGa3 is an itinerant weak antiferromagnet. The effect of chemical pressure on the <span class="hlt">electronic</span> <span class="hlt">structures</span> of U X3 compounds was also studied by utilizing the smaller lattice constants of UAl3 and UGa3 than that of UIn3. The valence band spectrum of UIn3 is accompanied by a satellitelike <span class="hlt">structure</span> on the high-binding-energy side. The core-level spectrum of UIn3 is also qualitatively different from those of UAl3 and UGa3. These findings suggest that the U 5 f states in UIn3 are more <span class="hlt">localized</span> than those in UAl3 and UGa3.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApSS..447..618C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApSS..447..618C"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of strongly reduced (1 ‾ 1 1) surface of monoclinic HfO2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cheng, YingXing; Zhu, Linggang; Ying, Yile; Zhou, Jian; Sun, Zhimei</p> <p>2018-07-01</p> <p>Material surface is playing an increasingly important role in <span class="hlt">electronic</span> devices as their size down to nanoscale. Here, by first-principles calculations we studied the surface oxygen-vacancies (Vos) induced <span class="hlt">electronic-structure</span> variation of HfO2 , in order to explore its potential applications in surface-controlled <span class="hlt">electronic</span> devices. Firstly, it is found that single Vo tends to segregate onto the surface and attracts each other as they form pairs, making the formation of vacancies-contained functional surface possible. Then extensive Vo-chains whose formation/rupture can represent the high/low conductivity state are constructed. The <span class="hlt">electronic</span> states induced by the Vos remain <span class="hlt">localized</span> in the band-gap region for most of the Vo-chains studied here. A transition to a metallic conductance is found in metastable Vo-chain with formation energy increased by 0.25 eV per Vo. Moreover, we highlight the significance of the Hubbard U correction for density functional theory when studying the <span class="hlt">electronic-structure</span> based conductance in the oxides. By comprehensive calculations, we find a conductivity-stability dilemma of the Vo-chains, providing guideline for understanding and designing the <span class="hlt">electronic</span> devices based on HfO2 surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MARA12003S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MARA12003S"><span><span class="hlt">Structure</span> and Dynamics with Ultrafast <span class="hlt">Electron</span> Microscopes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Siwick, Bradley</p> <p></p> <p>In this talk I will describe how combining ultrafast lasers and <span class="hlt">electron</span> microscopes in novel ways makes it possible to directly `watch' the time-evolving <span class="hlt">structure</span> of condensed matter, both at the level of atomic-scale <span class="hlt">structural</span> rearrangements in the unit cell and at the level of a material's nano- microstructure. First, I will briefly describe my group's efforts to develop ultrafast <span class="hlt">electron</span> diffraction using radio- frequency compressed <span class="hlt">electron</span> pulses in the 100keV range, a system that rivals the capabilities of xray free <span class="hlt">electron</span> lasers for diffraction experiments. I will give several examples of the new kinds of information that can be gleaned from such experiments. In vanadium dioxide we have mapped the detailed reorganization of the unit cell during the much debated insulator-metal transition. In particular, we have been able to identify and separate lattice <span class="hlt">structural</span> changes from valence charge density redistribution in the material on the ultrafast timescale. In doing so we uncovered a previously unreported optically accessible phase/state of vanadium dioxide that has monoclinic crystallography like the insulator, but <span class="hlt">electronic</span> <span class="hlt">structure</span> and properties that are more like the rutile metal. We have also combined these dynamic <span class="hlt">structural</span> measurements with broadband ultrafast spectroscopy to make detailed connections between <span class="hlt">structure</span> and properties for the photoinduced insulator to metal transition. Second, I will show how dynamic transmission <span class="hlt">electron</span> microscopy (DTEM) can be used to make direct, real space images of nano-microstructural evolution during laser-induced crystallization of amorphous semiconductors at unprecedented spatio-temporal resolution. This is a remarkably complex process that involves several distinct modes of crystal growth and the development of intricate microstructural patterns on the nanosecond to ten microsecond timescales all of which can be imaged directly with DTEM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018CPL...691..283D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018CPL...691..283D"><span><span class="hlt">Structural</span> and <span class="hlt">electronic</span> properties of M-MOF-74 (M = Mg, Co or Mn)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Oliveira, Aline; de Lima, Guilherme Ferreira; De Abreu, Heitor Avelino</p> <p>2018-01-01</p> <p>The Metal-Organic Frameworks M-MOF-74 (M = Mg, Co or Mn) were investigated through Density Functional Theory calculations. <span class="hlt">Structural</span> parameters and band gap energies were determined in agreement with experimental data, with errors under 2%. The methods <span class="hlt">Electron</span> <span class="hlt">Localization</span> Function and Quantum Theory of Atoms in Molecules were applied to the analyses of the <span class="hlt">electronic</span> density topology of the three solids. These methodologies indicated that the bonds between the metallic cations and the oxygen atoms are predominantly ionic while the other ones are predominantly covalent. Furthermore, non-conventional hydrogen bonds were identified to Mg-MOF-74 and Co-MOF-74, which were not observed to Mn-MOF-74.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4368384','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4368384"><span>Modeling Biophysical and Biological Properties From the Characteristics of the Molecular <span class="hlt">Electron</span> Density, <span class="hlt">Electron</span> <span class="hlt">Localization</span> and Delocalization Matrices, and the Electrostatic Potential</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Matta*, Chérif F</p> <p>2014-01-01</p> <p>The <span class="hlt">electron</span> density and the electrostatic potential are fundamentally related to the molecular hamiltonian, and hence are the ultimate source of all properties in the ground- and excited-states. The advantages of using molecular descriptors derived from these fundamental scalar fields, both accessible from theory and from experiment, in the formulation of quantitative <span class="hlt">structure</span>-to-activity and <span class="hlt">structure</span>-to-property relationships, collectively abbreviated as QSAR, are discussed. A few such descriptors encode for a wide variety of properties including, for example, <span class="hlt">electronic</span> transition energies, pKa's, rates of ester hydrolysis, NMR chemical shifts, DNA dimers binding energies, π-stacking energies, toxicological indices, cytotoxicities, hepatotoxicities, carcinogenicities, partial molar volumes, partition coefficients (log P), hydrogen bond donor capacities, enzyme–substrate complementarities, bioisosterism, and regularities in the genetic code. <span class="hlt">Electronic</span> fingerprinting from the topological analysis of the <span class="hlt">electron</span> density is shown to be comparable and possibly superior to Hammett constants and can be used in conjunction with traditional bulk and liposolubility descriptors to accurately predict biological activities. A new class of descriptors obtained from the quantum theory of atoms in molecules' (QTAIM) <span class="hlt">localization</span> and delocalization indices and bond properties, cast in matrix format, is shown to quantify transferability and molecular similarity meaningfully. Properties such as “interacting quantum atoms (IQA)” energies which are expressible into an interaction matrix of two body terms (and diagonal one body “self” terms, as IQA energies) can be used in the same manner. The proposed QSAR-type studies based on similarity distances derived from such matrix representatives of molecular <span class="hlt">structure</span> necessitate extensive investigation before their utility is unequivocally established. © 2014 The Author and the Journal of Computational Chemistry Published</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27534565','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27534565"><span>Cytochrome b 6 f function and <span class="hlt">localization</span>, phosphorylation state of thylakoid membrane proteins and consequences on cyclic <span class="hlt">electron</span> flow.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dumas, Louis; Chazaux, Marie; Peltier, Gilles; Johnson, Xenie; Alric, Jean</p> <p>2016-09-01</p> <p>Both the <span class="hlt">structure</span> and the protein composition of thylakoid membranes have an impact on light harvesting and <span class="hlt">electron</span> transfer in the photosynthetic chain. Thylakoid membranes form stacks and lamellae where photosystem II and photosystem I <span class="hlt">localize</span>, respectively. Light-harvesting complexes II can be associated to either PSII or PSI depending on the redox state of the plastoquinone pool, and their distribution is governed by state transitions. Upon state transitions, the thylakoid ultrastructure and lateral distribution of proteins along the membrane are subject to significant rearrangements. In addition, quinone diffusion is limited to membrane microdomains and the cytochrome b 6 f complex <span class="hlt">localizes</span> either to PSII-containing grana stacks or PSI-containing stroma lamellae. Here, we discuss possible similarities or differences between green algae and C3 plants on the functional consequences of such heterogeneities in the photosynthetic <span class="hlt">electron</span> transport chain and propose a model in which quinones, accepting <span class="hlt">electrons</span> either from PSII (linear flow) or NDH/PGR pathways (cyclic flow), represent a crucial control point. Our aim is to give an integrated description of these processes and discuss their potential roles in the balance between linear and cyclic <span class="hlt">electron</span> flows.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5360252','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5360252"><span><span class="hlt">Local</span> <span class="hlt">structure</span> preserving sparse coding for infrared target recognition</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Han, Jing; Yue, Jiang; Zhang, Yi; Bai, Lianfa</p> <p>2017-01-01</p> <p>Sparse coding performs well in image classification. However, robust target recognition requires a lot of comprehensive template images and the sparse learning process is complex. We incorporate sparsity into a template matching concept to construct a <span class="hlt">local</span> sparse <span class="hlt">structure</span> matching (LSSM) model for general infrared target recognition. A <span class="hlt">local</span> <span class="hlt">structure</span> preserving sparse coding (LSPSc) formulation is proposed to simultaneously preserve the <span class="hlt">local</span> sparse and <span class="hlt">structural</span> information of objects. By adding a spatial <span class="hlt">local</span> <span class="hlt">structure</span> constraint into the classical sparse coding algorithm, LSPSc can improve the stability of sparse representation for targets and inhibit background interference in infrared images. Furthermore, a kernel LSPSc (K-LSPSc) formulation is proposed, which extends LSPSc to the kernel space to weaken the influence of the linear <span class="hlt">structure</span> constraint in nonlinear natural data. Because of the anti-interference and fault-tolerant capabilities, both LSPSc- and K-LSPSc-based LSSM can implement target identification based on a simple template set, which just needs several images containing enough <span class="hlt">local</span> sparse <span class="hlt">structures</span> to learn a sufficient sparse <span class="hlt">structure</span> dictionary of a target class. Specifically, this LSSM approach has stable performance in the target detection with scene, shape and occlusions variations. High performance is demonstrated on several datasets, indicating robust infrared target recognition in diverse environments and imaging conditions. PMID:28323824</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790019938','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790019938"><span>A theory of <span class="hlt">local</span> and global processes which affect solar wind <span class="hlt">electrons</span>. 2: Experimental support</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Scudder, J. D.; Olbert, S.</p> <p>1979-01-01</p> <p>The microscopic characteristics of the Coulomb cross section show that there are three natural subpopulations for plasma <span class="hlt">electrons</span>: the subthermals with <span class="hlt">local</span> kinetic energy E kT sub c; the transthermals with kT sub c E 7 kT sub c and the extrathermals E 7 kT sub c. Data from three experimental groups on three different spacecraft in the interplanetary medium over a radial range are presented to support the five interrelations projected between solar wind <span class="hlt">electron</span> properties and changes in the interplanetary medium: (1) subthermals respond primarily to <span class="hlt">local</span> changes (compression and rarefactions) in stream dynamics; (2) the extrathermal fraction of the ambient <span class="hlt">electron</span> density should be anti-correlated with the asymptotic bulk speed; (3) the extrathermal "temperature" should be anti-correlated with the <span class="hlt">local</span> wind speed at 1 AU; (4) the heat flux carried by <span class="hlt">electrons</span> should be anti-correlated with the <span class="hlt">local</span> bulk speed; and (5) the extrathermal differential 'temperature' should be nearly independent of radius within 1 AU.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JChPh.144s1101S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JChPh.144s1101S"><span>Communication: Near-<span class="hlt">locality</span> of exchange and correlation density functionals for 1- and 2-<span class="hlt">electron</span> systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sun, Jianwei; Perdew, John P.; Yang, Zenghui; Peng, Haowei</p> <p>2016-05-01</p> <p>The uniform <span class="hlt">electron</span> gas and the hydrogen atom play fundamental roles in condensed matter physics and quantum chemistry. The former has an infinite number of <span class="hlt">electrons</span> uniformly distributed over the neutralizing positively charged background, and the latter only one <span class="hlt">electron</span> bound to the proton. The uniform <span class="hlt">electron</span> gas was used to derive the <span class="hlt">local</span> spin density approximation to the exchange-correlation functional that undergirds the development of the Kohn-Sham density functional theory. We show here that the ground-state exchange-correlation energies of the hydrogen atom and many other 1- and 2-<span class="hlt">electron</span> systems are modeled surprisingly well by a different <span class="hlt">local</span> spin density approximation (LSDA0). LSDA0 is constructed to satisfy exact constraints but agrees surprisingly well with the exact results for a uniform two-<span class="hlt">electron</span> density in a finite, curved three-dimensional space. We also apply LSDA0 to excited or noded 1-<span class="hlt">electron</span> densities, where it works less well. Furthermore, we show that the <span class="hlt">localization</span> of the exact exchange hole for a 1- or 2-<span class="hlt">electron</span> ground state can be measured by the ratio of the exact exchange energy to its optimal lower bound.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Nanot..28e5206A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Nanot..28e5206A"><span><span class="hlt">Structure</span> and <span class="hlt">local</span> charging of electromigrated Au nanocontacts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arnold, D.; Marz, M.; Schneider, S.; Hoffmann-Vogel, R.</p> <p>2017-02-01</p> <p>We study the <span class="hlt">structure</span> and the <span class="hlt">electronic</span> properties of Au nanocontacts created by controlled electromigration of thin film devices, a method frequently used to contact molecules. In contrast to electromigration testing, a current is applied in a cyclic fashion and during each cycle the resistance increase of the metal upon heating is used to avoid thermal runaway. In this way, nanometer sized-gaps are obtained. The thin film devices with an optimized <span class="hlt">structure</span> at the origin of the electromigration process are made by shadow evaporation without contamination by organic materials. Defining rounded edges and a thinner area in the center of the device allow to pre-determine the location where the electromigration takes place. Scanning force microscopy images of the pristine Au film and electromigrated contact show its grainy <span class="hlt">structure</span>. Through electromigration, a 1.5 μm-wide slit is formed, with extensions only on the anode side that had previously not been observed in narrower <span class="hlt">structures</span>. It is discussed whether this could be explained by asymmetric heating of both electrodes. New grains are formed in the slit and on the extensions on both, the anode and the cathode side. The smaller <span class="hlt">structures</span> inside the slit lead to an electrode distance below 150 nm. Kelvin probe force microscopy images show a <span class="hlt">local</span> work function difference with fluctuations of 70 mV on the metal before electromigration. Between the electrodes, disconnected through electromigration, a work function difference of 3.2 V is observed due to charging. Some of the grains newly formed by electromigration are electrically disconnected from the electrodes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JLTP..tmp...27G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JLTP..tmp...27G"><span>Anomalous <span class="hlt">Electron</span> Spectrum and Its Relation to Peak <span class="hlt">Structure</span> of <span class="hlt">Electron</span> Scattering Rate in Cuprate Superconductors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gao, Deheng; Mou, Yingping; Feng, Shiping</p> <p>2018-02-01</p> <p>The recent discovery of a direct link between the sharp peak in the <span class="hlt">electron</span> quasiparticle scattering rate of cuprate superconductors and the well-known peak-dip-hump <span class="hlt">structure</span> in the <span class="hlt">electron</span> quasiparticle excitation spectrum is calling for an explanation. Within the framework of the kinetic-energy-driven superconducting mechanism, the complicated line-shape in the <span class="hlt">electron</span> quasiparticle excitation spectrum of cuprate superconductors is investigated. It is shown that the interaction between <span class="hlt">electrons</span> by the exchange of spin excitations generates a notable peak <span class="hlt">structure</span> in the <span class="hlt">electron</span> quasiparticle scattering rate around the antinodal and nodal regions. However, this peak <span class="hlt">structure</span> disappears at the hot spots, which leads to that the striking peak-dip-hump <span class="hlt">structure</span> is developed around the antinodal and nodal regions, and vanishes at the hot spots. The theory also confirms that the sharp peak observed in the <span class="hlt">electron</span> quasiparticle scattering rate is directly responsible for the remarkable peak-dip-hump <span class="hlt">structure</span> in the <span class="hlt">electron</span> quasiparticle excitation spectrum of cuprate superconductors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21403375','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21403375"><span>Magnetic forces and <span class="hlt">localized</span> resonances in <span class="hlt">electron</span> transfer through quantum rings.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Poniedziałek, M R; Szafran, B</p> <p>2010-11-24</p> <p>We study the current flow through semiconductor quantum rings. In high magnetic fields the current is usually injected into the arm of the ring preferred by classical magnetic forces. However, for narrow magnetic field intervals that appear periodically on the magnetic field scale the current is injected into the other arm of the ring. We indicate that the appearance of the anomalous-non-classical-current circulation results from Fano interference involving <span class="hlt">localized</span> resonant states. The identification of the Fano interference is based on the comparison of the solution of the scattering problem with the results of the stabilization method. The latter employs the bound-state type calculations and allows us to extract both the energy of metastable states <span class="hlt">localized</span> within the ring and the width of resonances by analysis of the energy spectrum of a finite size system as a function of its length. The Fano resonances involving states of anomalous current circulation become extremely narrow on both the magnetic field and energy scales. This is consistent with the orientation of the Lorentz force that tends to keep the <span class="hlt">electron</span> within the ring and thus increases the lifetime of the <span class="hlt">electron</span> <span class="hlt">localization</span> within the ring. Absence of periodic Fano resonances in <span class="hlt">electron</span> transfer probability through a quantum ring containing an elastic scatterer is also explained.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvB..96c5440W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvB..96c5440W"><span><span class="hlt">Local</span> field enhancement and thermoplasmonics in multimodal aluminum <span class="hlt">structures</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wiecha, Peter R.; Mennemanteuil, Marie-Maxime; Khlopin, Dmitry; Martin, Jérôme; Arbouet, Arnaud; Gérard, Davy; Bouhelier, Alexandre; Plain, Jérôme; Cuche, Aurélien</p> <p>2017-07-01</p> <p>Aluminum nanostructures have recently been at the focus of numerous studies due to their properties including oxidation stability and surface plasmon resonances covering the ultraviolet and visible spectral windows. In this article, we reveal a facet of this metal relevant for both plasmonic purposes and photothermal conversion. The field distribution of high-order plasmonic resonances existing in two-dimensional Al <span class="hlt">structures</span> is studied by nonlinear photoluminescence microscopy in a spectral region where <span class="hlt">electronic</span> interband transitions occur. The polarization sensitivity of the field intensity maps shows that the electric field concentration can be addressed and controlled on demand. We use a numerical tool based on the Green dyadic method to analyze our results and to simulate the absorbed energy that is <span class="hlt">locally</span> converted into heat. The polarization-dependent temperature increase of the Al <span class="hlt">structures</span> is experimentally quantitatively measured, and is in an excellent agreement with theoretical predictions. Our work highlights Al as a promising candidate for designing thermal nanosources integrated in coplanar geometries for thermally assisted nanomanipulation or biophysical applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29220075','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29220075"><span>Protein 3D <span class="hlt">Structure</span> and <span class="hlt">Electron</span> Microscopy Map Retrieval Using 3D-SURFER2.0 and EM-SURFER.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Han, Xusi; Wei, Qing; Kihara, Daisuke</p> <p>2017-12-08</p> <p>With the rapid growth in the number of solved protein <span class="hlt">structures</span> stored in the Protein Data Bank (PDB) and the <span class="hlt">Electron</span> Microscopy Data Bank (EMDB), it is essential to develop tools to perform real-time <span class="hlt">structure</span> similarity searches against the entire <span class="hlt">structure</span> database. Since conventional <span class="hlt">structure</span> alignment methods need to sample different orientations of proteins in the three-dimensional space, they are time consuming and unsuitable for rapid, real-time database searches. To this end, we have developed 3D-SURFER and EM-SURFER, which utilize 3D Zernike descriptors (3DZD) to conduct high-throughput protein <span class="hlt">structure</span> comparison, visualization, and analysis. Taking an atomic <span class="hlt">structure</span> or an <span class="hlt">electron</span> microscopy map of a protein or a protein complex as input, the 3DZD of a query protein is computed and compared with the 3DZD of all other proteins in PDB or EMDB. In addition, <span class="hlt">local</span> geometrical characteristics of a query protein can be analyzed using VisGrid and LIGSITE CSC in 3D-SURFER. This article describes how to use 3D-SURFER and EM-SURFER to carry out protein surface shape similarity searches, <span class="hlt">local</span> geometric feature analysis, and interpretation of the search results. © 2017 by John Wiley & Sons, Inc. Copyright © 2017 John Wiley & Sons, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28323208','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28323208"><span>Platinum replica <span class="hlt">electron</span> microscopy: Imaging the cytoskeleton globally and <span class="hlt">locally</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Svitkina, Tatyana M</p> <p>2017-05-01</p> <p><span class="hlt">Structural</span> studies reveal how smaller components of a system work together as a whole. However, combining high resolution of details with full coverage of the whole is challenging. In cell biology, light microscopy can image many cells in their entirety, but at a lower resolution, whereas <span class="hlt">electron</span> microscopy affords very high resolution, but usually at the expense of the sample size and coverage. <span class="hlt">Structural</span> analyses of the cytoskeleton are especially demanding, because cytoskeletal networks are unresolvable by light microscopy due to their density and intricacy, whereas their proper preservation is a challenge for <span class="hlt">electron</span> microscopy. Platinum replica <span class="hlt">electron</span> microscopy can uniquely bridge the gap between the "comfort zones" of light and <span class="hlt">electron</span> microscopy by allowing high resolution imaging of the cytoskeleton throughout the entire cell and in many cells in the population. This review describes the principles and applications of platinum replica <span class="hlt">electron</span> microscopy for studies of the cytoskeleton. Copyright © 2017 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5424547','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5424547"><span>Platinum Replica <span class="hlt">Electron</span> Microscopy: Imaging the Cytoskeleton Globally and <span class="hlt">Locally</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>SVITKINA, Tatyana M.</p> <p>2017-01-01</p> <p><span class="hlt">Structural</span> studies reveal how smaller components of a system work together as a whole. However, combining high resolution of details with full coverage of the whole is challenging. In cell biology, light microscopy can image many cells in their entirety, but at a lower resolution, whereas <span class="hlt">electron</span> microscopy affords very high resolution, but usually at the expense of the sample size and coverage. <span class="hlt">Structural</span> analyses of the cytoskeleton are especially demanding, because cytoskeletal networks are unresolvable by light microscopy due to their density and intricacy, whereas their proper preservation is a challenge for <span class="hlt">electron</span> microscopy. Platinum replica <span class="hlt">electron</span> microscopy can uniquely bridge the gap between the “comfort zones” of light and <span class="hlt">electron</span> microscopy by allowing high resolution imaging of the cytoskeleton throughout the entire cell and in many cells in the population. This review describes the principles and applications of platinum replica <span class="hlt">electron</span> microscopy for studies of the cytoskeleton. PMID:28323208</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1985SurSc.164..367T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1985SurSc.164..367T"><span><span class="hlt">Structure</span> analysis of Si(111)-7 × 7 reconstructed surface by transmission <span class="hlt">electron</span> diffraction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Takayanagi, Kunio; Tanishiro, Yasumasa; Takahashi, Shigeki; Takahashi, Masaetsu</p> <p>1985-12-01</p> <p>The atomic <span class="hlt">structure</span> of the 7 × 7 reconstructed Si(111) surface has been analysed by ultra-high vacuum (UHV) transmission <span class="hlt">electron</span> diffraction (TED). A possible projected <span class="hlt">structure</span> of the surface is deduced from the intensity distribution in TED patterns of normal <span class="hlt">electron</span> incidence and from Patterson and Fourier syntheses of the intensities. A new three-dimensional <span class="hlt">structure</span> model, the DAS model, is proposed: The model consists of 12 adatoms arranged <span class="hlt">locally</span> in the 2 × 2 <span class="hlt">structure</span>, a stacking fault layer and a layer with a vacancy at the corner and 9 dimers on the sides of each of the two triangular subcells of the 7 × 7 unit cell. The silicon layers in one subcell are stacked with the normal sequence, CcAaB + adatoms, while those in the other subcell are stacked with a faulted sequence, CcAa/C + adatoms. The model has only 19 dangling bonds, the smallest number among models so far proposed. Previously proposed models are tested quantitatively by the TED intensity. Advantages and limits of the TED analysis are discussed.</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('https://www.ncbi.nlm.nih.gov/pubmed/23851673','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23851673"><span>Strain and curvature induced evolution of <span class="hlt">electronic</span> band <span class="hlt">structures</span> in twisted graphene bilayer.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yan, Wei; He, Wen-Yu; Chu, Zhao-Dong; Liu, Mengxi; Meng, Lan; Dou, Rui-Fen; Zhang, Yanfeng; Liu, Zhongfan; Nie, Jia-Cai; He, Lin</p> <p>2013-01-01</p> <p>It is well established that strain and geometry could affect the band <span class="hlt">structure</span> of graphene monolayer dramatically. Here we study the evolution of <span class="hlt">local</span> <span class="hlt">electronic</span> properties of a twisted graphene bilayer induced by a strain and a high curvature, which are found to strongly affect the <span class="hlt">local</span> band <span class="hlt">structures</span> of the twisted graphene bilayer. The energy difference of the two low-energy van Hove singularities decreases with increasing lattice deformation and the states condensed into well-defined pseudo-Landau levels, which mimic the quantization of massive chiral fermions in a magnetic field of about 100 T, along a graphene wrinkle. The joint effect of strain and out-of-plane distortion in the graphene wrinkle also results in a valley polarization with a significant gap. These results suggest that strained graphene bilayer could be an ideal platform to realize the high-temperature zero-field quantum valley Hall effect.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhPl...25d2303S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhPl...25d2303S"><span><span class="hlt">Electron</span> acoustic nonlinear <span class="hlt">structures</span> in planetary magnetospheres</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shah, K. H.; Qureshi, M. N. S.; Masood, W.; Shah, H. A.</p> <p>2018-04-01</p> <p>In this paper, we have studied linear and nonlinear propagation of <span class="hlt">electron</span> acoustic waves (EAWs) comprising cold and hot populations in which the ions form the neutralizing background. The hot <span class="hlt">electrons</span> have been assumed to follow the generalized ( r , q ) distribution which has the advantage that it mimics most of the distribution functions observed in space plasmas. Interestingly, it has been found that unlike Maxwellian and kappa distributions, the <span class="hlt">electron</span> acoustic waves admit not only rarefactive <span class="hlt">structures</span> but also allow the formation of compressive solitary <span class="hlt">structures</span> for generalized ( r , q ) distribution. It has been found that the flatness parameter r , tail parameter q , and the nonlinear propagation velocity u affect the propagation characteristics of nonlinear EAWs. Using the plasmas parameters, typically found in Saturn's magnetosphere and the Earth's auroral region, where two populations of <span class="hlt">electrons</span> and <span class="hlt">electron</span> acoustic solitary waves (EASWs) have been observed, we have given an estimate of the scale lengths over which these nonlinear waves are expected to form and how the size of these <span class="hlt">structures</span> would vary with the change in the shape of the distribution function and with the change of the plasma parameters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008NPGeo..15..831D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008NPGeo..15..831D"><span>The formation of relativistic plasma <span class="hlt">structures</span> and their potential role in the generation of cosmic ray <span class="hlt">electrons</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dieckmann, M. E.</p> <p>2008-11-01</p> <p>Recent particle-in-cell (PIC) simulation studies have addressed particle acceleration and magnetic field generation in relativistic astrophysical flows by plasma phase space <span class="hlt">structures</span>. We discuss the astrophysical environments such as the jets of compact objects, and we give an overview of the global PIC simulations of shocks. These reveal several types of phase space <span class="hlt">structures</span>, which are relevant for the energy dissipation. These <span class="hlt">structures</span> are typically coupled in shocks, but we choose to consider them here in an isolated form. Three <span class="hlt">structures</span> are reviewed. (1) Simulations of interpenetrating or colliding plasma clouds can trigger filamentation instabilities, while simulations of thermally anisotropic plasmas observe the Weibel instability. Both transform a spatially uniform plasma into current filaments. These filament <span class="hlt">structures</span> cause the growth of the magnetic fields. (2) The development of a modified two-stream instability is discussed. It saturates first by the formation of <span class="hlt">electron</span> phase space holes. The relativistic <span class="hlt">electron</span> clouds modulate the ion beam and a secondary, spatially <span class="hlt">localized</span> electrostatic instability grows, which saturates by forming a relativistic ion phase space hole. It accelerates <span class="hlt">electrons</span> to ultra-relativistic speeds. (3) A simulation is also revised, in which two clouds of an <span class="hlt">electron</span>-ion plasma collide at the speed 0.9c. The inequal densities of both clouds and a magnetic field that is oblique to the collision velocity vector result in waves with a mixed electrostatic and electromagnetic polarity. The waves give rise to growing corkscrew distributions in the <span class="hlt">electrons</span> and ions that establish an equipartition between the <span class="hlt">electron</span>, the ion and the magnetic energy. The filament-, phase space hole- and corkscrew <span class="hlt">structures</span> are discussed with respect to <span class="hlt">electron</span> acceleration and magnetic field generation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23235114','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23235114"><span>Quasiparticle band <span class="hlt">structure</span> of rocksalt-CdO determined using maximally <span class="hlt">localized</span> Wannier functions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dixit, H; Lamoen, D; Partoens, B</p> <p>2013-01-23</p> <p>CdO in the rocksalt <span class="hlt">structure</span> is an indirect band gap semiconductor. Thus, in order to determine its band gap one needs to calculate the complete band <span class="hlt">structure</span>. However, in practice, the exact evaluation of the quasiparticle band <span class="hlt">structure</span> for the large number of k-points which constitute the different symmetry lines in the Brillouin zone can be an extremely demanding task compared to the standard density functional theory (DFT) calculation. In this paper we report the full quasiparticle band <span class="hlt">structure</span> of CdO using a plane-wave pseudopotential approach. In order to reduce the computational effort and time, we make use of maximally <span class="hlt">localized</span> Wannier functions (MLWFs). The MLWFs offer a highly accurate method for interpolation of the DFT or GW band <span class="hlt">structure</span> from a coarse k-point mesh in the irreducible Brillouin zone, resulting in a much reduced computational effort. The present paper discusses the technical details of the scheme along with the results obtained for the quasiparticle band gap and the <span class="hlt">electron</span> effective mass.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22004925','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22004925"><span>The <span class="hlt">electronic</span> <span class="hlt">structure</span> of lithium metagallate.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Johnson, N W; McLeod, J A; Moewes, A</p> <p>2011-11-09</p> <p>Herein we present a study of the <span class="hlt">electronic</span> <span class="hlt">structure</span> of lithium metagallate (LiGaO(2)), a material of interest in the field of optoelectronics. We use soft x-ray spectroscopy to probe the <span class="hlt">electronic</span> <span class="hlt">structure</span> of both the valence and conduction bands and compare our measurements to ab initio density functional theory calculations. We use several different exchange-correlation functionals, but find that no single theoretical approach used herein accurately quantifies both the band gap and the Ga 3d(10) states in LiGaO(2). We derive a band gap of 5.6 eV, and characterize <span class="hlt">electron</span> hybridization in both the valence and conduction bands. Our study of the x-ray spectra may prove useful in analysing spectra from more complicated LiGaO(2) heterostructures. © 2011 IOP Publishing Ltd</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA187296','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA187296"><span><span class="hlt">Electronic</span> <span class="hlt">Structure</span> of Alpha-Quartz and the Influence of Some <span class="hlt">Local</span> Disorder: A Tight Binding Study,</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1977-01-01</p> <p>An s extended summary of the theoretical and ex- perimental work on Si02 is to be found in that paper. The tight-binding basis con- sists of the four... theoretical and experimental works contained therein. 4. B. Fischer, R. A. Pollak, T. H. Distefano and W. D. Grobman, "<span class="hlt">Electronic</span> <span class="hlt">Structure</span> of SiO 2, SixGe 1 x...and GeO 2 from Photoemission Spectroscopy," Phys. Rev. BI5, 3193 (1977), and references to earlier works therein. 5. J. H. Scofield , "Hartree-Slater</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1953k0014B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1953k0014B"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of Ag7GeS5I superionic compound</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bletskan, Dmytro; Studenyak, Ihor; Bletskan, Mykhailo; Vakulchak, Vasyl</p> <p>2018-05-01</p> <p>This paper presents the originally results of ab initio calculations of <span class="hlt">electronic</span> <span class="hlt">structure</span>, total and partial densities of <span class="hlt">electronic</span> states as well as <span class="hlt">electronic</span> charge density distribution of Ag7GeS5I crystal performed within the density functional theory (DFT) in the <span class="hlt">local</span> density approximation (LDA) for exchange-correlation potential. According to performed calculations, Ag7GeS5I is the direct-gap semiconductor with the valence band top and the conductivity band bottom in the Γ point of Brillouin zone. The band gap width calculated in the LDA-approximation is Egd = 0.73 eV. The analysis of total and partial densities of <span class="hlt">electronic</span> states allow us to identify the atomic orbital contributions into the crystal orbitals as well as the formation data of chemical bond in the studied crystal. In the top part of Ag7GeS5I valence band it was revealed the considerable mixing (hybridization) of the occupied d-states of Ag noble metal and the delocalized p-states of sulfur and iodine, which is undoubtedly associated with the covalent character of chemical bond between S, I atoms and noble metal atom.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JPCM...27H3001C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JPCM...27H3001C"><span>Atomic-scale mapping of <span class="hlt">electronic</span> <span class="hlt">structures</span> across heterointerfaces by cross-sectional scanning tunneling microscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chiu, Ya-Ping; Huang, Bo-Chao; Shih, Min-Chuan; Huang, Po-Cheng; Chen, Chun-Wei</p> <p>2015-09-01</p> <p>Interfacial science has received much attention recently based on the development of state-of-the-art analytical tools that can create and manipulate the charge, spin, orbital, and lattice degrees of freedom at interfaces. Motivated by the importance of nanoscale interfacial science that governs device operation, we present a technique to probe the <span class="hlt">electronic</span> characteristics of heterointerfaces with atomic resolution. In this work, the interfacial characteristics of heteroepitaxial <span class="hlt">structures</span> are investigated and the fundamental mechanisms that pertain in these systems are elucidated through cross-sectional scanning tunneling microscopy (XSTM). The XSTM technique is employed here to directly observe epitaxial interfacial <span class="hlt">structures</span> and probe <span class="hlt">local</span> <span class="hlt">electronic</span> properties with atomic-level capability. Scanning tunneling microscopy and spectroscopy experiments with atomic precision provide insight into the origin and spatial distribution of <span class="hlt">electronic</span> properties across heterointerfaces. The first part of this report provides a brief description of the cleavage technique and spectroscopy analysis in XSTM measurements. The second part addresses interfacial <span class="hlt">electronic</span> <span class="hlt">structures</span> of several model heterostructures in current condensed matter research using XSTM. Topics to be discussed include high-κ‘s/III-V’s semiconductors, polymer heterojunctions, and complex oxide heterostructures, which are all material systems whose investigation using this technique is expected to benefit the research community. Finally, practical aspects and perspectives of using XSTM in interface science are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvM...2b5001M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvM...2b5001M"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of lanthanide scandates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mizzi, Christopher A.; Koirala, Pratik; Marks, Laurence D.</p> <p>2018-02-01</p> <p>X-ray photoelectron spectroscopy, ultraviolet photoelectron spectroscopy, and density functional theory calculations were used to study the <span class="hlt">electronic</span> <span class="hlt">structure</span> of three lanthanide scandates: GdSc O3,TbSc O3 , and DySc O3 . X-ray photoelectron spectra simulated from first-principles calculations using a combination of on-site hybrid and GGA +U methods were found to be in good agreement with experimental x-ray photoelectron spectra. The hybrid method was used to model the ground state <span class="hlt">electronic</span> <span class="hlt">structure</span> and the GGA +U method accounted for the shift of valence state energies due to photoelectron emission via a Slater-Janak transition state approach. From these results, the lanthanide scandate valence bands were determined to be composed of Ln 4 f ,O 2 p , and Sc 3 d states, in agreement with previous work. However, contrary to previous work the minority Ln 4 f states were found to be located closer to, and in some cases at, the valence band maximum. This suggests that minority Ln 4 f <span class="hlt">electrons</span> may play a larger role in lanthanide scandate properties than previously thought.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004JChPh.120..845B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004JChPh.120..845B"><span>Measurement and dynamics of the spatial distribution of an <span class="hlt">electron</span> <span class="hlt">localized</span> at a metal-dielectric interface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bezel, Ilya; Gaffney, Kelly J.; Garrett-Roe, Sean; Liu, Simon H.; Miller, André D.; Szymanski, Paul; Harris, Charles B.</p> <p>2004-01-01</p> <p>The ability of time- and angle-resolved two-photon photoemission to estimate the size distribution of <span class="hlt">electron</span> <span class="hlt">localization</span> in the plane of a metal-adsorbate interface is discussed. It is shown that the width of angular distribution of the photoelectric current is inversely proportional to the <span class="hlt">electron</span> <span class="hlt">localization</span> size within the most common approximations in the description of image potential states. The <span class="hlt">localization</span> of the n=1 image potential state for two monolayers of butyronitrile on Ag(111) is used as an example. For the delocalized n=1 state, the shape of the signal amplitude as a function of momentum parallel to the surface changes rapidly with time, indicating efficient intraband relaxation on a 100 fs time scale. For the <span class="hlt">localized</span> state, little change was observed. The latter is related to the constant size distribution of <span class="hlt">electron</span> <span class="hlt">localization</span>, which is estimated to be a Gaussian with a 15±4 Å full width at half maximum in the plane of the interface. A simple model was used to study the effect of a weak <span class="hlt">localization</span> potential on the overall width of the angular distribution of the photoemitted <span class="hlt">electrons</span>, which exhibited little sensitivity to the details of the potential. This substantiates the validity of the <span class="hlt">localization</span> size estimate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ARCMP...9..125C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ARCMP...9..125C"><span>The Key Ingredients of the <span class="hlt">Electronic</span> <span class="hlt">Structure</span> of FeSe</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Coldea, Amalia I.; Watson, Matthew D.</p> <p>2018-03-01</p> <p>FeSe is a fascinating superconducting material at the frontier of research in condensed matter physics. Here, we provide an overview of the current understanding of the <span class="hlt">electronic</span> <span class="hlt">structure</span> of FeSe, focusing in particular on its low-energy <span class="hlt">electronic</span> <span class="hlt">structure</span> as determined from angle-resolved photoemission spectroscopy, quantum oscillations, and magnetotransport measurements of single-crystal samples. We discuss the unique place of FeSe among iron-based superconductors, as it is a multiband system exhibiting strong orbitally dependent <span class="hlt">electronic</span> correlations and unusually small Fermi surfaces and is prone to different <span class="hlt">electronic</span> instabilities. We pay particular attention to the evolution of the <span class="hlt">electronic</span> <span class="hlt">structure</span> that accompanies the tetragonal-orthorhombic <span class="hlt">structural</span> distortion of the lattice around 90 K, which stabilizes a unique nematic <span class="hlt">electronic</span> state. Finally, we discuss how the multiband multiorbital nematic <span class="hlt">electronic</span> <span class="hlt">structure</span> impacts our understanding of the superconductivity, and show that the tunability of the nematic state with chemical and physical pressure helps to disentangle the role of different competing interactions relevant for enhancing superconductivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22617502-non-local-currents-structure-eigenstates-planar-discrete-systems-local-symmetries','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22617502-non-local-currents-structure-eigenstates-planar-discrete-systems-local-symmetries"><span>Non-<span class="hlt">local</span> currents and the <span class="hlt">structure</span> of eigenstates in planar discrete systems with <span class="hlt">local</span> symmetries</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>Röntgen, M., E-mail: mroentge@physnet.uni-hamburg.de; Morfonios, C.V., E-mail: christian.morfonios@physnet.uni-hamburg.de; Diakonos, F.K., E-mail: fdiakono@phys.uoa.gr</p> <p></p> <p><span class="hlt">Local</span> symmetries are spatial symmetries present in a subdomain of a complex system. By using and extending a framework of so-called non-<span class="hlt">local</span> currents that has been established recently, we show that one can gain knowledge about the <span class="hlt">structure</span> of eigenstates in <span class="hlt">locally</span> symmetric setups through a Kirchhoff-type law for the non-<span class="hlt">local</span> currents. The framework is applicable to all discrete planar Schrödinger setups, including those with non-uniform connectivity. Conditions for spatially constant non-<span class="hlt">local</span> currents are derived and we explore two types of <span class="hlt">locally</span> symmetric subsystems in detail, closed-loops and one-dimensional open ended chains. We find these systems to support <span class="hlt">locally</span> similarmore » or even <span class="hlt">locally</span> symmetric eigenstates. - Highlights: • We extend the framework of non-<span class="hlt">local</span> currents to discrete planar systems. • <span class="hlt">Structural</span> information about the eigenstates is gained. • Conditions for the constancy of non-<span class="hlt">local</span> currents are derived. • We use the framework to design two types of example systems featuring <span class="hlt">locally</span> symmetric eigenstates.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8e5125C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8e5125C"><span>First principle study of <span class="hlt">electronic</span> <span class="hlt">structures</span> and optical properties of Ce-doped SiO2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cong, Wei-Yan; Lu, Ying-Bo; Zhang, Peng; Guan, Cheng-Bo</p> <p>2018-05-01</p> <p><span class="hlt">Electronic</span> <span class="hlt">structures</span> and optical properties of Silicon dioxide (SiO2) systems with and without cerium(Ce) dopant were calculated using the density functional theory. We find that after the Ce incorporation, a new <span class="hlt">localized</span> impurity band appears between the valance band maximum (VBM) and the conduction band minimum (CBM) of SiO2 system, which is induced mainly by the Ce-4f orbitals. The <span class="hlt">localized</span> impurity band constructs a bridge between the valence band and the conduction band, making the <span class="hlt">electronic</span> transition much easier. The calculated optical properties show that in contrast from the pure SiO2 sample, absorption in the visible-light region is found in Ce-doped SiO2 system, which originates from the transition between the valence band and Ce-4f dominated impurity band, as well as the <span class="hlt">electronic</span> transition from Ce-4f states to Ce-5d states. All calculated results indicate that Ce doping is an effective strategy to improve the optical performance of SiO2 sample, which is in agreement with the experimental results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SeScT..30g5001M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SeScT..30g5001M"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of germanium selenide investigated using ultra-violet photo-<span class="hlt">electron</span> spectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mishra, P.; Lohani, H.; Kundu, A. K.; Patel, R.; Solanki, G. K.; Menon, Krishnakumar S. R.; Sekhar, B. R.</p> <p>2015-07-01</p> <p>The valence band <span class="hlt">electronic</span> <span class="hlt">structure</span> of GeSe single crystals has been investigated using angle resolved photoemission spectroscopy (ARPES) and x-ray photoelectron spectroscopy. The experimentally observed bands from ARPES, match qualitatively with our LDA-based band <span class="hlt">structure</span> calculations along the Γ-Z, Γ-Y and Γ-T symmetry directions. The valence band maximum occurs nearly midway along the Γ-Z direction, at a binding energy of -0.5 eV, substantiating the indirect band gap of GeSe. Non-dispersive features associated with surface states and indirect transitions have been observed. The difference in hybridization of Se and Ge 4p orbitals leads to the variation of dispersion along the three symmetry directions. The predominance of the Se 4pz orbitals, evidenced from theoretical calculations, may be the cause for highly dispersive bands along the Γ-T direction. Detailed <span class="hlt">electronic</span> <span class="hlt">structure</span> analysis reveals the significance of the cation-anion 4p orbitals hybridization in the valence band dispersion of IV-VI semiconductors. This is the first comprehensive report of the <span class="hlt">electronic</span> <span class="hlt">structure</span> of a GeSe single crystal using ARPES in conjugation with theoretical band <span class="hlt">structure</span> analysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1409754-local-structure-model-network-analysis','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1409754-local-structure-model-network-analysis"><span>A <span class="hlt">local</span> <span class="hlt">structure</span> model for network analysis</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Casleton, Emily; Nordman, Daniel; Kaiser, Mark</p> <p>2017-04-01</p> <p>The statistical analysis of networks is a popular research topic with ever widening applications. Exponential random graph models (ERGMs), which specify a model through interpretable, global network features, are common for this purpose. In this study we introduce a new class of models for network analysis, called <span class="hlt">local</span> <span class="hlt">structure</span> graph models (LSGMs). In contrast to an ERGM, a LSGM specifies a network model through <span class="hlt">local</span> features and allows for an interpretable and controllable <span class="hlt">local</span> dependence <span class="hlt">structure</span>. In particular, LSGMs are formulated by a set of full conditional distributions for each network edge, e.g., the probability of edge presence/absence, depending onmore » neighborhoods of other edges. Additional model features are introduced to aid in specification and to help alleviate a common issue (occurring also with ERGMs) of model degeneracy. Finally, the proposed models are demonstrated on a network of tornadoes in Arkansas where a LSGM is shown to perform significantly better than a model without <span class="hlt">local</span> dependence.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1409754','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1409754"><span>A <span class="hlt">local</span> <span class="hlt">structure</span> model for network analysis</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>Casleton, Emily; Nordman, Daniel; Kaiser, Mark</p> <p></p> <p>The statistical analysis of networks is a popular research topic with ever widening applications. Exponential random graph models (ERGMs), which specify a model through interpretable, global network features, are common for this purpose. In this study we introduce a new class of models for network analysis, called <span class="hlt">local</span> <span class="hlt">structure</span> graph models (LSGMs). In contrast to an ERGM, a LSGM specifies a network model through <span class="hlt">local</span> features and allows for an interpretable and controllable <span class="hlt">local</span> dependence <span class="hlt">structure</span>. In particular, LSGMs are formulated by a set of full conditional distributions for each network edge, e.g., the probability of edge presence/absence, depending onmore » neighborhoods of other edges. Additional model features are introduced to aid in specification and to help alleviate a common issue (occurring also with ERGMs) of model degeneracy. Finally, the proposed models are demonstrated on a network of tornadoes in Arkansas where a LSGM is shown to perform significantly better than a model without <span class="hlt">local</span> dependence.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4661528','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4661528"><span>Orbital-dependent <span class="hlt">Electron</span>-Hole Interaction in Graphene and Associated Multi-Layer <span class="hlt">Structures</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>Deng, Tianqi; Su, Haibin</p> <p>2015-01-01</p> <p>We develop an orbital-dependent potential to describe <span class="hlt">electron</span>-hole interaction in materials with <span class="hlt">structural</span> 2D character, i.e. quasi-2D materials. The modulated orbital-dependent potentials are also constructed with non-<span class="hlt">local</span> screening, multi-layer screening, and finite gap due to the coupling with substrates. We apply the excitonic Hamiltonian in coordinate-space with developed effective <span class="hlt">electron</span>-hole interacting potentials to compute excitons’ binding strength at M (π band) and Γ (σ band) points in graphene and its associated multi-layer forms. The orbital-dependent potential provides a range-separated property for regulating both long- and short-range interactions. This accounts for the existence of the resonant π exciton in single- and bi-layer graphenes. The remarkable strong <span class="hlt">electron</span>-hole interaction in σ orbitals plays a decisive role in the existence of σ exciton in graphene stack at room temperature. The interplay between gap-opening and screening from substrates shed a light on the weak dependence of σ exciton binding energy on the thickness of graphene stacks. Moreover, the analysis of non-hydrogenic exciton spectrum in quasi-2D systems clearly demonstrates the remarkable comparable contribution of orbital dependent potential with respect to non-<span class="hlt">local</span> screening process. The understanding of orbital-dependent potential developed in this work is potentially applicable for a wide range of materials with low dimension. PMID:26610715</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21715662','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21715662"><span><span class="hlt">Localization</span> of <span class="hlt">electrons</span> due to orbitally ordered bi-stripes in the bilayer manganite La(2-2x)Sr(1+2x)Mn2O7 (x ~ 0.59).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sun, Z; Wang, Q; Fedorov, A V; Zheng, H; Mitchell, J F; Dessau, D S</p> <p>2011-07-19</p> <p><span class="hlt">Electronic</span> phases with stripe patterns have been intensively investigated for their vital roles in unique properties of correlated <span class="hlt">electronic</span> materials. How these real-space patterns affect the conductivity and other properties of materials (which are usually described in momentum space) is one of the major challenges of modern condensed matter physics. By studying the <span class="hlt">electronic</span> <span class="hlt">structure</span> of La(2-2x)Sr(1+2x)Mn(2)O(7) (x ∼ 0.59) and in combination with earlier scattering measurements, we demonstrate the variation of <span class="hlt">electronic</span> properties accompanying the melting of so-called bi-stripes in this material. The static bi-stripes can strongly <span class="hlt">localize</span> the <span class="hlt">electrons</span> in the insulating phase above T(c) ∼ 160 K, while the fraction of mobile <span class="hlt">electrons</span> grows, coexisting with a significant portion of <span class="hlt">localized</span> <span class="hlt">electrons</span> when the static bi-stripes melt below T(c). The presence of <span class="hlt">localized</span> <span class="hlt">electrons</span> below T(c) suggests that the melting bi-stripes exist as a disordered or fluctuating counterpart. From static to melting, the bi-stripes act as an atomic-scale <span class="hlt">electronic</span> valve, leading to a "colossal" metal-insulator transition in this material.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5059764','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5059764"><span>Nanoscale probing of <span class="hlt">electron</span>-regulated <span class="hlt">structural</span> transitions in silk proteins by near-field IR imaging and nano-spectroscopy</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Qin, Nan; Zhang, Shaoqing; Jiang, Jianjuan; Corder, Stephanie Gilbert; Qian, Zhigang; Zhou, Zhitao; Lee, Woonsoo; Liu, Keyin; Wang, Xiaohan; Li, Xinxin; Shi, Zhifeng; Mao, Ying; Bechtel, Hans A.; Martin, Michael C.; Xia, Xiaoxia; Marelli, Benedetto; Kaplan, David L.; Omenetto, Fiorenzo G.; Liu, Mengkun; Tao, Tiger H.</p> <p>2016-01-01</p> <p>Silk protein fibres produced by silkworms and spiders are renowned for their unparalleled mechanical strength and extensibility arising from their high-β-sheet crystal contents as natural materials. Investigation of β-sheet-oriented conformational transitions in silk proteins at the nanoscale remains a challenge using conventional imaging techniques given their limitations in chemical sensitivity or limited spatial resolution. Here, we report on <span class="hlt">electron</span>-regulated nanoscale polymorphic transitions in silk proteins revealed by near-field infrared imaging and nano-spectroscopy at resolutions approaching the molecular level. The ability to <span class="hlt">locally</span> probe nanoscale protein <span class="hlt">structural</span> transitions combined with nanometre-precision <span class="hlt">electron</span>-beam lithography offers us the capability to finely control the <span class="hlt">structure</span> of silk proteins in two and three dimensions. Our work paves the way for unlocking essential nanoscopic protein <span class="hlt">structures</span> and critical conditions for <span class="hlt">electron</span>-induced conformational transitions, offering new rules to design protein-based nanoarchitectures. PMID:27713412</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/919475','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/919475"><span><span class="hlt">Local</span> Quark-Hadron Duality in <span class="hlt">Electron</span> Scattering</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>Wally Melnitchouk</p> <p>2007-09-10</p> <p>We present some recent developments in the study of quark-hadron duality in <span class="hlt">structure</span> functions in the resonance region. To understand the workings of <span class="hlt">local</span> duality we introduce the concept of truncated moments, which are used to describe the Q^2 dependence of specific resonance regions within a QCD framework.</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/2015APS..MARJ15001H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..MARJ15001H"><span><span class="hlt">Electron</span> and hole dynamics in the <span class="hlt">electronic</span> and <span class="hlt">structural</span> phase transitions of VO2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haglund, Richard</p> <p>2015-03-01</p> <p>The ultrafast, optically induced insulator-to-metal transition (IMT) and the associated <span class="hlt">structural</span> phase transition (SPT) in vanadium dioxide (VO2) have been studied for over a decade. However, only recently have effects due to the combined presence of <span class="hlt">electron</span>-hole pairs and injected <span class="hlt">electrons</span> been observed. Here we compare and contrast IMT dynamics when both hot <span class="hlt">electrons</span> and optically excited <span class="hlt">electron</span>-hole pairs are involved, in (1) thin films of VO2 overlaid by a thin gold foil, in which hot <span class="hlt">electrons</span> are generated by 1.5 eV photons absorbed in the foil and accelerated through the VO2 by an applied electric field; (2) VO2 nanoparticles covered with a sparse mesh of gold nanoparticles averaging 20-30 nm in diameter in which hot <span class="hlt">electrons</span> are generated by resonant excitation and decay of the <span class="hlt">localized</span> surface plasmon; and (3) bare VO2 thin films excited by intense near-single-cycle THz pulses. In the first case, the IMT is driven by excitation of the bulk gold plasmon, and the SPT appears on a few-picosecond time scale. In the second case, density-functional calculations indicate that above a critical carrier density, the addition of a single <span class="hlt">electron</span> to a 27-unit supercell drives the catastrophic collapse of the coherent phonon associated with, and leading to, the SPT. In the third case, sub-bandgap-energy photons (approximately 0.1 eV) initiate the IMT, but exhibit the same sub-100 femtosecond switching time and coherent phonon dynamics as observed when the IMT is initiated by 1.5 eV photons. This suggests that the underlying mechanism must be quite different, possibly THz-field induced interband tunneling of spatially separated <span class="hlt">electron</span>-hole pairs. The implications of these findings for ultrafast switching in opto-<span class="hlt">electronic</span> devices - such as hybrid VO2 silicon ring resonators - are briefly considered. Support from the National Science Foundation (DMR-1207407), the Office of Science, U.S. Department of Energy (DE-FG02-01ER45916) and the Defense Threat</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18579771','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18579771"><span>A generative, probabilistic model of <span class="hlt">local</span> protein <span class="hlt">structure</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Boomsma, Wouter; Mardia, Kanti V; Taylor, Charles C; Ferkinghoff-Borg, Jesper; Krogh, Anders; Hamelryck, Thomas</p> <p>2008-07-01</p> <p>Despite significant progress in recent years, protein <span class="hlt">structure</span> prediction maintains its status as one of the prime unsolved problems in computational biology. One of the key remaining challenges is an efficient probabilistic exploration of the <span class="hlt">structural</span> space that correctly reflects the relative conformational stabilities. Here, we present a fully probabilistic, continuous model of <span class="hlt">local</span> protein <span class="hlt">structure</span> in atomic detail. The generative model makes efficient conformational sampling possible and provides a framework for the rigorous analysis of <span class="hlt">local</span> sequence-<span class="hlt">structure</span> correlations in the native state. Our method represents a significant theoretical and practical improvement over the widely used fragment assembly technique by avoiding the drawbacks associated with a discrete and nonprobabilistic approach.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4060508','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4060508"><span><span class="hlt">Structure</span> of <span class="hlt">local</span> interactions in complex financial dynamics</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Jiang, X. F.; Chen, T. T.; Zheng, B.</p> <p>2014-01-01</p> <p>With the network methods and random matrix theory, we investigate the interaction <span class="hlt">structure</span> of communities in financial markets. In particular, based on the random matrix decomposition, we clarify that the <span class="hlt">local</span> interactions between the business sectors (subsectors) are mainly contained in the sector mode. In the sector mode, the average correlation inside the sectors is positive, while that between the sectors is negative. Further, we explore the time evolution of the interaction <span class="hlt">structure</span> of the business sectors, and observe that the <span class="hlt">local</span> interaction <span class="hlt">structure</span> changes dramatically during a financial bubble or crisis. PMID:24936906</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JChPh.147h4101H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JChPh.147h4101H"><span>Pair 2-<span class="hlt">electron</span> reduced density matrix theory using <span class="hlt">localized</span> orbitals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Head-Marsden, Kade; Mazziotti, David A.</p> <p>2017-08-01</p> <p>Full configuration interaction (FCI) restricted to a pairing space yields size-extensive correlation energies but its cost scales exponentially with molecular size. Restricting the variational two-<span class="hlt">electron</span> reduced-density-matrix (2-RDM) method to represent the same pairing space yields an accurate lower bound to the pair FCI energy at a mean-field-like computational scaling of O (r3) where r is the number of orbitals. In this paper, we show that <span class="hlt">localized</span> molecular orbitals can be employed to generate an efficient, approximately size-extensive pair 2-RDM method. The use of <span class="hlt">localized</span> orbitals eliminates the substantial cost of optimizing iteratively the orbitals defining the pairing space without compromising accuracy. In contrast to the <span class="hlt">localized</span> orbitals, the use of canonical Hartree-Fock molecular orbitals is shown to be both inaccurate and non-size-extensive. The pair 2-RDM has the flexibility to describe the spectra of one-<span class="hlt">electron</span> RDM occupation numbers from all quantum states that are invariant to time-reversal symmetry. Applications are made to hydrogen chains and their dissociation, n-acene from naphthalene through octacene, and cadmium telluride 2-, 3-, and 4-unit polymers. For the hydrogen chains, the pair 2-RDM method recovers the majority of the energy obtained from similar calculations that iteratively optimize the orbitals. The <span class="hlt">localized</span>-orbital pair 2-RDM method with its mean-field-like computational scaling and its ability to describe multi-reference correlation has important applications to a range of strongly correlated phenomena in chemistry and physics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22299632-electronic-structures-gesi-nanoislands-grown-pit-patterned-si-substrate','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22299632-electronic-structures-gesi-nanoislands-grown-pit-patterned-si-substrate"><span><span class="hlt">Electronic</span> <span class="hlt">structures</span> of GeSi nanoislands grown on pit-patterned Si(001) substrate</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>Ye, Han, E-mail: Dabombyh@aliyun.com; Yu, Zhongyuan</p> <p>2014-11-15</p> <p>Patterning pit on Si(001) substrate prior to Ge deposition is an important approach to achieve GeSi nanoislands with high ordering and size uniformity. In present work, the <span class="hlt">electronic</span> <span class="hlt">structures</span> of realistic uncapped pyramid, dome, barn and cupola nanoislands grown in (105) pits are systematically investigated by solving Schrödinger equation for heavy-hole, which resorts to inhomogeneous strain distribution and nonlinear composition-dependent band parameters. Uniform, partitioned and equilibrium composition profile (CP) in nanoisland and inverted pyramid <span class="hlt">structure</span> are simulated separately. We demonstrate the huge impact of composition profile on <span class="hlt">localization</span> of heavy-hole: wave function of ground state is confined near pit facetsmore » for uniform CP, at bottom of nanoisland for partitioned CP and at top of nanoisland for equilibrium CP. Moreover, such <span class="hlt">localization</span> is gradually compromised by the size effect as pit filling ratio or pit size decreases. The results pave the fundamental guideline of designing nanoislands on pit-patterned substrates for desired applications.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ChPhB..23g7301T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ChPhB..23g7301T"><span>Lattice <span class="hlt">structures</span> and <span class="hlt">electronic</span> properties of CIGS/CdS interface: First-principles calculations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tang, Fu-Ling; Liu, Ran; Xue, Hong-Tao; Lu, Wen-Jiang; Feng, Yu-Dong; Rui, Zhi-Yuan; Huang, Min</p> <p>2014-07-01</p> <p>Using first-principles calculations within density functional theory, we study the atomic <span class="hlt">structures</span> and <span class="hlt">electronic</span> properties of the perfect and defective (2VCu+InCu) CuInGaSe2/CdS interfaces theoretically, especially the interface states. We find that the <span class="hlt">local</span> lattice <span class="hlt">structure</span> of (2VCu+InCu) interface is somewhat disorganized. By analyzing the <span class="hlt">local</span> density of states projected on several atomic layers of the two interfaces models, we find that for the (2VCu+InCu) interface the interface states near the Fermi level in CuInGaSe2 and CdS band gap regions are mainly composed of interfacial Se-4p, Cu-3d and S-3p orbitals, while for the perfect interface there are no clear interface states in the CuInGaSe2 region but only some interface states which are mainly composed of S-3p orbitals in the valance band of CdS region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JEMat..47.3277P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JEMat..47.3277P"><span><span class="hlt">Electronic</span> <span class="hlt">Structure</span> and Thermoelectric Properties of Transition Metal Monosilicides</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pshenay-Severin, D. A.; Ivanov, Yu. V.; Burkov, A. T.; Novikov, S. V.; Zaitsev, V. K.; Reith, H.</p> <p>2018-06-01</p> <p>We present theoretical and experimental results on <span class="hlt">electronic</span> <span class="hlt">structure</span> and thermoelectric properties of cobalt monosilicide (CoSi) and of Co1- x M x Si diluted alloys (M = Fe and Ni) at temperatures from 2 K to 800 K. CoSi crystallizes into a non-centrosymmetric cubic B20 <span class="hlt">structure</span>, which suggests the possibility of a topologically non-trivial <span class="hlt">electronic</span> <span class="hlt">structure</span>. We show that the <span class="hlt">electronic</span> <span class="hlt">structure</span> of CoSi exhibits linear band crossings in close vicinity to Fermi energy, confirming the possibility of non-trivial topology. The proximity of the linear-dispersion bands to Fermi energy implies their important contribution to the <span class="hlt">electronic</span> transport. Calculation of thermopower of CoSi, using ab initio band <span class="hlt">structure</span> and the constant relaxation time approximation, is carried out. It reveals that many body corrections to the <span class="hlt">electronic</span> spectrum are important in order to obtain qualitative agreement of theoretical and experimental temperature dependences of thermopower. Phonon dispersion and lattice thermal conductivity are calculated. The phonons give a major contribution to the thermal conductivity of the compound below room temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28655846','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28655846"><span><span class="hlt">Local</span> thermal energy as a <span class="hlt">structural</span> indicator in glasses.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zylberg, Jacques; Lerner, Edan; Bar-Sinai, Yohai; Bouchbinder, Eran</p> <p>2017-07-11</p> <p>Identifying heterogeneous <span class="hlt">structures</span> in glasses-such as <span class="hlt">localized</span> soft spots-and understanding <span class="hlt">structure</span>-dynamics relations in these systems remain major scientific challenges. Here, we derive an exact expression for the <span class="hlt">local</span> thermal energy of interacting particles (the mean <span class="hlt">local</span> potential energy change caused by thermal fluctuations) in glassy systems by a systematic low-temperature expansion. We show that the <span class="hlt">local</span> thermal energy can attain anomalously large values, inversely related to the degree of softness of <span class="hlt">localized</span> <span class="hlt">structures</span> in a glass, determined by a coupling between internal stresses-an intrinsic signature of glassy frustration-anharmonicity and low-frequency vibrational modes. These anomalously large values follow a fat-tailed distribution, with a universal exponent related to the recently observed universal [Formula: see text] density of states of quasilocalized low-frequency vibrational modes. When the spatial thermal energy field-a "softness field"-is considered, this power law tail manifests itself by highly <span class="hlt">localized</span> spots, which are significantly softer than their surroundings. These soft spots are shown to be susceptible to plastic rearrangements under external driving forces, having predictive powers that surpass those of the normal modes-based approach. These results offer a general, system/model-independent, physical/observable-based approach to identify <span class="hlt">structural</span> properties of quiescent glasses and relate them to glassy dynamics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA243633','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA243633"><span>A Cache Design to Exploit <span class="hlt">Structural</span> <span class="hlt">Locality</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1991-12-01</p> <p>memory and secondary storage. Main memory was used to store the instructions and data of an executing pro- gram, while secondary storage held programs ...efficiency of the CPU and faster turnaround of executing programs . In addition to the well known spatial and temporal aspects of <span class="hlt">locality</span>, Hobart has...identified a third aspect, which he has called <span class="hlt">structural</span> <span class="hlt">locality</span> (9). This type of <span class="hlt">locality</span> is defined as the tendency of an executing program to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1405938-correlations-between-transition-metal-chemistry-local-structure-global-structure-li2ru0-investigated-wide-voltage-window','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1405938-correlations-between-transition-metal-chemistry-local-structure-global-structure-li2ru0-investigated-wide-voltage-window"><span>Correlations between Transition Metal Chemistry, <span class="hlt">Local</span> <span class="hlt">Structure</span> and Global <span class="hlt">Structure</span> in Li 2Ru 0.5Mn 0.5O 3 Investigated in a Wide Voltage Window</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Lyu, Yingchun; Hu, Enyuan; Xiao, Dongdong; ...</p> <p>2017-10-20</p> <p>Li 2Ru 0.5Mn 0.5O 3, a high capacity lithium rich layered cathode material for lithium-ion batteries, was subject to comprehen-sive diagnostic studies including in situ/ex situ X-ray diffraction (XRD), X-ray absorption spectroscopy (XAS), pair distribu-tion function (PDF) and high resolution scanning transmission <span class="hlt">electron</span> microscopy (STEM) analysis, to understand the cor-relations between transition metal chemistry, <span class="hlt">structure</span> and lithium storage electrochemical behavior. Ru-Ru dimers have been identified in the as-prepared sample and found to be preserved upon prolonged cycling. Presence of these dimers, which are likely caused by the delocalized nature of 4d <span class="hlt">electrons</span>, is found to favor the stabilization of themore » <span class="hlt">structure</span> in a lay-ered phase. The in situ XAS results confirm the participation of oxygen redox into the charge compensation at high charge voltage, and the great flexibility of the covalent bond between Ru and O may provide great reversibility of the global <span class="hlt">struc-ture</span> despite of the significant <span class="hlt">local</span> distortion around Ru. In contrast, the <span class="hlt">local</span> distortion around Mn occurs at low discharge voltage and is accompanied by a “layered to 1T” phase transformation, which is found to be detrimental to the cycle per-formances. It is clear that the changes of <span class="hlt">local</span> <span class="hlt">structure</span> around individual transition metal cations respond separately and differently to lithium intercalation/deintercalation. Here, cations with the capability to tolerate the lattice distortion will benefit for maintaining the integrality of the crystal <span class="hlt">structure</span> and therefore is able to enhance the long-term cycling performance of the electrode materials.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1405938-correlations-between-transition-metal-chemistry-local-structure-global-structure-li2ru0-investigated-wide-voltage-window','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1405938-correlations-between-transition-metal-chemistry-local-structure-global-structure-li2ru0-investigated-wide-voltage-window"><span>Correlations between Transition Metal Chemistry, <span class="hlt">Local</span> <span class="hlt">Structure</span> and Global <span class="hlt">Structure</span> in Li 2Ru 0.5Mn 0.5O 3 Investigated in a Wide Voltage Window</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>Lyu, Yingchun; Hu, Enyuan; Xiao, Dongdong</p> <p></p> <p>Li 2Ru 0.5Mn 0.5O 3, a high capacity lithium rich layered cathode material for lithium-ion batteries, was subject to comprehen-sive diagnostic studies including in situ/ex situ X-ray diffraction (XRD), X-ray absorption spectroscopy (XAS), pair distribu-tion function (PDF) and high resolution scanning transmission <span class="hlt">electron</span> microscopy (STEM) analysis, to understand the cor-relations between transition metal chemistry, <span class="hlt">structure</span> and lithium storage electrochemical behavior. Ru-Ru dimers have been identified in the as-prepared sample and found to be preserved upon prolonged cycling. Presence of these dimers, which are likely caused by the delocalized nature of 4d <span class="hlt">electrons</span>, is found to favor the stabilization of themore » <span class="hlt">structure</span> in a lay-ered phase. The in situ XAS results confirm the participation of oxygen redox into the charge compensation at high charge voltage, and the great flexibility of the covalent bond between Ru and O may provide great reversibility of the global <span class="hlt">struc-ture</span> despite of the significant <span class="hlt">local</span> distortion around Ru. In contrast, the <span class="hlt">local</span> distortion around Mn occurs at low discharge voltage and is accompanied by a “layered to 1T” phase transformation, which is found to be detrimental to the cycle per-formances. It is clear that the changes of <span class="hlt">local</span> <span class="hlt">structure</span> around individual transition metal cations respond separately and differently to lithium intercalation/deintercalation. Here, cations with the capability to tolerate the lattice distortion will benefit for maintaining the integrality of the crystal <span class="hlt">structure</span> and therefore is able to enhance the long-term cycling performance of the electrode materials.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/ED368335.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/ED368335.pdf"><span><span class="hlt">Electronic</span> Document Imaging and Optical Storage Systems for <span class="hlt">Local</span> Governments: An Introduction. <span class="hlt">Local</span> Government Records Technical Information Series. Number 21.</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>Schwartz, Stanley F.</p> <p></p> <p>This publication introduces <span class="hlt">electronic</span> document imaging systems and provides guidance for <span class="hlt">local</span> governments in New York in deciding whether such systems should be adopted for their own records and information management purposes. It advises <span class="hlt">local</span> governments on how to develop plans for using such technology by discussing its advantages and…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRA..123.3919D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRA..123.3919D"><span>Shapes of Magnetically Controlled <span class="hlt">Electron</span> Density <span class="hlt">Structures</span> in the Dayside Martian Ionosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Diéval, C.; Kopf, A. J.; Wild, J. A.</p> <p>2018-05-01</p> <p>Nonhorizontal <span class="hlt">localized</span> <span class="hlt">electron</span> density <span class="hlt">structures</span> associated with regions of near-radial crustal magnetic fields are routinely detected via radar oblique echoes on the dayside of Mars with the ionospheric sounding mode of the Mars Advanced Radar for Subsurface and Ionospheric Sounding (MARSIS) radar onboard Mars Express. Previous studies mostly investigated these <span class="hlt">structures</span> at a fixed plasma frequency and assumed that the larger apparent altitude of the <span class="hlt">structures</span> compared to the normal surrounding ionosphere implied that they are bulges. However, the signal is subjected to dispersion when it propagates through the plasma, so interpretations based on the apparent altitude should be treated with caution. We go further by investigating the frequency dependence (i.e., the altitude dependence) of the shape of 48 density <span class="hlt">structure</span> events, using time series of MARSIS <span class="hlt">electron</span> density profiles corrected for signal dispersion. Four possible simplest shapes are detected in these time series, which can give oblique echoes: bulges, dips, downhill slopes, and uphill slopes. The altitude differences between the density <span class="hlt">structures</span> and their edges are, in absolute value, larger at low frequency (high altitude) than at high frequency (low altitude), going from a few tens of kilometers to a few kilometers as frequency increases. Bulges dominate in numbers in most of the frequency range. Finally, the geographical extension of the density <span class="hlt">structures</span> covers a wide range of crustal magnetic fields orientations, with near-vertical fields toward their center and near-horizontal fields toward their edges, as expected. Transport processes are suggested to be a key driver for these density <span class="hlt">structures</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007PhRvB..75g3411X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007PhRvB..75g3411X"><span>Phonon-induced <span class="hlt">localization</span> of <span class="hlt">electron</span> states in quasi-one-dimensional systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xiong, Ye</p> <p>2007-02-01</p> <p>It is shown that hot phonons with random phases can cause <span class="hlt">localization</span> of <span class="hlt">electron</span> states in quasi-one-dimensional systems. Owing to the nature of long-range correlation of the disorder induced by phonons, only the states at edges of one-dimensional (1D) subbands are <span class="hlt">localized</span>, and the states inside the 1D subbands are still extended. As a result, the conductance exhibits gradual quantum steps in varying the gate potential. By increasing the temperature the degree of <span class="hlt">localization</span> increases. In the <span class="hlt">localization</span> regime the distribution of Lyapunov exponent (LE) is Gaussian and the relation of the mean-value and standard variance of LE to the system size obeys the single-parameter hypothesis. The mean value of LE can be used as an order parameter to distinguish the <span class="hlt">local</span> and extended states.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22415944-local-structure-solid-rb-megabar-pressures','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22415944-local-structure-solid-rb-megabar-pressures"><span><span class="hlt">Local</span> <span class="hlt">structure</span> of solid Rb at megabar pressures</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>De Panfilis, S.; Gorelli, F.; Santoro, M.</p> <p>2015-06-07</p> <p>We have investigated the <span class="hlt">local</span> and <span class="hlt">electronic</span> <span class="hlt">structure</span> of solid rubidium by means of x-ray absorption spectroscopy up to 101.0 GPa, thus doubling the maximum investigated experimental pressure. This study confirms the predicted stability of phase VI and was completed by the combination of two pivotal instrumental solutions. On one side, we made use of nanocrystalline diamond anvils, which, contrary to the more commonly used single crystal diamond anvils, do not generate sharp Bragg peaks (glitches) at specific energies that spoil the weak fine <span class="hlt">structure</span> oscillations in the x-ray absorption cross section. Second, we exploited the performance of a state-of-the-artmore » x-ray focussing device yielding a beam spot size of 5 × 5 μm{sup 2}, spatially stable over the entire energy scan. An advanced data analysis protocol was implemented to extract the pressure dependence of the <span class="hlt">structural</span> parameters in phase VI of solid Rb from 51.2 GPa up to the highest pressure. A continuous reduction of the nearest neighbour distances was observed, reaching about 6% over the probed pressure range. We also discuss a phenomenological model based on the Einstein approximation to describe the pressure behaviour of the mean-square relative displacement. Within this simplified scheme, we estimate the Grüneisen parameter for this high pressure Rb phase to be in the 1.3–1.5 interval.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPS...342...56Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPS...342...56Z"><span>Investigation of <span class="hlt">electronic</span> and <span class="hlt">local</span> <span class="hlt">structural</span> changes during lithium uptake and release of nano-crystalline NiFe2O4 by X-ray absorption spectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhou, Dong; Permien, Stefan; Rana, Jatinkumar; Krengel, Markus; Sun, Fu; Schumacher, Gerhard; Bensch, Wolfgang; Banhart, John</p> <p>2017-02-01</p> <p>Nano-crystalline NiFe2O4 particles were synthesized and used as active electrode material for a lithium ion battery that showed a high discharge capacity of 1534 mAh g-1 and charge capacity of 1170 mAh g-1 during the 1st cycle. X-ray absorption spectroscopy including XANES and EXAFS were used to investigate <span class="hlt">electronic</span> and <span class="hlt">local</span> <span class="hlt">structural</span> changes of NiFe2O4 during the 1st lithiation and de-lithiation process. As lithium is inserted into the <span class="hlt">structure</span>, tetrahedral site Fe3+ ions are reduced to Fe2+ and moved from tetrahedral sites to empty octahedral sites, while Ni2+ ions are unaffected. As a consequence, the matrix spinel <span class="hlt">structure</span> collapses and transforms to an intermediate rock-salt monoxide phase. Meanwhile, the inserted Li is partially consumed by the formation of SEI and other side reactions during the conversion reaction. With further lithiation, the monoxide phase is reduced to highly disordered metallic Fe/Ni nanoparticles with a number of nearest neighbors of 6.0(8) and 8.1(4) for Fe and Ni, respectively. During subsequent de-lithiation, the metal particles are individually re-oxidized to Fe2O3 and NiO phases instead to the original NiFe2O4 spinel phase.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ChPhL..31c7101X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ChPhL..31c7101X"><span>The <span class="hlt">Electronic</span> <span class="hlt">Structure</span> and Formation Energies of Ni-doped CuAlO2 by Density Functional Theory Calculation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Ying; Li, Fei; Sheng, Wei; Nie, Guo-Zheng; Yuan, Ding-Wang</p> <p>2014-03-01</p> <p>The <span class="hlt">electronic</span> <span class="hlt">structure</span> and formation energies of Ni-doped CuAlO2 are calculated by first-principles calculations. Our results show that Ni is good for p-type doping in CuAlO2. When Ni is doped into CuAlO2, it prefers to substitute Al-site. NiAl is a shallow acceptor, while NiCu is a deep acceptor and its formation energy is high. Further <span class="hlt">electronic</span> <span class="hlt">structure</span> calculations show that strong hybridization happens between Ni-3d and O-2p states for Ni substituting Al-site, while <span class="hlt">localized</span> Ni-3d states are found for Ni substituting Cu-site.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21446666','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21446666"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> and normal vibrations of the 1-ethyl-3-methylimidazolium ethyl sulfate ion pair.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dhumal, Nilesh R; Kim, Hyung J; Kiefer, Johannes</p> <p>2011-04-21</p> <p><span class="hlt">Electronic</span> and <span class="hlt">structural</span> properties of the ion pair 1-ethyl-3-methylimidazolium ethyl sulfate are studied using density functional methods. Three <span class="hlt">locally</span> stable conformers of the ion pair complex are considered to analyze molecular interactions between its cation and anion. Manifestations of these interactions in the vibrational spectra are discussed and compared with experimental IR and Raman spectroscopy data. NBO analysis and difference <span class="hlt">electron</span> density coupled with molecular <span class="hlt">electron</span> density topography are used to interpret the frequency shifts of the normal vibrations of the ion pair, compared to the free anion and cation. Excitation energies of low-lying singlet excited states of the conformers are also studied. The density functional theory results are found to be in a reasonable agreement with experimental UV/vis absorption spectra.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPCM...30o5303W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPCM...30o5303W"><span>Exploring the formation and <span class="hlt">electronic</span> <span class="hlt">structure</span> properties of the g-C3N4 nanoribbon with density functional theory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, Hong-Zhang; Zhong, Qing-Hua; Bandaru, Sateesh; Liu, Jin; Lau, Woon Ming; Li, Li-Li; Wang, Zhenling</p> <p>2018-04-01</p> <p>The optical properties and condensation degree (<span class="hlt">structure</span>) of polymeric g-C3N4 depend strongly on the process temperature. For polymeric g-C3N4, its <span class="hlt">structure</span> and condensation degree depend on the <span class="hlt">structure</span> of molecular strand(s). Here, the formation and <span class="hlt">electronic</span> <span class="hlt">structure</span> properties of the g-C3N4 nanoribbon are investigated by studying the polymerization and crystallinity of molecular strand(s) employing first-principle density functional theory. The calculations show that the width of the molecular strand has a significant effect on the <span class="hlt">electronic</span> <span class="hlt">structure</span> of polymerized and crystallized g-C3N4 nanoribbons, a conclusion which would be indirect evidence that the <span class="hlt">electronic</span> <span class="hlt">structure</span> depends on the <span class="hlt">structure</span> of g-C3N4. The edge shape also has a distinct effect on the <span class="hlt">electronic</span> <span class="hlt">structure</span> of the crystallized g-C3N4 nanoribbon. Furthermore, the conductive band minimum and valence band maximum of the polymeric g-C3N4 nanoribbon show a strong <span class="hlt">localization</span>, which is in good agreement with the quasi-monomer characters. In addition, molecular strands prefer to grow along the planar direction on graphene. These results provide new insight on the properties of the g-C3N4 nanoribbon and the relationship between the <span class="hlt">structure</span> and properties of g-C3N4.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29488471','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29488471"><span>Exploring the formation and <span class="hlt">electronic</span> <span class="hlt">structure</span> properties of the g-C3N4 nanoribbon with density functional theory.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wu, Hong-Zhang; Zhong, Qing-Hua; Bandaru, Sateesh; Liu, Jin; Lau, Woon Ming; Li, Li-Li; Wang, Zhenling</p> <p>2018-04-18</p> <p>The optical properties and condensation degree (<span class="hlt">structure</span>) of polymeric g-C 3 N 4 depend strongly on the process temperature. For polymeric g-C 3 N 4 , its <span class="hlt">structure</span> and condensation degree depend on the <span class="hlt">structure</span> of molecular strand(s). Here, the formation and <span class="hlt">electronic</span> <span class="hlt">structure</span> properties of the g-C 3 N 4 nanoribbon are investigated by studying the polymerization and crystallinity of molecular strand(s) employing first-principle density functional theory. The calculations show that the width of the molecular strand has a significant effect on the <span class="hlt">electronic</span> <span class="hlt">structure</span> of polymerized and crystallized g-C 3 N 4 nanoribbons, a conclusion which would be indirect evidence that the <span class="hlt">electronic</span> <span class="hlt">structure</span> depends on the <span class="hlt">structure</span> of g-C 3 N 4 . The edge shape also has a distinct effect on the <span class="hlt">electronic</span> <span class="hlt">structure</span> of the crystallized g-C 3 N 4 nanoribbon. Furthermore, the conductive band minimum and valence band maximum of the polymeric g-C 3 N 4 nanoribbon show a strong <span class="hlt">localization</span>, which is in good agreement with the quasi-monomer characters. In addition, molecular strands prefer to grow along the planar direction on graphene. These results provide new insight on the properties of the g-C 3 N 4 nanoribbon and the relationship between the <span class="hlt">structure</span> and properties of g-C 3 N 4 .</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('http://adsabs.harvard.edu/abs/2009ApSS..255.6661P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009ApSS..255.6661P"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> and mechanical properties of plasma nitrided ferrous alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Portolan, E.; Baumvol, I. J. R.; Figueroa, C. A.</p> <p>2009-04-01</p> <p>The <span class="hlt">electronic</span> <span class="hlt">structures</span> of the near-surface regions of two different nitrided steels (AISI 316 and 4140) were investigated using X-ray photoelectron spectroscopy. Photoelectron groups from all main chemical elements involved were addressed for steel samples with implanted-N concentrations in the range 16-32 at.%. As the implanted-N concentrations were increased, rather contrasting behaviors were observed for the two kinds of steel. The N1s photoelectrons had spectral shifts toward lower (nitrided AISI 316) or higher (nitrided AISI 4140) binding energies, whereas the Fe2p 3/2 photoelectron spectrum remains at a constant binding energy (nitrided AISI 316) or shifts toward higher binding energies (AISI 4140). These trends are discussed in terms of the metallic nitride formation and the overlapping of atomic orbitals. For nitrided AISI 316, a semi-classical approach of charge transfer between Cr and N is used to explain the experimental facts (formation of CrN), while for nitrided AISI 4140 we propose that the interaction between orbitals 4s from Fe and 2p from N promotes <span class="hlt">electrons</span> to the conduction band increasing the electrical attraction of the N1s and Fe2p <span class="hlt">electrons</span> in core shells (formation of FeN x). The increase in hardness of the steel upon N implantation is attributed to the <span class="hlt">localization</span> of <span class="hlt">electrons</span> in specific bonds, which diminishes the metallic bond character.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1988PhRvB..38..913W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1988PhRvB..38..913W"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> studies of La2CuO4</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wachs, A. L.; Turchi, P. E. A.; Jean, Y. C.; Wetzler, K. H.; Howell, R. H.; Fluss, M. J.; Harshman, D. R.; Remeika, J. P.; Cooper, A. S.; Fleming, R. M.</p> <p>1988-07-01</p> <p>We report results of positron-<span class="hlt">electron</span> momentum-distribution measurements of single-crystal La2CuO4 using two-dimensional angular correlation of positron-annihilation-radiation techniques. The data contain two components: a large (~85%), isotropic corelike <span class="hlt">electron</span> contribution and a remaining, anisotropic valence-<span class="hlt">electron</span> contribution modeled using a linear combination of atomic orbitals-molecular orbital method and a <span class="hlt">localized</span> ion scheme, within the independent-particle model approximation. This work suggests a ligand-field Hamiltonian to be justified for describing the <span class="hlt">electronic</span> properties of perovskite materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EL.....9824002F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EL.....9824002F"><span><span class="hlt">Localized</span> <span class="hlt">structures</span> in vibrated emulsions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Falcón, Claudio; Bruggeman, Jake; Pasquali, Matteo; Deegan, Robert D.</p> <p>2012-04-01</p> <p>We report our observations of <span class="hlt">localized</span> <span class="hlt">structures</span> in a thin layer of an emulsion subjected to vertical oscillations. We observe persistent holes, which are voids that span the layer depth, and kinks, which are fronts between regions with and without fluid. These <span class="hlt">structures</span> form in response to a finite amplitude perturbation. Combining experimental and rheological measurements, we argue that the ability of these <span class="hlt">structures</span> to withstand the hydrostatic pressure of the surrounding fluid is due to convection within their rim. For persistent holes the oscillatory component of the convection generates a normal stress which opposes contraction, while for kinks the steady component of the convection generates a shear stress which opposes the hydrostatic stress of the surrounding fluid.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29715033','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29715033"><span><span class="hlt">Electronic</span> <span class="hlt">Structure</span> of a Self-Assembled Monolayer with Two Surface Anchors: 6-Mercaptopurine on Au(111).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fernández, Cynthia C; Pensa, Evangelina; Carro, Pilar; Salvarezza, Roberto; Williams, Federico J</p> <p>2018-05-22</p> <p>The <span class="hlt">electronic</span> <span class="hlt">structure</span> of aromatic and aliphatic thiols on Au(111) has been extensively studied in relation to possible applications in molecular <span class="hlt">electronics</span>. In this work, the effect on the <span class="hlt">electronic</span> <span class="hlt">structure</span> of an additional anchor to the S-Au bond using 6-mercaptopurine as a model system has been investigated. Results from X-ray photoelectron spectroscopy, near-edge X-ray absorption fine <span class="hlt">structure</span> spectroscopy, and density functional theory (DFT) confirm that this molecule adsorbs on Au(111) with S-Au and iminic N-Au bonds. Combined ultraviolet photoelectron spectroscopy and DFT data reveal that formation of the 6MP self-assembled monolayer generates a molecular dipole perpendicular to the surface, with negative charges residing at the metal/monolayer interface and positive charges at the monolayer/vacuum interface, which lowers the substrate work function. Scanning tunneling microscopy shows two surface molecular domains: a well-ordered rectangular lattice where molecules are tilted on average 30° with respect to the substrate and aligned 6MP islands where molecules are standing upright. Finally, we found a new <span class="hlt">electronic</span> state located at -1.7 eV with respect to the Fermi level that corresponds to a <span class="hlt">localized</span> π molecular state, while the state corresponding to the N-Au bond is hybridized with Au d <span class="hlt">electrons</span> and stabilized at much lower energies (-3 eV).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvB..96x5108L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvB..96x5108L"><span>Chemical modulation of <span class="hlt">electronic</span> <span class="hlt">structure</span> at the excited state</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, F.; Song, C.; Gu, Y. D.; Saleem, M. S.; Pan, F.</p> <p>2017-12-01</p> <p>Spin-polarized <span class="hlt">electronic</span> <span class="hlt">structures</span> are the cornerstone of spintronics, and have thus attracted a significant amount of interest; in particular, researchers are looking into how to modulate the <span class="hlt">electronic</span> <span class="hlt">structure</span> to enable multifunctional spintronics applications, especially in half-metallic systems. However, the control of the spin polarization has only been predicted in limited two-dimensional systems with spin-polarized Dirac <span class="hlt">structures</span> and is difficult to achieve experimentally. Here, we report the modulation of the <span class="hlt">electronic</span> <span class="hlt">structure</span> in the light-induced excited state in a typical half-metal, L a1 /2S r1 /2Mn O3 -δ . According to the spin-transport measurements, there appears a light-induced increase in magnetoresistance due to the enhanced spin scattering, which is closely associated with the excited spin polarization. Strikingly, the light-induced variation can be enhanced via alcohol processing and reduced by oxygen annealing. X-ray photoelectron spectroscopy measurements show that in the chemical process, a redox reaction occurs with a change in the valence of Mn. Furthermore, first-principles calculations reveal that the change in the valence of Mn alters the <span class="hlt">electronic</span> <span class="hlt">structure</span> and consequently modulates the spin polarization in the excited state. Our findings thus report a chemically tunable <span class="hlt">electronic</span> <span class="hlt">structure</span>, demonstrating interesting physics and the potential for multifunctional applications and ultrafast spintronics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16342274','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16342274"><span>Evaluating the quality of NMR <span class="hlt">structures</span> by <span class="hlt">local</span> density of protons.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ban, Yih-En Andrew; Rudolph, Johannes; Zhou, Pei; Edelsbrunner, Herbert</p> <p>2006-03-01</p> <p>Evaluating the quality of experimentally determined protein <span class="hlt">structural</span> models is an essential step toward identifying potential errors and guiding further <span class="hlt">structural</span> refinement. Herein, we report the use of proton <span class="hlt">local</span> density as a sensitive measure to assess the quality of nuclear magnetic resonance (NMR) <span class="hlt">structures</span>. Using 256 high-resolution crystal <span class="hlt">structures</span> with protons added and optimized, we show that the <span class="hlt">local</span> density of different proton types display distinct distributions. These distributions can be characterized by statistical moments and are used to establish <span class="hlt">local</span> density Z-scores for evaluating both global and <span class="hlt">local</span> packing for individual protons. Analysis of 546 crystal <span class="hlt">structures</span> at various resolutions shows that the <span class="hlt">local</span> density Z-scores increase as the <span class="hlt">structural</span> resolution decreases and correlate well with the ClashScore (Word et al. J Mol Biol 1999;285(4):1711-1733) generated by all atom contact analysis. <span class="hlt">Local</span> density Z-scores for NMR <span class="hlt">structures</span> exhibit a significantly wider range of values than for X-ray <span class="hlt">structures</span> and demonstrate a combination of potentially problematic inflation and compression. Water-refined NMR <span class="hlt">structures</span> show improved packing quality. Our analysis of a high-quality <span class="hlt">structural</span> ensemble of ubiquitin refined against order parameters shows proton density distributions that correlate nearly perfectly with our standards derived from crystal <span class="hlt">structures</span>, further validating our approach. We present an automated analysis and visualization tool for proton packing to evaluate the quality of NMR <span class="hlt">structures</span>. 2005 Wiley-Liss, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ChPhL..30f6801L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ChPhL..30f6801L"><span>Adsorption and <span class="hlt">Electronic</span> <span class="hlt">Structure</span> of Sr and Ag Atoms on Graphite Surfaces: a First-Principles Study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Luo, Xiao-Feng; Fang, Chao; Li, Xin; Lai, Wen-Sheng; Sun, Li-Feng; Liang, Tong-Xiang</p> <p>2013-06-01</p> <p>The adsorption behaviors of radioactive strontium and silver nuclides on the graphite surface in a high-temperature gas-cooled reactor are studied by first-principles theory using generalized gradient approximation (GGA) and <span class="hlt">local</span> density approximation (LDA) pseudo-potentials. It turns out that Sr prefers to be absorbed at the hollow of the carbon hexagonal cell by 0.54 eV (GGA), while Ag likes to sit right above the carbon atom with an adsorption energy of almost zero (GGA) and 0.45 eV (LDA). <span class="hlt">Electronic</span> <span class="hlt">structure</span> analysis reveals that Sr donates its partial <span class="hlt">electrons</span> of the 4p and 5s states to the graphite substrate, while Ag on graphite is a physical adsorption without any <span class="hlt">electron</span> transfer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JMMM..374...50M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JMMM..374...50M"><span>Spin-polarized <span class="hlt">structural</span>, elastic, <span class="hlt">electronic</span> and magnetic properties of half-metallic ferromagnetism in V-doped ZnSe</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Monir, M. El Amine.; Baltache, H.; Murtaza, G.; Khenata, R.; Ahmed, Waleed K.; Bouhemadou, A.; Omran, S. Bin; Seddik, T.</p> <p>2015-01-01</p> <p>Based on first principles spin-polarized density functional theory, the <span class="hlt">structural</span>, elastic <span class="hlt">electronic</span> and magnetic properties of Zn1-xVxSe (for x=0.25, 0.50, 0.75) in zinc blende <span class="hlt">structure</span> have been studied. The investigation was done using the full-potential augmented plane wave method as implemented in WIEN2k code. The exchange-correlation potential was treated with the generalized gradient approximation PBE-GGA for the <span class="hlt">structural</span> and elastic properties. Moreover, the PBE-GGA+U approximation (where U is the Hubbard correlation terms) is employed to treat the "d" <span class="hlt">electrons</span> properly. A comparative study between the band <span class="hlt">structures</span>, <span class="hlt">electronic</span> <span class="hlt">structures</span>, total and partial densities of states and <span class="hlt">local</span> moments calculated within both GGA and GGA+U schemes is presented. The analysis of spin-polarized band <span class="hlt">structure</span> and density of states shows the half-metallic ferromagnetic character and are also used to determine s(p)-d exchange constants N0α (conduction band) and N0β (valence band) due to Se(4p)-V(3d) hybridization. It has been clearly evidence that the magnetic moment of V is reduced from its free space change value of 3 μB and the minor atomic magnetic moment on Zn and Se are generated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22577814-crystal-growth-electronic-structure-low-temperature-phase-srmgf-sub','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22577814-crystal-growth-electronic-structure-low-temperature-phase-srmgf-sub"><span>Crystal growth and <span class="hlt">electronic</span> <span class="hlt">structure</span> of low-temperature phase SrMgF{sub 4}</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>Atuchin, Victor V.; Functional Electronics Laboratory, Tomsk State University, Tomsk 634050; Laboratory of Semiconductor and Dielectric Materials, Novosibirsk State University, Novosibirsk 630090</p> <p>2016-04-15</p> <p>Using the vertical Bridgman method, the single crystal of low temperature phase SrMgF{sub 4} is obtained. The crystal is in a very good optical quality with the size of 10×7×5 mm{sup 3}. Detailed photoemission spectra of the element core levels are determined by a monochromatic AlKa (1486.6 eV) X-ray source. Moreover, the first-principles calculations are performed to investigate the <span class="hlt">electronic</span> <span class="hlt">structure</span> of SrMgF{sub 4}. A good agreement between experimental and calculated results is achieved. It is demonstrated that almost all the <span class="hlt">electronic</span> orbitals are strongly <span class="hlt">localized</span> and the hybridization with the others is very small, but the Mg–F bonds covalencymore » is relatively stronger than that of Sr–F bonds. - Graphical abstract: Large size of low-temperature phase SrMgF{sub 4} crystal was obtained (right) and its <span class="hlt">electronic</span> <span class="hlt">structure</span> was investigated by X-ray photoelectron spectroscopy and first-principles calculation (left). - Highlights: • Large size single crystal of low-temperature phase SrMgF{sub 4} is obtained. • <span class="hlt">Electronic</span> <span class="hlt">structure</span> of SrMgF{sub 4} is measured by X-ray photoelectron spectroscopy. • Partial densities of states are determined by first-principles calculation. • Good agreement between experimental and calculated results is achieved. • Strong ionic characteristics of chemical bonds are exhibited in SrMgF{sub 4}.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014Nanos...612450S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014Nanos...612450S"><span>Copper plasmonics and catalysis: role of <span class="hlt">electron</span>-phonon interactions in dephasing <span class="hlt">localized</span> surface plasmons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sun, Qi-C.; Ding, Yuchen; Goodman, Samuel M.; H. Funke, Hans; Nagpal, Prashant</p> <p>2014-10-01</p> <p>Copper metal can provide an important alternative for the development of efficient, low-cost and low-loss plasmonic nanoparticles, and selective nanocatalysts. However, poor chemical stability and lack of insight into photophysics and plasmon decay mechanisms has impeded study. Here, we use smooth conformal ALD coating on copper nanoparticles to prevent surface oxidation, and study dephasing time for <span class="hlt">localized</span> surface plasmons on different sized copper nanoparticles. Using dephasing time as a figure of merit, we elucidate the role of <span class="hlt">electron-electron</span>, <span class="hlt">electron</span>-phonon, impurity, surface and grain boundary scattering on the decay of <span class="hlt">localized</span> surface plasmon waves. Using our quantitative analysis and different temperature dependent measurements, we show that <span class="hlt">electron</span>-phonon interactions dominate over other scattering mechanisms in dephasing plasmon waves. While interband transitions in copper metal contributes substantially to plasmon losses, tuning surface plasmon modes to infrared frequencies leads to a five-fold enhancement in the quality factor. These findings demonstrate that conformal ALD coatings can improve the chemical stability for copper nanoparticles, even at high temperatures (>300 °C) in ambient atmosphere, and nanoscaled copper is a good alternative material for many potential applications in nanophotonics, plasmonics, catalysis and nanoscale <span class="hlt">electronics</span>.Copper metal can provide an important alternative for the development of efficient, low-cost and low-loss plasmonic nanoparticles, and selective nanocatalysts. However, poor chemical stability and lack of insight into photophysics and plasmon decay mechanisms has impeded study. Here, we use smooth conformal ALD coating on copper nanoparticles to prevent surface oxidation, and study dephasing time for <span class="hlt">localized</span> surface plasmons on different sized copper nanoparticles. Using dephasing time as a figure of merit, we elucidate the role of <span class="hlt">electron-electron</span>, <span class="hlt">electron</span>-phonon, impurity, surface and grain</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvB..96w5137H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvB..96w5137H"><span><span class="hlt">Structural</span>, <span class="hlt">electronic</span>, and thermodynamic properties of curium dioxide: Density functional theory calculations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hou, Ling; Li, Wei-Dong; Wang, Fangwei; Eriksson, Olle; Wang, Bao-Tian</p> <p>2017-12-01</p> <p>We present a systematic investigation of the <span class="hlt">structural</span>, magnetic, <span class="hlt">electronic</span>, mechanical, and thermodynamic properties of CmO2 with the <span class="hlt">local</span> density approximation (LDA)+U and the generalized gradient approximation (GGA)+U approaches. The strong Coulomb repulsion and the spin-orbit coupling (SOC) effects on the lattice <span class="hlt">structures</span>, <span class="hlt">electronic</span> density of states, and band gaps are carefully studied, and compared with other A O2 (A =U , Np, Pu, and Am). The ferromagnetic configuration with half-metallic character is predicted to be energetically stable while a charge-transfer semiconductor is predicted for the antiferromagnetic configuration. The elastic constants and phonon spectra show that the fluorite <span class="hlt">structure</span> is mechanically and dynamically stable. Based on the first-principles phonon density of states, the lattice vibrational energy is calculated using the quasiharmonic approximation. Then, the Gibbs free energy, thermal expansion coefficient, specific heat, and entropy are obtained and compared with experimental data. The mode Grüneisen parameters are presented to analyze the anharmonic properties. The Slack relation is applied to obtain the lattice thermal conductivity in temperature range of 300-1600 K. The phonon group velocities are also calculated to investigate the heat transfer. For all these properties, if available, we compare the results of CmO2 with other A O2 .</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JPhD...47b5304Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JPhD...47b5304Z"><span>The <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties of amorphous HgCdTe from first-principles calculations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Huxian; Chen, Xiaoshuang; Lu, Jianping; Shu, Haibo; Lu, Wei</p> <p>2014-01-01</p> <p>Amorphous mercury cadmium telluride (a-MCT) model <span class="hlt">structures</span>, with x being 0.125 and 0.25, are obtained from first-principles calculations. We generate initial <span class="hlt">structures</span> by computation alchemy method. It is found that most atoms in the network of amorphous <span class="hlt">structures</span> tend to be fourfold and form tetrahedral <span class="hlt">structures</span>, implying that the chemical ordered continuous random network with some coordination defects is the ideal <span class="hlt">structure</span> for a-MCT. The <span class="hlt">electronic</span> <span class="hlt">structure</span> is also concerned. The gap is found to be 0.30 and 0.26 eV for a-Hg0.875Cd0.125Te and a-Hg0.75Cd0.25Te model <span class="hlt">structures</span>, independent of the composition. By comparing with the properties of crystalline MCT with the same composition, we observe a blue-shift of energy band gap. The <span class="hlt">localization</span> of tail states and its atomic origin are also discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PNAS..114.7289Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PNAS..114.7289Z"><span><span class="hlt">Local</span> thermal energy as a <span class="hlt">structural</span> indicator in glasses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zylberg, Jacques; Lerner, Edan; Bar-Sinai, Yohai; Bouchbinder, Eran</p> <p>2017-07-01</p> <p>Identifying heterogeneous <span class="hlt">structures</span> in glasses—such as <span class="hlt">localized</span> soft spots—and understanding <span class="hlt">structure</span>-dynamics relations in these systems remain major scientific challenges. Here, we derive an exact expression for the <span class="hlt">local</span> thermal energy of interacting particles (the mean <span class="hlt">local</span> potential energy change caused by thermal fluctuations) in glassy systems by a systematic low-temperature expansion. We show that the <span class="hlt">local</span> thermal energy can attain anomalously large values, inversely related to the degree of softness of <span class="hlt">localized</span> <span class="hlt">structures</span> in a glass, determined by a coupling between internal stresses—an intrinsic signature of glassy frustration—anharmonicity and low-frequency vibrational modes. These anomalously large values follow a fat-tailed distribution, with a universal exponent related to the recently observed universal <mml:math><mml:msup><mml:mi>ω</mml:mi><mml:mn>4</mml:mn></mml:msup></mml:math>ω4 density of states of quasilocalized low-frequency vibrational modes. When the spatial thermal energy field—a “softness field”—is considered, this power law tail manifests itself by highly <span class="hlt">localized</span> spots, which are significantly softer than their surroundings. These soft spots are shown to be susceptible to plastic rearrangements under external driving forces, having predictive powers that surpass those of the normal modes-based approach. These results offer a general, system/model-independent, physical/observable-based approach to identify <span class="hlt">structural</span> properties of quiescent glasses and relate them to glassy dynamics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1266003-electronic-structure-electron-phonon-coupling-tih-_2','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1266003-electronic-structure-electron-phonon-coupling-tih-_2"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> and <span class="hlt">electron</span>-phonon coupling in TiH$$_2$$</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Shanavas, Kavungal Veedu; Lindsay, Lucas R.; Parker, David S.</p> <p>2016-06-15</p> <p>Calculations using first principles methods and strong coupling theory are carried out to understand the <span class="hlt">electronic</span> <span class="hlt">structure</span> and superconductivity in cubic and tetragonal TiHmore » $$_2$$. A large <span class="hlt">electronic</span> density of states at the Fermi level in the cubic phase arises from Ti-$$t_{2g}$$ states and leads to a <span class="hlt">structural</span> instability against tetragonal distortion at low temperatures. However, constraining the in-plane lattice constants diminishes the energy gain associated with the tetragonal distortion, allowing the cubic phase to be stable at low temperatures. Furthermore, calculated phonon dispersions show decoupled acoustic and optic modes arising from Ti and H vibrations, respectively and frequencies of optic modes to be rather high. The cubic phase has a large <span class="hlt">electron</span>-phonon coupling parameter $$\\lambda$$ and critical temperature of several K. Contribution of the hydrogen sublattice to $$\\lambda$$ is found to be small in this material, which we understand from strong coupling theory to be due to the small H-$s$ DOS at the Fermi level and high energy of hydrogen modes at the tetrahedral sites.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1435309-local-structure-defects-ion-irradiated-ktao3','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1435309-local-structure-defects-ion-irradiated-ktao3"><span><span class="hlt">Local</span> <span class="hlt">structure</span> and defects in ion irradiated KTaO 3</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, Fuxiang; Xi, Jianqi; Zhang, Yanwen</p> <p></p> <p>Here, the modification of the <span class="hlt">local</span> <span class="hlt">structure</span> in cubic perovskite KTaO 3 irradiated with 3 MeV and 1.1 GeV Au ions is studied by Raman and x-ray absorption spectroscopy, complemented by density functional theory (DFT) calculations. In the case of irradiation with 3 MeV Au ions where displacement cascade processes are dominant, the Ta L 3-edge x-ray absorption measurements suggest that a peak corresponding to the Ta–O bonds in the TaO 6 octahedra splits, which is attributed to the formation of Ta K antisite defects that are coupled with oxygen vacancies, V O. This finding is consistent with the DFTmore » calculations. Under irradiation with 1.1 GeV ions, the intense ionization and <span class="hlt">electronic</span> energy deposition lead to a blue shift and an intensity reduction of active Raman bands. In the case of sequential irradiations, extended x-ray absorption fine <span class="hlt">structure</span> measurements reveal a decrease in concentration of coupled Ta K-V O defects under subsequent irradiation with 1.1 GeV Au ions.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPCM...30n5401Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPCM...30n5401Z"><span><span class="hlt">Local</span> <span class="hlt">structure</span> and defects in ion irradiated KTaO3</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, F. X.; Xi, J.; Zhang, Y.; Tong, Yang; Xue, H.; Huang, R.; Trautmann, C.; Weber, W. J.</p> <p>2018-04-01</p> <p>The modification of the <span class="hlt">local</span> <span class="hlt">structure</span> in cubic perovskite KTaO3 irradiated with 3 MeV and 1.1 GeV Au ions is studied by Raman and x-ray absorption spectroscopy, complemented by density functional theory (DFT) calculations. In the case of irradiation with 3 MeV Au ions where displacement cascade processes are dominant, the Ta L3-edge x-ray absorption measurements suggest that a peak corresponding to the Ta-O bonds in the TaO6 octahedra splits, which is attributed to the formation of TaK antisite defects that are coupled with oxygen vacancies, V O. This finding is consistent with the DFT calculations. Under irradiation with 1.1 GeV ions, the intense ionization and <span class="hlt">electronic</span> energy deposition lead to a blue shift and an intensity reduction of active Raman bands. In the case of sequential irradiations, extended x-ray absorption fine <span class="hlt">structure</span> measurements reveal a decrease in concentration of coupled TaK-V O defects under subsequent irradiation with 1.1 GeV Au ions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1435309-local-structure-defects-ion-irradiated-ktao3','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1435309-local-structure-defects-ion-irradiated-ktao3"><span><span class="hlt">Local</span> <span class="hlt">structure</span> and defects in ion irradiated KTaO 3</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Zhang, Fuxiang; Xi, Jianqi; Zhang, Yanwen; ...</p> <p>2018-03-12</p> <p>Here, the modification of the <span class="hlt">local</span> <span class="hlt">structure</span> in cubic perovskite KTaO 3 irradiated with 3 MeV and 1.1 GeV Au ions is studied by Raman and x-ray absorption spectroscopy, complemented by density functional theory (DFT) calculations. In the case of irradiation with 3 MeV Au ions where displacement cascade processes are dominant, the Ta L 3-edge x-ray absorption measurements suggest that a peak corresponding to the Ta–O bonds in the TaO 6 octahedra splits, which is attributed to the formation of Ta K antisite defects that are coupled with oxygen vacancies, V O. This finding is consistent with the DFTmore » calculations. Under irradiation with 1.1 GeV ions, the intense ionization and <span class="hlt">electronic</span> energy deposition lead to a blue shift and an intensity reduction of active Raman bands. In the case of sequential irradiations, extended x-ray absorption fine <span class="hlt">structure</span> measurements reveal a decrease in concentration of coupled Ta K-V O defects under subsequent irradiation with 1.1 GeV Au ions.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006CPL...425..311C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006CPL...425..311C"><span>OsB 2 and RuB 2, ultra-incompressible, hard materials: First-principles <span class="hlt">electronic</span> <span class="hlt">structure</span> calculations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chiodo, S.; Gotsis, H. J.; Russo, N.; Sicilia, E.</p> <p>2006-07-01</p> <p>Recently it has been reported that osmium diboride has an unusually large bulk modulus combined with high hardness, and consequently is a most interesting candidate as an ultra-incompressible and hard material. The <span class="hlt">electronic</span> and <span class="hlt">structural</span> properties of the transition metal diborides OsB 2 and RuB 2 have been calculated within the <span class="hlt">local</span> density approximation (LDA). It is shown that the high hardness is the result of covalent bonding between transition metal d states and boron p states in the orthorhombic <span class="hlt">structure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhSen...4..344Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhSen...4..344Z"><span>Aluminum alloy material <span class="hlt">structure</span> impact <span class="hlt">localization</span> by using FBG sensors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Xiubin</p> <p>2014-12-01</p> <p>The aluminum alloy <span class="hlt">structure</span> impact <span class="hlt">localization</span> system by using fiber Bragg grating (FBG) sensors and impact <span class="hlt">localization</span> algorithm was investigated. A four-FBG sensing network was established. And the power intensity demodulation method was initialized employing the narrow-band tunable laser. The wavelet transform was used to weaken the impact signal noise. And the impact signal time difference was extracted to build the time difference <span class="hlt">localization</span> algorithm. At last, a fiber Bragg grating impact <span class="hlt">localization</span> system was established and experimentally verified. The experimental results showed that in the aluminum alloy plate with the 500 mm*500 mm*2 mm test area, the maximum and average impact abscissa <span class="hlt">localization</span> errors were 11 mm and 6.25 mm, and the maximum and average impact ordinate <span class="hlt">localization</span> errors were 9 mm and 4.25 mm, respectively. The fiber Bragg grating sensors and demodulation system are feasible to realize the aviation aluminum alloy material <span class="hlt">structure</span> impact <span class="hlt">localization</span>. The research results provide a reliable method for the aluminum alloy material <span class="hlt">structure</span> impact <span class="hlt">localization</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/935669','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/935669"><span>Likelihood-based modification of experimental crystal <span class="hlt">structure</span> <span class="hlt">electron</span> density maps</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Terwilliger, Thomas C [Sante Fe, NM</p> <p>2005-04-16</p> <p>A maximum-likelihood method for improves an <span class="hlt">electron</span> density map of an experimental crystal <span class="hlt">structure</span>. A likelihood of a set of <span class="hlt">structure</span> factors {F.sub.h } is formed for the experimental crystal <span class="hlt">structure</span> as (1) the likelihood of having obtained an observed set of <span class="hlt">structure</span> factors {F.sub.h.sup.OBS } if <span class="hlt">structure</span> factor set {F.sub.h } was correct, and (2) the likelihood that an <span class="hlt">electron</span> density map resulting from {F.sub.h } is consistent with selected prior knowledge about the experimental crystal <span class="hlt">structure</span>. The set of <span class="hlt">structure</span> factors {F.sub.h } is then adjusted to maximize the likelihood of {F.sub.h } for the experimental crystal <span class="hlt">structure</span>. An improved <span class="hlt">electron</span> density map is constructed with the maximized <span class="hlt">structure</span> factors.</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('https://www.ncbi.nlm.nih.gov/pubmed/23831940','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23831940"><span>Method for <span class="hlt">local</span> temperature measurement in a nanoreactor for in situ high-resolution <span class="hlt">electron</span> microscopy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Vendelbo, S B; Kooyman, P J; Creemer, J F; Morana, B; Mele, L; Dona, P; Nelissen, B J; Helveg, S</p> <p>2013-10-01</p> <p>In situ high-resolution transmission <span class="hlt">electron</span> microscopy (TEM) of solids under reactive gas conditions can be facilitated by microelectromechanical system devices called nanoreactors. These nanoreactors are windowed cells containing nanoliter volumes of gas at ambient pressures and elevated temperatures. However, due to the high spatial confinement of the reaction environment, traditional methods for measuring process parameters, such as the <span class="hlt">local</span> temperature, are difficult to apply. To address this issue, we devise an <span class="hlt">electron</span> energy loss spectroscopy (EELS) method that probes the <span class="hlt">local</span> temperature of the reaction volume under inspection by the <span class="hlt">electron</span> beam. The <span class="hlt">local</span> gas density, as measured using quantitative EELS, is combined with the inherent relation between gas density and temperature, as described by the ideal gas law, to obtain the <span class="hlt">local</span> temperature. Using this method we determined the temperature gradient in a nanoreactor in situ, while the average, global temperature was monitored by a traditional measurement of the electrical resistivity of the heater. The <span class="hlt">local</span> gas temperatures had a maximum of 56 °C deviation from the global heater values under the applied conditions. The <span class="hlt">local</span> temperatures, obtained with the proposed method, are in good agreement with predictions from an analytical model. Copyright © 2013 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007PhDT........29L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007PhDT........29L"><span>Crystal and <span class="hlt">electronic</span> <span class="hlt">structure</span> of copper sulfides</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lukashev, Pavel</p> <p></p> <p>Copper sulfides with different copper concentration exist in mineral form ranging from CuS to Cu2S. Among these, chalcosite Cu 2S, and digenite Cu1.8S were the subject of extensive research for decades mainly because of their use as the absorber in photovoltaic cells. Yet; their <span class="hlt">electronic</span> <span class="hlt">structure</span> is poorly understood because their crystal <span class="hlt">structure</span> is complex. Most of the results published so far report the semiconducting nature of these compounds with the energy band gap being in the range of 0.84 to 1.9 eV. The crystal <span class="hlt">structure</span> consists of a close-packed lattice of S with mobile Cu occupying various types of interstitial sites with a statistical distribution depending on temperature. In this thesis we present the first computational study of their <span class="hlt">electronic</span> band <span class="hlt">structure</span>. Initially, we investigated the simpler antifluorite <span class="hlt">structure</span>. Both <span class="hlt">local</span> density approximation (LDA) and self-consistent quasiparticle GW calculations with the full-potential linearized muffin-tin orbital method give a semimetallic band <span class="hlt">structure</span>. Inspection of the nature of the bands shows that the lowest conduction band is mainly Cu-s-like except right near the center of the Brillouin zone where a Cu-s-like state lies about 1 eV below the valence band maximum. Significantly, in GW calculations, this state shifts up by several 0.1 eV but not sufficiently to open a gap. A random distortion of the Cu atoms from the perfect antifluorite positions is found to break the degeneracy of the d state at the Gamma-point and thus opens up a small gap of about 0.1 eV in LDA. As our next step we constructed supercell models for the cubic and hexagonal phases with the Cu positions determined by a weighted random number generator. The low temperature monoclinic phase was also studied. The computed total energies of these <span class="hlt">structures</span> follow the same order as the reported phases with increasing temperatures. All these models gave similar small band gaps of order 0.1-0.2 eV. However, their conduction band</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MS%26E..292a2020L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MS%26E..292a2020L"><span>Effects of B site doping on <span class="hlt">electronic</span> <span class="hlt">structures</span> of InNbO4 based on hybrid density functional calculations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lu, M. F.; Zhou, C. P.; Li, Q. Q.; Zhang, C. L.; Shi, H. F.</p> <p>2018-01-01</p> <p>In order to improve the photocatalytic activity under visible-light irradiation, we adopted first principle calculations based on density functional theory (DFT) to calculate the <span class="hlt">electronic</span> <span class="hlt">structures</span> of B site transition metal element doped InNbO4. The results indicated that the complete hybridization of Nb 4d states and some Ti 3d states contributed to the new conduction band of Ti doped InNbO4, barely changing the position of band edge. For Cr doping, some <span class="hlt">localized</span> Cr 3d states were introduced into the band gap. Nonetheless, the potential of <span class="hlt">localized</span> levels was too positive to cause visible-light reaction. When it came to Cu doping, the band gap was almost same with that of InNbO4 as well as some <span class="hlt">localized</span> Cu 3d states appeared above the top of VB. The introduction of <span class="hlt">localized</span> energy levels benefited <span class="hlt">electrons</span> to migrate from valence band (VB) to conduction band (CB) by absorbing lower energy photons, realizing visible-light response.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000APS..DPPGI3005S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000APS..DPPGI3005S"><span>A Non <span class="hlt">Local</span> <span class="hlt">Electron</span> Heat Transport Model for Multi-Dimensional Fluid Codes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schurtz, Guy</p> <p>2000-10-01</p> <p>Apparent inhibition of thermal heat flow is one of the most ancient problems in computational Inertial Fusion and flux-limited Spitzer-Harm conduction has been a mainstay in multi-dimensional hydrodynamic codes for more than 25 years. Theoretical investigation of the problem indicates that heat transport in laser produced plasmas has to be considered as a non <span class="hlt">local</span> process. Various authors contributed to the non <span class="hlt">local</span> theory and proposed convolution formulas designed for practical implementation in one-dimensional fluid codes. Though the theory, confirmed by kinetic calculations, actually predicts a reduced heat flux, it fails to explain the very small limiters required in two-dimensional simulations. Fokker-Planck simulations by Epperlein, Rickard and Bell [PRL 61, 2453 (1988)] demonstrated that non <span class="hlt">local</span> effects could lead to a strong reduction of heat flow in two dimensions, even in situations where a one-dimensional analysis suggests that the heat flow is nearly classical. We developed at CEA/DAM a non <span class="hlt">local</span> <span class="hlt">electron</span> heat transport model suitable for implementation in our two-dimensional radiation hydrodynamic code FCI2. This model may be envisionned as the first step of an iterative solution of the Fokker-Planck equations; it takes the mathematical form of multigroup diffusion equations, the solution of which yields both the heat flux and the departure of the <span class="hlt">electron</span> distribution function to the Maxwellian. Although direct implementation of the model is straightforward, formal solutions of it can be expressed in convolution form, exhibiting a three-dimensional tensor propagator. Reduction to one dimension retrieves the original formula of Luciani, Mora and Virmont [PRL 51, 1664 (1983)]. Intense magnetic fields may be generated by thermal effects in laser targets; these fields, as well as non <span class="hlt">local</span> effects, will inhibit <span class="hlt">electron</span> conduction. We present simulations where both effects are taken into account and shortly discuss the coupling strategy between them.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1417363-electron-poor-polar-intermetallics-complex-structures-novel-clusters-intriguing-bonding-pronounced-electron-delocalization','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1417363-electron-poor-polar-intermetallics-complex-structures-novel-clusters-intriguing-bonding-pronounced-electron-delocalization"><span><span class="hlt">Electron</span>-Poor Polar Intermetallics: Complex <span class="hlt">Structures</span>, Novel Clusters, and Intriguing Bonding with Pronounced <span class="hlt">Electron</span> Delocalization</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>Lin, Qisheng; Miller, Gordon J.</p> <p></p> <p>Intermetallic compounds represent an extensive pool of candidates for energy related applications stemming from magnetic, electric, optic, caloric, and catalytic properties. The discovery of novel intermetallic compounds can enhance understanding of the chemical principles that govern <span class="hlt">structural</span> stability and chemical bonding as well as finding new applications. Valence <span class="hlt">electron</span>-poor polar intermetallics with valence <span class="hlt">electron</span> concentrations (VECs) between 2.0 and 3.0 e –/atom show a plethora of unprecedented and fascinating <span class="hlt">structural</span> motifs and bonding features. Furthermore, establishing simple <span class="hlt">structure</span>-bonding-property relationships is especially challenging for this compound class because commonly accepted valence <span class="hlt">electron</span> counting rules are inappropriate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1417363-electron-poor-polar-intermetallics-complex-structures-novel-clusters-intriguing-bonding-pronounced-electron-delocalization','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1417363-electron-poor-polar-intermetallics-complex-structures-novel-clusters-intriguing-bonding-pronounced-electron-delocalization"><span><span class="hlt">Electron</span>-Poor Polar Intermetallics: Complex <span class="hlt">Structures</span>, Novel Clusters, and Intriguing Bonding with Pronounced <span class="hlt">Electron</span> Delocalization</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Lin, Qisheng; Miller, Gordon J.</p> <p>2017-12-18</p> <p>Intermetallic compounds represent an extensive pool of candidates for energy related applications stemming from magnetic, electric, optic, caloric, and catalytic properties. The discovery of novel intermetallic compounds can enhance understanding of the chemical principles that govern <span class="hlt">structural</span> stability and chemical bonding as well as finding new applications. Valence <span class="hlt">electron</span>-poor polar intermetallics with valence <span class="hlt">electron</span> concentrations (VECs) between 2.0 and 3.0 e –/atom show a plethora of unprecedented and fascinating <span class="hlt">structural</span> motifs and bonding features. Furthermore, establishing simple <span class="hlt">structure</span>-bonding-property relationships is especially challenging for this compound class because commonly accepted valence <span class="hlt">electron</span> counting rules are inappropriate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPCM...29g5302D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPCM...29g5302D"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of multi-walled carbon fullerenes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Doore, Keith; Cook, Matthew; Clausen, Eric; Lukashev, Pavel V.; Kidd, Tim E.; Stollenwerk, Andrew J.</p> <p>2017-02-01</p> <p>Despite an enormous amount of research on carbon based nanostructures, relatively little is known about the <span class="hlt">electronic</span> <span class="hlt">structure</span> of multi-walled carbon fullerenes, also known as carbon onions. In part, this is due to the very high computational expense involved in estimating <span class="hlt">electronic</span> <span class="hlt">structure</span> of large molecules. At the same time, experimentally, the exact crystal <span class="hlt">structure</span> of the carbon onion is usually unknown, and therefore one relies on qualitative arguments only. In this work we present the results of a computational study on a series of multi-walled fullerenes and compare their <span class="hlt">electronic</span> <span class="hlt">structures</span> to experimental data. Experimentally, the carbon onions were fabricated using ultrasonic agitation of isopropanol alcohol and deposited onto the surface of highly ordered pyrolytic graphite using a drop cast method. Scanning tunneling microscopy images indicate that the carbon onions produced using this technique are ellipsoidal with dimensions on the order of 10 nm. The majority of differential tunneling spectra acquired on individual carbon onions are similar to that of graphite with the addition of molecular-like peaks, indicating that these particles span the transition between molecules and bulk crystals. A smaller, yet sizable number exhibited a semiconducting gap between the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) levels. These results are compared with the <span class="hlt">electronic</span> <span class="hlt">structure</span> of different carbon onion configurations calculated using first-principles. Similar to the experimental results, the majority of these configurations are metallic with a minority behaving as semiconductors. Analysis of the configurations investigated here reveals that each carbon onion exhibiting an energy band gap consisted only of non-metallic fullerene layers, indicating that the interlayer interaction is not significant enough to affect the total density of states in these <span class="hlt">structures</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JPhCS.291a2021M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JPhCS.291a2021M"><span><span class="hlt">Local</span> <span class="hlt">structure</span> of high-coercivity Fe-Ni-Al alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Menushenkov, A. P.; Menushenkov, V. P.; Chernikov, R. V.; Sviridova, T. A.; Grishina, O. V.; Sidorov, V. V.</p> <p>2011-04-01</p> <p>Results of hard magnetic Fe-Ni-Al alloys after various thermal processing <span class="hlt">local</span> <span class="hlt">structure</span> researches by method of EXAFS-spectroscopy with use of synchrotron radiation at temperature 77 K are presented. It is established, that during cooling a firm solution with critical speed reorganization of a <span class="hlt">local</span> environment of nickel relative to quickly tempered sample owing to stratification of a firm solution is observed. The subsequent aging at 780°C practically restores <span class="hlt">local</span> <span class="hlt">structure</span>, characteristic for quickly tempered sample, keeping thus rather high coercitive force.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998EPJAP...4..143M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998EPJAP...4..143M"><span><span class="hlt">Local</span> spin density functional investigations of a manganite with perovskite-type derived <span class="hlt">structures</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matar, S. F.; Studer, F.; Siberchicot, B.; Subramanian, M. A.; Demazeau, G.; Etourneau, J.</p> <p>1998-11-01</p> <p>The <span class="hlt">electronic</span> and magnetic <span class="hlt">structures</span> of the perovskite CaMnO3 are self-consistently calculated assuming two crystal <span class="hlt">structures</span> at the same formula unit volume within the <span class="hlt">local</span> spin density functional theory and the augmented spherical wave (ASW) method. From the comparisons of energy differences between the different magnetic states the ground state configuration is an insulator with G-type ordering. This result together with the magnitudes of the magnetic moments are in agreement with experiment. The influence of mixing between Mn and O is found spin dependent from the analysis of the crystal orbital overlap population (COOP) which enable to describe the chemical bond. The calculations underline a feature of a half metallic ferromagnet which could be connected with the colossal magnetoresistance (CMR) property of related compounds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22004762-calculation-electron-structure-vacancies-compensated-states-iii-vi-semiconductors','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22004762-calculation-electron-structure-vacancies-compensated-states-iii-vi-semiconductors"><span>Calculation of the <span class="hlt">electron</span> <span class="hlt">structure</span> of vacancies and their compensated states in III-VI semiconductors</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>Mehrabova, M. A., E-mail: Mehrabova@mail.ru; Madatov, R. S.</p> <p>2011-08-15</p> <p>The Green's functions theory and the bond-orbital model are used as a basis for calculations of the <span class="hlt">electron</span> <span class="hlt">structure</span> of <span class="hlt">local</span> defects-specifically, vacancies and their compensated states in III-VI semiconductors. The energy levels in the band gap are established, and the changes induced in the <span class="hlt">electron</span> densities in the GaS, GaSe, and InSe semiconductors by anion and cation vacancies and their compensated states are calculated. It is established that, if a vacancy is compensated by an atom of an element from the same subgroup with the same tetrahedral coordination and if the ionic radius of the compensating atom is smallermore » than that of the substituted atom, the <span class="hlt">local</span> levels formed by the vacancy completely disappear. It is shown that this mechanism of compensation of vacancies provides a means not only for recovering the parameters of the crystal, but for improving the characteristics of the crystal as well.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21360184','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21360184"><span><span class="hlt">Structure</span> and <span class="hlt">electronic</span> properties of Alq3 derivatives with <span class="hlt">electron</span> acceptor/donor groups at the C4 positions of the quinolate ligands: a theoretical study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rao, Joshi Laxmikanth; Bhanuprakash, Kotamarthi</p> <p>2011-12-01</p> <p>The molecular <span class="hlt">structures</span> of the ground (S(0)) and first singlet excited (S(1)) states of Alq3 derivatives in which pyrazolyl and 3-methylpyrazolyl groups are substituted at the C4 positions of the 8-hydroxyquinolate ligands as <span class="hlt">electron</span> acceptors, and piperidinyl and N-methylpiperazinyl groups are substituted at the same positions as <span class="hlt">electron</span> donors, have been optimized using the B3LYP/6-31G and CIS/6-31G methods, respectively. In order to analyze the <span class="hlt">electronic</span> transitions in these derivatives, the frontier molecular orbital characteristics were analyzed systematically, and it was found that the highest occupied molecular orbital is <span class="hlt">localized</span> on the A ligand while the lowest unoccupied molecular orbital is <span class="hlt">localized</span> on the B ligand in their ground states, similar to what is seen for mer-Alq3. The absorption and emission spectra were evaluated at the TD-PBE0/6-31G level, and it was observed that <span class="hlt">electron</span> acceptor substitution causes a red-shift in the emission spectra, which is also seen experimentally. The reorganization energies were calculated at the B3LYP/6-31G level and the results show that acceptor/donor substitution has a significant effect on the intrinsic charge mobilities of these derivatives as compared to mer-Alq3.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18491388','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18491388"><span>Taking advantage of <span class="hlt">local</span> <span class="hlt">structure</span> descriptors to analyze interresidue contacts in protein <span class="hlt">structures</span> and protein complexes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Martin, Juliette; Regad, Leslie; Etchebest, Catherine; Camproux, Anne-Claude</p> <p>2008-11-15</p> <p>Interresidue protein contacts in proteins <span class="hlt">structures</span> and at protein-protein interface are classically described by the amino acid types of interacting residues and the <span class="hlt">local</span> <span class="hlt">structural</span> context of the contact, if any, is described using secondary <span class="hlt">structures</span>. In this study, we present an alternate analysis of interresidue contact using <span class="hlt">local</span> <span class="hlt">structures</span> defined by the <span class="hlt">structural</span> alphabet introduced by Camproux et al. This <span class="hlt">structural</span> alphabet allows to describe a 3D <span class="hlt">structure</span> as a sequence of prototype fragments called <span class="hlt">structural</span> letters, of 27 different types. Each residue can then be assigned to a particular <span class="hlt">local</span> <span class="hlt">structure</span>, even in loop regions. The analysis of interresidue contacts within protein <span class="hlt">structures</span> defined using Voronoï tessellations reveals that pairwise contact specificity is greater in terms of <span class="hlt">structural</span> letters than amino acids. Using a simple heuristic based on specificity score comparison, we find that 74% of the long-range contacts within protein <span class="hlt">structures</span> are better described using <span class="hlt">structural</span> letters than amino acid types. The investigation is extended to a set of protein-protein complexes, showing that the similar global rules apply as for intraprotein contacts, with 64% of the interprotein contacts best described by <span class="hlt">local</span> <span class="hlt">structures</span>. We then present an evaluation of pairing functions integrating <span class="hlt">structural</span> letters to decoy scoring and show that some complexes could benefit from the use of <span class="hlt">structural</span> letter-based pairing functions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJD...71..191Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJD...71..191Y"><span>The stabilities and <span class="hlt">electron</span> <span class="hlt">structures</span> of Al-Mg clusters with 18 and 20 valence <span class="hlt">electrons</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Huihui; Chen, Hongshan</p> <p>2017-07-01</p> <p>The spherical jellium model predicts that metal clusters having 18 and 20 valence <span class="hlt">electrons</span> correspond to the magic numbers and will show specific stabilities. We explore in detail the geometric <span class="hlt">structures</span>, stabilities and <span class="hlt">electronic</span> <span class="hlt">structures</span> of Al-Mg clusters containing 18 and 20 valence <span class="hlt">electrons</span> by using genetic algorithm combined with density functional theories. The stabilities of the clusters are governed by the <span class="hlt">electronic</span> configurations and Mg/Al ratios. The clusters with lower Mg/Al ratios are more stable. The molecular orbitals accord with the shell <span class="hlt">structures</span> predicted by the jellium model but the 2S level interweaves with the 1D levels and the 2S and 1D orbitals form a subgroup. The clusters having 20 valence <span class="hlt">electrons</span> form closed 1S21P61D102S2 shells and show enhanced stability. The Al-Mg clusters with a valence <span class="hlt">electron</span> count of 18 do not form closed shells because one 1D orbital is unoccupied. The ionization potential and <span class="hlt">electron</span> affinity are closely related to the <span class="hlt">electronic</span> configurations; their values are determined by the subgroups the HOMO or LUMO belong to. Supplementary material in the form of one pdf file available from the Journal web page at http://https://doi.org/10.1140/epjd/e2017-80042-9</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JMoSt1160...92T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JMoSt1160...92T"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of binuclear acetylacetonates of boron difluoride</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tikhonov, Sergey A.; Svistunova, Irina V.; Samoilov, Ilya S.; Osmushko, Ivan S.; Borisenko, Aleksandr V.; Vovna, Vitaliy I.</p> <p>2018-05-01</p> <p>The <span class="hlt">electronic</span> <span class="hlt">structure</span> of boron difluoride acetylacetonate and its three derivatives was studied using photoelectron and absorption spectroscopy, as well as the density functional theory. In a series of binuclear acetylacetonate complexes containing bridge-moieties of sulfur and selenium atoms, it was found an appreciable mixing of the π3-orbital of the chelate cycle with atomic orbitals S 3p and Se 4p resulting in destabilization of the HOMO levels by 0.4-0.6 eV, in comparison with the monomer. The positively charged fragment C(CH3)-CX-C(CH3) causes the field effect, which leads to stabilization of the LUMO levels by 0.3-0.4 eV and C 1s-levels by 0.5-1.2 eV. An analysis of the research results on the <span class="hlt">electronic</span> <span class="hlt">structure</span> made it possible to determine the effect of substituents in the γ position on the absorption spectra, which is mainly determined by the <span class="hlt">electron</span> density transfer from the chalcogen atoms to the chelate cycles. It is shown that the calculated energy intervals between <span class="hlt">electron</span> levels correlate well with the <span class="hlt">structure</span> of the photoelectron spectra of valence and core <span class="hlt">electrons</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=teste+AND+CAT-A+AND+%5d&pg=5&id=EJ870575','ERIC'); return false;" href="https://eric.ed.gov/?q=teste+AND+CAT-A+AND+%5d&pg=5&id=EJ870575"><span><span class="hlt">Electronic</span> Resources in a Next-Generation Catalog: The Case of WorldCat <span class="hlt">Local</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>Shadle, Steve</p> <p>2009-01-01</p> <p>In April 2007, the University of Washington Libraries debuted WorldCat <span class="hlt">Local</span> (WCL), a <span class="hlt">localized</span> version of the WorldCat database that interoperates with a library's integrated library system and fulfillment services to provide a single-search interface for a library's physical and <span class="hlt">electronic</span> content. This brief will describe how WCL incorporates a…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPCS..113..102D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPCS..113..102D"><span>Theoretical study of the <span class="hlt">local</span> <span class="hlt">structures</span> and the EPR parameters for RLNKB glasses with VO2+ and Cu2+ dopants</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ding, Chang-Chun; Wu, Shao-Yi; Wu, Li-Na; Zhang, Li-Juan; Peng, Li; Wu, Ming-He; Teng, Bao-Hua</p> <p>2018-02-01</p> <p>The <span class="hlt">electron</span> paramagnetic resonance (EPR) parameters and <span class="hlt">local</span> <span class="hlt">structures</span> for impurities VO2+ and Cu2+ in RO-Li2O-Na2O-K2O-B2O3 (RLNKB; R = Zn, Mg, Sr and Ba) glasses are theoretically investigated by using the perturbation formulas of the EPR parameters for tetragonally compressed octahedral 3d1 and tetragonally elongated octahedral 3d9 clusters, respectively. The VO2+ and Cu2+ dopants are found to undergo the tetragonal compression (characterized by the negative relative distortion ratios ρ ≈ -3%, -0.98%, -1% and -0.8% for R = Zn, Mg, Sr and Ba) and elongation (characterized by the positive relative distortion ratios ρ ≈ 29%, 17%, 16% and 28%), respectively, due to the Jahn-Teller effect. Both dopants show similar overall decreasing trends of cubic field parameter Dq and covalency factor N with decreasing electronegativity of alkali earth cation R. The conventional optical basicities Λth and <span class="hlt">local</span> optical basicities Λloc are calculated for both systems, and the <span class="hlt">local</span> Λloc are higher for Cu2+ than for VO2+ in the same RLNKB glass, despite the opposite relationship for the conventional Λth. This point is supported by the weaker covalency or stronger ionicity for Cu2+ than VO2+ in the same RLNKB system, characterized by the larger N in the former. The above comparative analysis on the spectral and <span class="hlt">local</span> <span class="hlt">structural</span> properties would be helpful to understand <span class="hlt">structures</span> and spectroscopic properties for the similar oxide glasses with transition-metal dopants of complementary <span class="hlt">electronic</span> configurations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21351757','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21351757"><span>Proton-coupled <span class="hlt">electron</span> transfer versus hydrogen atom transfer: generation of charge-<span class="hlt">localized</span> diabatic states.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sirjoosingh, Andrew; Hammes-Schiffer, Sharon</p> <p>2011-03-24</p> <p>The distinction between proton-coupled <span class="hlt">electron</span> transfer (PCET) and hydrogen atom transfer (HAT) mechanisms is important for the characterization of many chemical and biological processes. PCET and HAT mechanisms can be differentiated in terms of <span class="hlt">electronically</span> nonadiabatic and adiabatic proton transfer, respectively. In this paper, quantitative diagnostics to evaluate the degree of <span class="hlt">electron</span>-proton nonadiabaticity are presented. Moreover, the connection between the degree of <span class="hlt">electron</span>-proton nonadiabaticity and the physical characteristics distinguishing PCET from HAT, namely, the extent of <span class="hlt">electronic</span> charge redistribution, is clarified. In addition, a rigorous diabatization scheme for transforming the adiabatic <span class="hlt">electronic</span> states into charge-<span class="hlt">localized</span> diabatic states for PCET reactions is presented. These diabatic states are constructed to ensure that the first-order nonadiabatic couplings with respect to the one-dimensional transferring hydrogen coordinate vanish exactly. Application of these approaches to the phenoxyl-phenol and benzyl-toluene systems characterizes the former as PCET and the latter as HAT. The diabatic states generated for the phenoxyl-phenol system possess physically meaningful, <span class="hlt">localized</span> <span class="hlt">electronic</span> charge distributions that are relatively invariant along the hydrogen coordinate. These diabatic <span class="hlt">electronic</span> states can be combined with the associated proton vibrational states to generate the reactant and product <span class="hlt">electron</span>-proton vibronic states that form the basis of nonadiabatic PCET theories. Furthermore, these vibronic states and the corresponding vibronic couplings may be used to calculate rate constants and kinetic isotope effects of PCET reactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910060168&hterms=research+methods&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dresearch%2Bmethods','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910060168&hterms=research+methods&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dresearch%2Bmethods"><span>Global/<span class="hlt">local</span> methods research using a common <span class="hlt">structural</span> analysis framework</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Knight, Norman F., Jr.; Ransom, Jonathan B.; Griffin, O. H., Jr.; Thompson, Danniella M.</p> <p>1991-01-01</p> <p>Methodologies for global/<span class="hlt">local</span> stress analysis are described including both two- and three-dimensional analysis methods. These methods are being developed within a common <span class="hlt">structural</span> analysis framework. Representative <span class="hlt">structural</span> analysis problems are presented to demonstrate the global/<span class="hlt">local</span> methodologies being developed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19466857','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19466857"><span><span class="hlt">Structural</span>, <span class="hlt">electronic</span>, and vibrational properties of high-density amorphous silicon: a first-principles molecular-dynamics study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Morishita, Tetsuya</p> <p>2009-05-21</p> <p>We report a first-principles study of the <span class="hlt">structural</span>, <span class="hlt">electronic</span>, and dynamical properties of high-density amorphous (HDA) silicon, which was found to be formed by pressurizing low-density amorphous (LDA) silicon (a normal amorphous Si) [T. Morishita, Phys. Rev. Lett. 93, 055503 (2004); P. F. McMillan, M. Wilson, D. Daisenberger, and D. Machon, Nature Mater. 4, 680 (2005)]. Striking <span class="hlt">structural</span> differences between HDA and LDA are revealed. The LDA <span class="hlt">structure</span> holds a tetrahedral network, while the HDA <span class="hlt">structure</span> contains a highly distorted tetrahedral network. The fifth neighboring atom in HDA tends to be located at an interstitial position of a distorted tetrahedron composed of the first four neighboring atoms. Consequently, the coordination number of HDA is calculated to be approximately 5 unlike that of LDA. The <span class="hlt">electronic</span> density of state (EDOS) shows that HDA is metallic, which is consistent with a recent experimental measurement of the <span class="hlt">electronic</span> resistance of HDA Si. We find from <span class="hlt">local</span> EDOS that highly distorted tetrahedral configurations enhance the metallic nature of HDA. The vibrational density of state (VDOS) also reflects the <span class="hlt">structural</span> differences between HDA and LDA. Some of the characteristic vibrational modes of LDA are dematerialized in HDA, indicating the degradation of covalent bonds. The overall profile of the VDOS for HDA is found to be an intermediate between that for LDA and liquid Si under pressure (high-density liquid Si).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20640084-exploration-momentum-evolution-three-dimensional-localization-recombined-electron-wave-packets','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20640084-exploration-momentum-evolution-three-dimensional-localization-recombined-electron-wave-packets"><span>Exploration of momentum evolution and three-dimensional <span class="hlt">localization</span> in recombined <span class="hlt">electron</span> wave packets</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>Zeibel, J. G.; Jones, R. R.</p> <p>2003-08-01</p> <p>Picosecond ''half-cycle'' pulses (HCPs) have been used to produce <span class="hlt">electronic</span> wave packets by recombining photoelectrons with their parent ions. The time-dependent momentum distributions of the bound wave packets are probed using a second HCP and the impulsive momentum retrieval (IMR) method. For a given delay between the initial photoionization event and the HCP recombination, classical trajectory simulations predict pronounced periodic wave packet motion for a restricted range of recombining HCP amplitudes. This motion is characterized by the repeated formation and collapse of a highly <span class="hlt">localized</span> spike in the three-dimensional <span class="hlt">electron</span> probability density at a large distance from the nucleus. Ourmore » experiments confirm that oscillatory wave packet motion occurs only for certain recombination ''kick'' strengths. Moreover, the measured time-dependent momentum distributions are consistent with the predicted formation of a highly <span class="hlt">localized</span> <span class="hlt">electron</span> packet. We demonstrate a variation of the IMR in which amplitude modulation of the HCP probe field is employed to suppress noise and allow for a more direct recovery of <span class="hlt">electron</span> momentum from experimental ionization data.« 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_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/1989RvMP...61..433P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1989RvMP...61..433P"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of the high-temperature oxide superconductors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pickett, Warren E.</p> <p>1989-04-01</p> <p>Since the discovery of superconductivity above 30 K by Bednorz and Müller in the La copper oxide system, the critical temperature has been raised to 90 K in YBa2Cu3O7 and to 110 and 125 K in Bi-based and Tl-based copper oxides, respectively. In the two years since this Nobel-prize-winning discovery, a large number of <span class="hlt">electronic</span> <span class="hlt">structure</span> calculations have been carried out as a first step in understanding the <span class="hlt">electronic</span> properties of these materials. In this paper these calculations (mostly of the density-functional type) are gathered and reviewed, and their results are compared with the relevant experimental data. The picture that emerges is one in which the important <span class="hlt">electronic</span> states are dominated by the copper d and oxygen p orbitals, with strong hybridization between them. Photon, <span class="hlt">electron</span>, and positron spectroscopies provide important information about the <span class="hlt">electronic</span> states, and comparison with <span class="hlt">electronic</span> <span class="hlt">structure</span> calculations indicates that, while many features can be interpreted in terms of existing calculations, self-energy corrections ("correlations") are important for a more detailed understanding. The antiferromagnetism that occurs in some regions of the phase diagram poses a particularly challenging problem for any detailed theory. The study of <span class="hlt">structural</span> stability, lattice dynamics, and <span class="hlt">electron</span>-phonon coupling in the copper oxides is also discussed. Finally, a brief review is given of the attempts so far to identify interaction constants appropriate for a model Hamiltonian treatment of many-body interactions in these materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=sarkar&pg=4&id=EJ754983','ERIC'); return false;" href="https://eric.ed.gov/?q=sarkar&pg=4&id=EJ754983"><span><span class="hlt">Electronic</span> <span class="hlt">Structure</span> Principles and Aromaticity</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>Chattaraj, P. K.; Sarkar, U.; Roy, D. R.</p> <p>2007-01-01</p> <p>The relationship between aromaticity and stability in molecules on the basis of quantities such as hardness and electrophilicity is explored. The findings reveal that aromatic molecules are less energetic, harder, less polarizable, and less electrophilic as compared to antiaromatic molecules, as expected from the <span class="hlt">electronic</span> <span class="hlt">structure</span> principles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170004859&hterms=porter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D30%26Ntt%3Dporter','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170004859&hterms=porter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D30%26Ntt%3Dporter"><span>The <span class="hlt">Structure</span> of the <span class="hlt">Local</span> Hot Bubble</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Liu, W.; Chiao, M.; Collier, M. R.; Cravens, T.; Galeazzi, M.; Koutroumpa, D.; Kuntz, K. D.; Lallement, R.; Lepri, S. T.; McCammon, Dan; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170004859'); toggleEditAbsImage('author_20170004859_show'); toggleEditAbsImage('author_20170004859_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170004859_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170004859_hide"></p> <p>2016-01-01</p> <p>Diffuse X-rays from the <span class="hlt">Local</span> Galaxy (DXL) is a sounding rocket mission designed to quantify and characterize the contribution of Solar Wind Charge eXchange (SWCX) to the Diffuse X-ray Background and study the properties of the <span class="hlt">Local</span> Hot Bubble (LHB). Based on the results from the DXL mission, we quantified and removed the contribution of SWCX to the diffuse X-ray background measured by the ROSAT All Sky Survey. The cleaned maps were used to investigate the physical properties of the LHB. Assuming thermal ionization equilibrium, we measured a highly uniform temperature distributed around kT = 0.097 keV +/- 0.013 keV (FWHM) +/- 0.006 keV(systematic). We also generated a thermal emission measure map and used it to characterize the three-dimensional (3D) <span class="hlt">structure</span> of the LHB, which we found to be in good agreement with the <span class="hlt">structure</span> of the <span class="hlt">local</span> cavity measured from dust and gas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1060120-molecular-structure-free-energy-landscape-electron-transport-deca-heme-cytochrome-mtrf','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1060120-molecular-structure-free-energy-landscape-electron-transport-deca-heme-cytochrome-mtrf"><span>Molecular <span class="hlt">Structure</span> and Free Energy Landscape for <span class="hlt">Electron</span> Transport in the Deca-Heme Cytochrome MtrF</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>Breuer, Marian; Zarzycki, Piotr P.; Shi, Liang</p> <p>2012-12-01</p> <p>The free energy profile for <span class="hlt">electron</span> flow through the bacterial deca-heme cytochrome MtrF has been computed using thermodynamic integration and classical molecular dynamics. The extensive calculations on two versions of the <span class="hlt">structure</span> help validate the method and results, because differences in the profiles can be related to differences in the charged amino acids <span class="hlt">local</span> to specific heme groups. First estimates of reorganization free energies λ yield a range consistent with expectations for partially solvent exposed cofactors, and reveal an activation energy range surmountable for <span class="hlt">electron</span> flow. Future work will aim at increasing the accuracy of λ with polarizable force fieldmore » dynamics and quantum chemical energy gap calculations, as well as quantum chemical computation of <span class="hlt">electronic</span> coupling matrix elements.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999JChEd..76.1463M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999JChEd..76.1463M"><span>Writing <span class="hlt">Electron</span> Dot <span class="hlt">Structures</span>: Abstract of Issue 9905M</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Magnell, Kenneth R.</p> <p>1999-10-01</p> <p>Writing <span class="hlt">Electron</span> Dot <span class="hlt">Structures</span> is a computer program for Mac OS that provides drill with feedback for students learning to write <span class="hlt">electron</span> dot <span class="hlt">structures</span>. While designed for students in the first year of college general chemistry it may also be used by high school chemistry students. A systematic method similar to that found in many general chemistry texts is employed: <OL TYPE="1"> <LI>determine the number of valence shell <span class="hlt">electrons</span>, <LI>select the central atom, <LI>construct a skeleton, <LI>add <span class="hlt">electrons</span> to complete octets, <LI>examine the <span class="hlt">structure</span> for resonance forms. </OL> During the construction of a <span class="hlt">structure</span>, the student has the option of quitting, selecting another formula, or returning to a previous step. If an incorrect number of <span class="hlt">electrons</span> is entered the student may not proceed until the correct number is entered. The symbol entered for the central atom must follow accepted upper/lower case practice, and entry of the correct symbol must be accomplished before proceeding to the next step. A periodic table is accessible and feedback provides assistance for these steps. Construction of the skeleton begins with the placement of the central atom. Atoms can be added, moved, or removed. Prompts and feedback keep the student informed of progress and problems. A correct skeleton is required before proceeding to the next step. Completion of the <span class="hlt">structure</span> begins with the addition of <span class="hlt">electron</span> pairs to form the required bonds. Remaining <span class="hlt">electrons</span> are added to complete the formation of multiple bonds, assure compliance with the octet rule, and form expanded octets. Resonance forms are made by moving or removing and replacing <span class="hlt">electron</span> pairs in the existing skeleton. Prompts and feedback guide the student through this process. A running tally of bond pairs, unshared pairs, octets, <span class="hlt">electrons</span> used, and <span class="hlt">electrons</span> remaining is provided during this step. <IMG SRC="Images/Oct99p1463_1.gif" width="194" height="146"> <IMG SRC="Images/Oct99p1463_2.gif" width="194" height="146</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PCM....39..713A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PCM....39..713A"><span><span class="hlt">Local</span> <span class="hlt">structural</span> relaxation around Co2+ along the hardystonite-Co-åkermanite melilite solid solution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ardit, Matteo; Cruciani, Giuseppe; Dondi, Michele</p> <p>2012-10-01</p> <p>Six pure compounds belonging to the hardystonite (Ca2ZnSi2O7)-Co-åkermanite (Ca2CoSi2O7) solid solution were investigated by the combined application of X-ray powder diffraction and <span class="hlt">electronic</span> absorption spectroscopy. <span class="hlt">Structural</span> refinements of the XRPD data revealed a negative excess volume of mixing due to the single isovalent substitution of Co for Zn in the tetrahedral site. In agreement with the diffraction data, deconvolution of the optical spectra showed a progressive decreasing of the crystal field strength parameter 10 Dq moving toward the Co-åkermanite end-member, meaning that the <span class="hlt">local</span> cobalt-oxygen bond distance, < {{Co}}{-}{{O}}rangle^{{<span class="hlt">local</span>}} , increased along the join with the amount of cobalt. The calculated <span class="hlt">structural</span> relaxation coefficient around the fourfold coordinated Co2+ in the Ca2(Zn1- x Co x )Si2O7 join was ɛ = 0.69, very far from the one predicted by the Vegard's law ( ɛ = 0) and at variance with ɛ = 0.47 previously found for tetrahedrally coordinated Co2+ in gahnite-Co-aluminate spinel solid solution. This difference is consistent with the largest constraints existing on the spinel <span class="hlt">structure</span>, based on cubic closest packing, compared to the more flexible layered melilite <span class="hlt">structure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29150657','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29150657"><span>Specific heat, Electrical resistivity and <span class="hlt">Electronic</span> band <span class="hlt">structure</span> properties of noncentrosymmetric Th7Fe3 superconductor.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tran, V H; Sahakyan, M</p> <p>2017-11-17</p> <p>Noncentrosymmetric superconductor Th 7 Fe 3 has been investigated by means of specific heat, electrical resisitivity measurements and <span class="hlt">electronic</span> properties calculations. Sudden drop in the resistivity at 2.05 ± 0.15 K and specific heat jump at 1.98 ± 0.02 K are observed, rendering the superconducting transition. A model of two BCS-type gaps appears to describe the zero-magnetic-field specific heat better than those based on the isotropic BCS theory or anisotropic functions. A positive curvature of the upper critical field H c2 (T c ) and nonlinear field dependence of the Sommerfeld coefficient at 0.4 K qualitatively support the two-gap scenario, which predicts H c2 (0) = 13 kOe. The theoretical densities of states and <span class="hlt">electronic</span> band <span class="hlt">structures</span> (EBS) around the Fermi energy show a mixture of Th 6d- and Fe 3d-<span class="hlt">electrons</span> bands, being responsible for the superconductivity. Furthermore, the EBS and Fermi surfaces disclose significantly anisotropic splitting associated with asymmetric spin-orbit coupling (ASOC). The ASOC sets up also multiband <span class="hlt">structure</span>, which presumably favours a multigap superconductivity. <span class="hlt">Electron</span> <span class="hlt">Localization</span> Function reveals the existence of both metallic and covalent bonds, the latter may have different strengths depending on the regions close to the Fe or Th atoms. The superconducting, <span class="hlt">electronic</span> properties and implications of asymmetric spin-orbit coupling associated with noncentrosymmetric <span class="hlt">structure</span> are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1995003','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1995003"><span><span class="hlt">Local</span> backbone <span class="hlt">structure</span> prediction of proteins</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 Brevern, Alexandre G.; Benros, Cristina; Gautier, Romain; Valadié, Hélène; Hazout, Serge; Etchebest, Catherine</p> <p>2004-01-01</p> <p>Summary A statistical analysis of the PDB <span class="hlt">structures</span> has led us to define a new set of small 3D <span class="hlt">structural</span> prototypes called Protein Blocks (PBs). This <span class="hlt">structural</span> alphabet includes 16 PBs, each one is defined by the (φ, Ψ) dihedral angles of 5 consecutive residues. The amino acid distributions observed in sequence windows encompassing these PBs are used to predict by a Bayesian approach the <span class="hlt">local</span> 3D <span class="hlt">structure</span> of proteins from the sole knowledge of their sequences. LocPred is a software which allows the users to submit a protein sequence and performs a prediction in terms of PBs. The prediction results are given both textually and graphically. PMID:15724288</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JChPh.133q4114K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JChPh.133q4114K"><span>State-selective optimization of <span class="hlt">local</span> excited <span class="hlt">electronic</span> states in extended systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kovyrshin, Arseny; Neugebauer, Johannes</p> <p>2010-11-01</p> <p>Standard implementations of time-dependent density-functional theory (TDDFT) for the calculation of excitation energies give access to a number of the lowest-lying <span class="hlt">electronic</span> excitations of a molecule under study. For extended systems, this can become cumbersome if a particular excited state is sought-after because many <span class="hlt">electronic</span> transitions may be present. This often means that even for systems of moderate size, a multitude of excited states needs to be calculated to cover a certain energy range. Here, we present an algorithm for the selective determination of predefined excited <span class="hlt">electronic</span> states in an extended system. A guess transition density in terms of orbital transitions has to be provided for the excitation that shall be optimized. The approach employs root-homing techniques together with iterative subspace diagonalization methods to optimize the <span class="hlt">electronic</span> transition. We illustrate the advantages of this method for solvated molecules, core-excitations of metal complexes, and adsorbates at cluster surfaces. In particular, we study the <span class="hlt">local</span> π →π∗ excitation of a pyridine molecule adsorbed at a silver cluster. It is shown that the method works very efficiently even for high-lying excited states. We demonstrate that the assumption of a single, well-defined <span class="hlt">local</span> excitation is, in general, not justified for extended systems, which can lead to root-switching during optimization. In those cases, the method can give important information about the spectral distribution of the orbital transition employed as a guess.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28869874','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28869874"><span>Effects of micro-<span class="hlt">structure</span> on aerodynamics of Coccinella septempunctata elytra (ladybird) in forward flight as assessed via <span class="hlt">electron</span> microscopy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Xiang, Jinwu; Liu, Kai; Li, Daochun; Du, Jianxun</p> <p>2017-11-01</p> <p>The effects of micro-<span class="hlt">structure</span> on aerodynamics of Coccinella septempunctata (Coleoptera: Coccinellidae) elytra in forward flight were investigated. The micro-<span class="hlt">structure</span> was examined by a scanning <span class="hlt">electron</span> microscope and a digital microscope. Based on the experimental results, five elytron models were constructed to separately investigate the effects of the camber and the <span class="hlt">local</span> corrugation in both leading edge and trailing edge on aerodynamics. Computational fluid dynamic simulations of five elytron models were conducted by solving the Reynolds-Averaged Navier-Stokes equations with the Reynolds number of 245. The results show that camber and the <span class="hlt">local</span> corrugation in the leading edge play significant roles in improving the aerodynamic performance, while the <span class="hlt">local</span> corrugation in the trailing edge has little effect on aerodynamics. Copyright © 2017 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25969148','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25969148"><span>A real-space stochastic density matrix approach for density functional <span class="hlt">electronic</span> <span class="hlt">structure</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Beck, Thomas L</p> <p>2015-12-21</p> <p>The recent development of real-space grid methods has led to more efficient, accurate, and adaptable approaches for large-scale electrostatics and density functional <span class="hlt">electronic</span> <span class="hlt">structure</span> modeling. With the incorporation of multiscale techniques, linear-scaling real-space solvers are possible for density functional problems if <span class="hlt">localized</span> orbitals are used to represent the Kohn-Sham energy functional. These methods still suffer from high computational and storage overheads, however, due to extensive matrix operations related to the underlying wave function grid representation. In this paper, an alternative stochastic method is outlined that aims to solve directly for the one-<span class="hlt">electron</span> density matrix in real space. In order to illustrate aspects of the method, model calculations are performed for simple one-dimensional problems that display some features of the more general problem, such as spatial nodes in the density matrix. This orbital-free approach may prove helpful considering a future involving increasingly parallel computing architectures. Its primary advantage is the near-<span class="hlt">locality</span> of the random walks, allowing for simultaneous updates of the density matrix in different regions of space partitioned across the processors. In addition, it allows for testing and enforcement of the particle number and idempotency constraints through stabilization of a Feynman-Kac functional integral as opposed to the extensive matrix operations in traditional approaches.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97o5109M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97o5109M"><span>Pseudogap and <span class="hlt">electronic</span> <span class="hlt">structure</span> of <span class="hlt">electron</span>-doped Sr2IrO4</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moutenet, Alice; Georges, Antoine; Ferrero, Michel</p> <p>2018-04-01</p> <p>We present a theoretical investigation of the effects of correlations on the <span class="hlt">electronic</span> <span class="hlt">structure</span> of the Mott insulator Sr2IrO4 upon <span class="hlt">electron</span> doping. A rapid collapse of the Mott gap upon doping is found, and the <span class="hlt">electronic</span> <span class="hlt">structure</span> displays a strong momentum-space differentiation at low doping level: The Fermi surface consists of pockets centered around (π /2 ,π /2 ) , while a pseudogap opens near (π ,0 ) . Its physical origin is shown to be related to short-range spin correlations. The pseudogap closes upon increasing doping, but a differentiated regime characterized by a modulation of the spectral intensity along the Fermi surface persists to higher doping levels. These results, obtained within the cellular dynamical mean-field-theory framework, are discussed in comparison to recent photoemission experiments and an overall good agreement is found.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25124437','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25124437"><span>Photosynthesis. <span class="hlt">Electronic</span> <span class="hlt">structure</span> of the oxygen-evolving complex in photosystem II prior to O-O bond formation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cox, Nicholas; Retegan, Marius; Neese, Frank; Pantazis, Dimitrios A; Boussac, Alain; Lubitz, Wolfgang</p> <p>2014-08-15</p> <p>The photosynthetic protein complex photosystem II oxidizes water to molecular oxygen at an embedded tetramanganese-calcium cluster. Resolving the geometric and <span class="hlt">electronic</span> <span class="hlt">structure</span> of this cluster in its highest metastable catalytic state (designated S3) is a prerequisite for understanding the mechanism of O-O bond formation. Here, multifrequency, multidimensional magnetic resonance spectroscopy reveals that all four manganese ions of the catalyst are <span class="hlt">structurally</span> and <span class="hlt">electronically</span> similar immediately before the final oxygen evolution step; they all exhibit a 4+ formal oxidation state and octahedral <span class="hlt">local</span> geometry. Only one <span class="hlt">structural</span> model derived from quantum chemical modeling is consistent with all magnetic resonance data; its formation requires the binding of an additional water molecule. O-O bond formation would then proceed by the coupling of two proximal manganese-bound oxygens in the transition state of the cofactor. Copyright © 2014, American Association for the Advancement of Science.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920012412','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920012412"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> Fermi liquid theory of high Tc superconductors: Comparison of predictions with experiments</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yu, Jaejun; Freeman, A. J.</p> <p>1991-01-01</p> <p>Predictions of <span class="hlt">local</span> density functional (LDF) calculations of the <span class="hlt">electronic</span> <span class="hlt">structure</span> and transport properties of high T(sub c) superconductors are presented. As evidenced by the excellent agreement with both photoemission and positron annihilation experiments, a Fermi liquid nature of the 'normal' state of the high T(sub c) superconductors become clear for the metallic phase of these oxides. In addition, LDF predictions on the normal state transport properties are qualitatively in agreement with experiments on single crystals. It is emphasized that the signs of the Hall coefficients for the high T(sub c) superconductors are not consistent with the types of dopants (e.g., <span class="hlt">electron</span>-doped or hole-doped) but are determined by the topology of the Fermi surfaces obtained from the LDF calculations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JAP...116s3709M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JAP...116s3709M"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> and optical properties of CdSxSe1-x solid solution nanostructures from X-ray absorption near edge <span class="hlt">structure</span>, X-ray excited optical luminescence, and density functional theory investigations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Murphy, M. W.; Yiu, Y. M.; Ward, M. J.; Liu, L.; Hu, Y.; Zapien, J. A.; Liu, Yingkai; Sham, T. K.</p> <p>2014-11-01</p> <p>The <span class="hlt">electronic</span> <span class="hlt">structure</span> and optical properties of a series of iso-<span class="hlt">electronic</span> and iso-<span class="hlt">structural</span> CdSxSe1-x solid solution nanostructures have been investigated using X-ray absorption near edge <span class="hlt">structure</span>, extended X-ray absorption fine <span class="hlt">structure</span>, and X-ray excited optical luminescence at various absorption edges of Cd, S, and Se. It is found that the system exhibits compositions, with variable <span class="hlt">local</span> <span class="hlt">structure</span> in-between that of CdS and CdSe accompanied by tunable optical band gap between that of CdS and CdSe. Theoretical calculation using density functional theory has been carried out to elucidate the observations. It is also found that luminescence induced by X-ray excitation shows new optical channels not observed previously with laser excitation. The implications of these observations are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28759072','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28759072"><span>Mechanical properties and <span class="hlt">electronic</span> <span class="hlt">structure</span> of edge-doped graphene nanoribbons with F, O, and Cl atoms.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Piriz, Sebastián; Fernández-Werner, Luciana; Pardo, Helena; Jasen, Paula; Faccio, Ricardo; Mombrú, Álvaro W</p> <p>2017-08-16</p> <p>In this study, we present the <span class="hlt">structural</span>, <span class="hlt">electronic</span>, and mechanical properties of edge-doped zigzag graphene nanoribbons (ZGNRs) doped with fluorine, oxygen, and chlorine atoms. To the best of our knowledge, to date, no experimental results concerning the mechanical properties of graphene-derived nanoribbons have been reported in the literature. Simulations indicate that Cl- and F-doped ZGNRs present an equivalent 2-dimensional Young's modulus E 2D , which seems to be higher than those of graphene and H-doped ZGNRs. This is a consequence of the <span class="hlt">electronic</span> <span class="hlt">structure</span> of the system, particularly originating from strong interactions between the dopant atoms <span class="hlt">localized</span> at the edges. The interaction between dopant atoms located at the edges is higher for Cl and lower for F and O atoms. This is the origin of the observed trend, in which E > E > E for all the analyzed ZGNRs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22679004-mixed-cerium-platinum-oxides-electronic-structure-ceo-pt-sub-ceo-sub-pt-complex-anions-neutrals','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22679004-mixed-cerium-platinum-oxides-electronic-structure-ceo-pt-sub-ceo-sub-pt-complex-anions-neutrals"><span>Mixed cerium-platinum oxides: <span class="hlt">Electronic</span> <span class="hlt">structure</span> of [CeO]Pt{sub n} (n = 1, 2) and [CeO{sub 2}]Pt complex anions and neutrals</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>Ray, Manisha; Kafader, Jared O.; Topolski, Josey E.</p> <p></p> <p>The <span class="hlt">electronic</span> <span class="hlt">structures</span> of several small Ce–Pt oxide complexes were explored using a combination of anion photoelectron (PE) spectroscopy and density functional theory calculations. Pt and Pt{sub 2} both accept <span class="hlt">electron</span> density from CeO diatomic molecules, in which the cerium atom is in a lower-than-bulk oxidation state (+2 versus bulk +4). Neutral [CeO]Pt and [CeO]Pt{sub 2} complexes are therefore ionic, with <span class="hlt">electronic</span> <span class="hlt">structures</span> described qualitatively as [CeO{sup +2}]Pt{sup −2} and [CeO{sup +}]Pt{sub 2}{sup −}, respectively. The associated anions are described qualitatively as [CeO{sup +}]Pt{sup −2} and [CeO{sup +}]Pt{sub 2}{sup −2}, respectively. In both neutrals and anions, the most stable molecularmore » <span class="hlt">structures</span> determined by calculations feature a distinct CeO moiety, with the positively charged Ce center pointing toward the <span class="hlt">electron</span> rich Pt or Pt{sub 2} moiety. Spectral simulations based on calculated spectroscopic parameters are in fair agreement with the spectra, validating the computationally determined <span class="hlt">structures</span>. In contrast, when Pt is coupled with CeO{sub 2}, which has no Ce-<span class="hlt">localized</span> <span class="hlt">electrons</span> that can readily be donated to Pt, the anion is described as [CeO{sub 2}]Pt{sup −}. The molecular <span class="hlt">structure</span> predicted computationally suggests that it is governed by charge-dipole interactions. The neutral [CeO{sub 2}]Pt complex lacks charge-dipole stabilizing interactions, and is predicted to be <span class="hlt">structurally</span> very different from the anion, featuring a single Pt–O–Ce bridge bond. The PE spectra of several of the complexes exhibit evidence of photodissociation with Pt{sup −} daughter ion formation. The <span class="hlt">electronic</span> <span class="hlt">structures</span> of these complexes are related to <span class="hlt">local</span> interactions in Pt-ceria catalyst-support systems.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhDT.......313M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhDT.......313M"><span>Exploring the <span class="hlt">Electronic</span> Landscape at Interfaces and Junctions in Semiconductor Nanowire Devices with Subsurface <span class="hlt">Local</span> Probing of Carrier Dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McGuckin, Terrence</p> <p></p> <p>The solid state devices that are pervasive in our society, are based on building blocks composed of interfaces between materials and junctions that manipulate how charge carriers behave in a device. As the dimensions of these devices are reduced to the nanoscale, surfaces and interfaces play a larger role in the behavior of carriers in devices and must be thoroughly investigated to understand not only the material properties but how these materials interact. Separating the effects of these different building blocks is a challenge, as most testing methods measure the performance of the whole device. Semiconductor nanowires represent an excellent test system to explore the limits of size and novel device <span class="hlt">structures</span>. The behavior of charge carriers in semiconductor nanowire devices under operational conditions is investigated using <span class="hlt">local</span> probing technique <span class="hlt">electron</span> beam induced current (EBIC). The behavior of <span class="hlt">locally</span> excited carriers are driven by the forces of drift, from electric fields within a device at junctions, surfaces, contacts and, applied voltage bias, and diffusion. This thesis presents the results of directly measuring these effects spatially with nanometer resolution, using EBIC in Ge, Si, and complex heterostructure GaAs/AlGaAs nanowire devices. Advancements to the EBIC technique, have pushed the resolution from tens of nanometers down to 1 to 2 nanometers. Depth profiling and tuning of the interaction volume allows for the separating the signal originating from the surface and the interior of the nanowire. Radial junctions and variations in bands can now be analyzed including core/shell hetero-<span class="hlt">structures</span>. This <span class="hlt">local</span> carrier probing reveals a number of surprising behaviors; Most notably, directly imaging the evolution of surface traps filling with <span class="hlt">electrons</span> causing bandbending at the surface of Ge nanowires that leads to an enhancement in the charge separation of <span class="hlt">electrons</span> and holes, and extracting different characteristic lengths from GaAs and AlGaAs in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016isms.confETJ08K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016isms.confETJ08K"><span><span class="hlt">Electronic</span> <span class="hlt">Structure</span> of Small Lanthanide Containing Molecules</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kafader, Jared O.; Ray, Manisha; Topolski, Josey E.; Chick Jarrold, Caroline</p> <p>2016-06-01</p> <p>Lanthanide-based materials have unusual <span class="hlt">electronic</span> properties because of the high number of <span class="hlt">electronic</span> degrees of freedom arising from partial occupation of 4f orbitals, which make these materials optimal for their utilization in many applications including <span class="hlt">electronics</span> and catalysis. <span class="hlt">Electronic</span> spectroscopy of small lanthanide molecules helps us understand the role of these 4f <span class="hlt">electrons</span>, which are generally considered core-like because of orbital contraction, but are energetically similar to valence <span class="hlt">electrons</span>. The spectroscopy of small lanthanide-containing molecules is relatively unexplored and to broaden this understanding we have completed the characterization of small cerium, praseodymium, and europium molecules using photoelectron spectroscopy coupled with DFT calculations. The characterization of PrO, EuH, EuO/EuOH, and CexOy molecules have allowed for the determination of their <span class="hlt">electron</span> affinity, the assignment of numerous anion to neutral state transitions, modeling of anion/neutral <span class="hlt">structures</span> and <span class="hlt">electron</span> orbital occupation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.osti.gov/accomplishments/hofstadter.html','SCIGOVWS'); return false;" href="http://www.osti.gov/accomplishments/hofstadter.html"><span>Robert Hofstadter, <span class="hlt">Electron</span> Scattering, the <span class="hlt">Structure</span> of the Nucleons, and</span></a></p> <p><a target="_blank" href="http://www.science.gov/aboutsearch.html">Science.gov Websites</a></p> <p></p> <p></p> <p>, <span class="hlt">Electron</span> Scattering, the <em><span class="hlt">Structure</span></em> of the Nucleons, and Scintillation Counters Resources with Additional -point particles and therefore possessed <em><span class="hlt">structure</span></em>. For this work Hofstadter was awarded the Nobel Prize <em><span class="hlt">structure</span></em> of the nucleons, and scintillation counters is available in <span class="hlt">electronic</span> documents and on the Web</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/2017PhRvB..95k5409D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvB..95k5409D"><span><span class="hlt">Structural</span> and <span class="hlt">electronic</span> properties of monolayer group III monochalcogenides</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Demirci, S.; Avazlı, N.; Durgun, E.; Cahangirov, S.</p> <p>2017-03-01</p> <p>We investigate the <span class="hlt">structural</span>, mechanical, and <span class="hlt">electronic</span> properties of the two-dimensional hexagonal <span class="hlt">structure</span> of group III-VI binary monolayers, M X (M =B , Al, Ga, In and X =O , S, Se, Te) using first-principles calculations based on the density functional theory. The <span class="hlt">structural</span> optimization calculations and phonon spectrum analysis indicate that all of the 16 possible binary compounds are thermally stable. In-plane stiffness values cover a range depending on the element types and can be as high as that of graphene, while the calculated bending rigidity is found to be an order of magnitude higher than that of graphene. The obtained <span class="hlt">electronic</span> band <span class="hlt">structures</span> show that M X monolayers are indirect band-gap semiconductors. The calculated band gaps span a wide optical spectrum from deep ultraviolet to near infrared. The <span class="hlt">electronic</span> <span class="hlt">structure</span> of oxides (M O ) is different from the rest because of the high electronegativity of oxygen atoms. The dispersions of the <span class="hlt">electronic</span> band edges and the nature of bonding between atoms can also be correlated with electronegativities of constituent elements. The unique characteristics of group III-VI binary monolayers can be suitable for high-performance device applications in nanoelectronics and optics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29251496','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29251496"><span><span class="hlt">Electron</span>-Poor Polar Intermetallics: Complex <span class="hlt">Structures</span>, Novel Clusters, and Intriguing Bonding with Pronounced <span class="hlt">Electron</span> Delocalization.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lin, Qisheng; Miller, Gordon J</p> <p>2018-01-16</p> <p>Intermetallic compounds represent an extensive pool of candidates for energy related applications stemming from magnetic, electric, optic, caloric, and catalytic properties. The discovery of novel intermetallic compounds can enhance understanding of the chemical principles that govern <span class="hlt">structural</span> stability and chemical bonding as well as finding new applications. Valence <span class="hlt">electron</span>-poor polar intermetallics with valence <span class="hlt">electron</span> concentrations (VECs) between 2.0 and 3.0 e - /atom show a plethora of unprecedented and fascinating <span class="hlt">structural</span> motifs and bonding features. Therefore, establishing simple <span class="hlt">structure</span>-bonding-property relationships is especially challenging for this compound class because commonly accepted valence <span class="hlt">electron</span> counting rules are inappropriate. During our efforts to find quasicrystals and crystalline approximants by valence <span class="hlt">electron</span> tuning near 2.0 e - /atom, we observed that compositions close to those of quasicrystals are exceptional sources for unprecedented valence <span class="hlt">electron</span>-poor polar intermetallics, e.g., Ca 4 Au 10 In 3 containing (Au 10 In 3 ) wavy layers, Li 14.7 Mg 36.8 Cu 21.5 Ga 66 adopting a type IV clathrate framework, and Sc 4 Mg x Cu 15-x Ga 7.5 that is incommensurately modulated. In particular, exploratory syntheses of AAu 3 T (A = Ca, Sr, Ba and T = Ge, Sn) phases led to interesting bonding features for Au, such as columns, layers, and lonsdaleite-type tetrahedral frameworks. Overall, the breadth of Au-rich polar intermetallics originates, in part, from significant relativistics effect on the valence <span class="hlt">electrons</span> of Au, effects which result in greater 6s/5d orbital mixing, a small effective metallic radius, and an enhanced Mulliken electronegativity, all leading to ultimate enhanced binding with nearly all metals including itself. Two other successful strategies to mine <span class="hlt">electron</span>-poor polar intermetallics include lithiation and "cation-rich" phases. Along these lines, we have studied lithiated Zn-rich compounds in which <span class="hlt">structural</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1372984-structure-stability-cah-surfaces-possibility-electron-rich-surfaces-metal-hydrides-catalysis','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1372984-structure-stability-cah-surfaces-possibility-electron-rich-surfaces-metal-hydrides-catalysis"><span><span class="hlt">Structure</span> and stability of CaH 2 surfaces: on the possibility of <span class="hlt">electron</span>-rich surfaces in metal hydrides for catalysis</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>Ong, Phuong-Vu; Johnson, Lewis E.; Hosono, Hideo</p> <p></p> <p><span class="hlt">Structure</span>, thermodynamic stability, and <span class="hlt">electronic</span> properties of CaH 2 surfaces in (001),(110), and (111) crystallographic orientations are investigated using ab initio modeling. We show that stoichiometric surfaces terminated with a hydrogen atomic plane are the most energetically favorable and discuss properties of hydrogen vacancies (VH) at these surfaces. The average calculated work function of the most stable pristine surfaces (~5.2 eV) is in agree-ment with experimental data for powder samples. Neutral hydrogen vacancies host <span class="hlt">localized</span> <span class="hlt">electrons</span> and induce defect states in the band gap, thereby shifting the effective work function to much lower values of ~2.7 eV. Surface VH aremore » predicted to aggregate into dimers and form <span class="hlt">electron</span>-rich centers (e -)Ca 2+(e -) stable to over 800 K. These results suggest that hydrogen-deficient surfaces of CaH 2 can host a large concentration of <span class="hlt">localized</span> <span class="hlt">electrons</span> and, thus, give rise to new catalytic functionalities involving <span class="hlt">electron</span> transfer between the surface, catalysts supported on it, and reacting species.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=web+AND+server&pg=4&id=EJ673398','ERIC'); return false;" href="https://eric.ed.gov/?q=web+AND+server&pg=4&id=EJ673398"><span>Usage Data for <span class="hlt">Electronic</span> Resources: A Comparison between <span class="hlt">Locally</span> Collected and Vendor-Provided Statistics.</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>Duy, Joanna; Vaughan, Liwen</p> <p>2003-01-01</p> <p>Vendor-provided <span class="hlt">electronic</span> resource usage statistics are not currently standardized across vendors. This study investigates the feasibility of using <span class="hlt">locally</span> collected data to check the reliability of vendor-provided data. Vendor-provided data were compared with <span class="hlt">local</span> data collected from North Carolina State University (NCSU) Libraries' Web…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97c5143N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97c5143N"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> and magnetic properties of the half-metallic ferrimagnet Mn2VAl probed by soft x-ray spectroscopies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nagai, K.; Fujiwara, H.; Aratani, H.; Fujioka, S.; Yomosa, H.; Nakatani, Y.; Kiss, T.; Sekiyama, A.; Kuroda, F.; Fujii, H.; Oguchi, T.; Tanaka, A.; Miyawaki, J.; Harada, Y.; Takeda, Y.; Saitoh, Y.; Suga, S.; Umetsu, R. Y.</p> <p>2018-01-01</p> <p>We have studied the <span class="hlt">electronic</span> <span class="hlt">structure</span> of ferrimagnetic Mn2VAl single crystals by means of soft x-ray absorption spectroscopy (XAS), x-ray absorption magnetic circular dichroism (XMCD), and resonant soft x-ray inelastic scattering (RIXS). We have successfully observed the XMCD signals for all the constituent elements. The Mn L2 ,3 XAS and XMCD spectra are reproduced by spectral simulations based on density-functional theory, indicating the itinerant character of the Mn 3 d states. On the other hand, the V 3 d <span class="hlt">electrons</span> are rather <span class="hlt">localized</span> since the ionic model can qualitatively explain the V L2 ,3 XAS and XMCD spectra. This picture is consistent with <span class="hlt">local</span> d d excitations revealed by the V L3 RIXS.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013MPLB...2730004S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013MPLB...2730004S"><span><span class="hlt">Structural</span> Dynamics of <span class="hlt">Electronic</span> Systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Suhir, E.</p> <p>2013-03-01</p> <p>The published work on analytical ("mathematical") and computer-aided, primarily finite-element-analysis (FEA) based, predictive modeling of the dynamic response of <span class="hlt">electronic</span> systems to shocks and vibrations is reviewed. While understanding the physics of and the ability to predict the response of an <span class="hlt">electronic</span> <span class="hlt">structure</span> to dynamic loading has been always of significant importance in military, avionic, aeronautic, automotive and maritime <span class="hlt">electronics</span>, during the last decade this problem has become especially important also in commercial, and, particularly, in portable <span class="hlt">electronics</span> in connection with accelerated testing of various surface mount technology (SMT) systems on the board level. The emphasis of the review is on the nonlinear shock-excited vibrations of flexible printed circuit boards (PCBs) experiencing shock loading applied to their support contours during drop tests. At the end of the review we provide, as a suitable and useful illustration, the exact solution to a highly nonlinear problem of the dynamic response of a "flexible-and-heavy" PCB to an impact load applied to its support contour during drop testing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28991450','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28991450"><span>Nature-Inspired <span class="hlt">Structural</span> Materials for Flexible <span class="hlt">Electronic</span> Devices.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Yaqing; He, Ke; Chen, Geng; Leow, Wan Ru; Chen, Xiaodong</p> <p>2017-10-25</p> <p>Exciting advancements have been made in the field of flexible <span class="hlt">electronic</span> devices in the last two decades and will certainly lead to a revolution in peoples' lives in the future. However, because of the poor sustainability of the active materials in complex stress environments, new requirements have been adopted for the construction of flexible devices. Thus, hierarchical architectures in natural materials, which have developed various environment-adapted <span class="hlt">structures</span> and materials through natural selection, can serve as guides to solve the limitations of materials and engineering techniques. This review covers the smart designs of <span class="hlt">structural</span> materials inspired by natural materials and their utility in the construction of flexible devices. First, we summarize <span class="hlt">structural</span> materials that accommodate mechanical deformations, which is the fundamental requirement for flexible devices to work properly in complex environments. Second, we discuss the functionalities of flexible devices induced by nature-inspired <span class="hlt">structural</span> materials, including mechanical sensing, energy harvesting, physically interacting, and so on. Finally, we provide a perspective on newly developed <span class="hlt">structural</span> materials and their potential applications in future flexible devices, as well as frontier strategies for biomimetic functions. These analyses and summaries are valuable for a systematic understanding of <span class="hlt">structural</span> materials in <span class="hlt">electronic</span> devices and will serve as inspirations for smart designs in flexible <span class="hlt">electronics</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011APS..MAR.C1184C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011APS..MAR.C1184C"><span>Theoretical Study of tip apex <span class="hlt">electronic</span> <span class="hlt">structure</span> in Scanning Tunneling Microscope</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Choi, Heesung; Huang, Min; Randall, John; Cho, Kyeongjae</p> <p>2011-03-01</p> <p>Scanning Tunneling Microscope (STM) has been widely used to explore diverse surface properties with an atomic resolution, and STM tip has played a critical role in controlling surface <span class="hlt">structures</span>. However, detailed information of atomic and <span class="hlt">electronic</span> <span class="hlt">structure</span> of STM tip and the fundamental understanding of STM images are still incomplete. Therefore, it is important to develop a comprehensive understanding of the <span class="hlt">electronic</span> <span class="hlt">structure</span> of STM tip. We have studied the atomic and <span class="hlt">electronic</span> <span class="hlt">structures</span> of STM tip with various transition metals (TMs) by DFT method. The d-<span class="hlt">electrons</span> of TM tip apex atoms show different orbital states near the Fermi level. We will present comprehensive data of STM tips from our DFT calculation. Verified quantification of the tip <span class="hlt">electronic</span> <span class="hlt">structures</span> will lead to fundamental understanding of STM tip <span class="hlt">structure</span>-property relationship. This work is supported by the DARPA TBN Program and the Texas ETF. DARPA Tip Based Nanofabrication Program and the Emerging Technology Fund of the State of Texas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1953d0018S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1953d0018S"><span><span class="hlt">Structural</span> stability and <span class="hlt">electronic</span> <span class="hlt">structure</span> of transition metal compound: HfN</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sarwan, Madhu; Shukoor, V. Abdul; Singh, Sadhna</p> <p>2018-05-01</p> <p>The <span class="hlt">structural</span> stability of transition metal nitride (HfN) has been investigated using density functional theory (DFT) with the help of Quantum-espresso codes. Our calculations confirm that the hafnium nitride (HfN) is stable in zinc-blende (B3) and rock-salt (B1) type <span class="hlt">structure</span>. We have also reported the <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties of HfN compound. These <span class="hlt">structural</span> properties have been compared with experimental and theoretical data available on this compound.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005APS..MARL32006D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005APS..MARL32006D"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of scandium-doped MgB2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de La Peña, Omar; Agrestini, Stefano</p> <p>2005-03-01</p> <p>Recently has been reported the synthesis of a new superconducting alloy based on MgB2, where Mg is partially substituted with Sc. In order to analyze the effect of Sc doping on the <span class="hlt">structural</span> and superconducting properties of Mg1-xScxB2, we have performed a detailed study of the <span class="hlt">electronic</span> <span class="hlt">structure</span> for this new diboride. The calculations have been done using the first-principles LAPW method, within the supercell approach for modeling the doping. In this work we report results for the <span class="hlt">electronic</span> band <span class="hlt">structure</span>, Fermi surface, and density of states. The effect of the Sc-d orbitals on the <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties of Mg1-xScxB2 is analyzed. Increasing the Sc concentration (x) the σ-band is gradually filled, because Sc have one valence <span class="hlt">electron</span> more than Mg. Interestingly, the analysis of the band <span class="hlt">structure</span> shows that even for ScB2 the top of the σ-band remain above the Fermi level, nevertheless the σ-band presents high dispersion and has an important contribution of d states. In this way, in addition to the band filling effect, Sc doping gradually reduces the two-dimensional character of the σ- band in Mg1-xScxB2 as a result of increasing the sp(B)-d(Sc) hybridization. This research was partially supported by Consejo Nacional de Ciencia y Tecnolog'ia (CONACYT, M'exico) under Grant. No. 43830-F</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9976E..0TT','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9976E..0TT"><span>Remote sensing image segmentation using <span class="hlt">local</span> sparse <span class="hlt">structure</span> constrained latent low rank representation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tian, Shu; Zhang, Ye; Yan, Yimin; Su, Nan; Zhang, Junping</p> <p>2016-09-01</p> <p>Latent low-rank representation (LatLRR) has been attached considerable attention in the field of remote sensing image segmentation, due to its effectiveness in exploring the multiple subspace <span class="hlt">structures</span> of data. However, the increasingly heterogeneous texture information in the high spatial resolution remote sensing images, leads to more severe interference of pixels in <span class="hlt">local</span> neighborhood, and the LatLRR fails to capture the <span class="hlt">local</span> complex <span class="hlt">structure</span> information. Therefore, we present a <span class="hlt">local</span> sparse <span class="hlt">structure</span> constrainted latent low-rank representation (LSSLatLRR) segmentation method, which explicitly imposes the <span class="hlt">local</span> sparse <span class="hlt">structure</span> constraint on LatLRR to capture the intrinsic <span class="hlt">local</span> <span class="hlt">structure</span> in manifold <span class="hlt">structure</span> feature subspaces. The whole segmentation framework can be viewed as two stages in cascade. In the first stage, we use the <span class="hlt">local</span> histogram transform to extract the texture <span class="hlt">local</span> histogram features (LHOG) at each pixel, which can efficiently capture the complex and micro-texture pattern. In the second stage, a <span class="hlt">local</span> sparse <span class="hlt">structure</span> (LSS) formulation is established on LHOG, which aims to preserve the <span class="hlt">local</span> intrinsic <span class="hlt">structure</span> and enhance the relationship between pixels having similar <span class="hlt">local</span> characteristics. Meanwhile, by integrating the LSS and the LatLRR, we can efficiently capture the <span class="hlt">local</span> sparse and low-rank <span class="hlt">structure</span> in the mixture of feature subspace, and we adopt the subspace segmentation method to improve the segmentation accuracy. Experimental results on the remote sensing images with different spatial resolution show that, compared with three state-of-the-art image segmentation methods, the proposed method achieves more accurate segmentation results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22608746-theoretical-investigation-electronic-structure-substituted-nickel-phthalocyanine','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22608746-theoretical-investigation-electronic-structure-substituted-nickel-phthalocyanine"><span>Theoretical investigation of the <span class="hlt">electronic</span> <span class="hlt">structure</span> of a substituted nickel phthalocyanine</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>Kaur, Prabhjot, E-mail: prabhphysics@gmail.com; Sachdeva, Ritika; Singh, Sukhwinder</p> <p>2016-05-23</p> <p>The optimized geometry and <span class="hlt">electronic</span> <span class="hlt">structure</span> of an organic compound nickel phthalocyanine tetrasulfonic acid tetra sodium salt have been investigated using density functional theory. We have also optimized the <span class="hlt">structure</span> of nickel phthalocyanine tetrasulfonic acid tetra sodium salt in dimethyl sulfoxide to study effects of solvent on the <span class="hlt">electronic</span> <span class="hlt">structure</span> and transitions. Experimentally, the <span class="hlt">electronic</span> transitions have been studied using UV-VIS spectroscopic technique. It is observed that the <span class="hlt">electronic</span> transitions obtained from the theoretical studies generally agree with the experiment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1224780-structure-electronic-properties-cu-nanoclusters-supported-mo2c-moc-surfaces','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1224780-structure-electronic-properties-cu-nanoclusters-supported-mo2c-moc-surfaces"><span><span class="hlt">Structure</span> and <span class="hlt">electronic</span> properties of Cu nanoclusters supported on Mo 2C(001) and MoC(001) surfaces</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Posada-Pérez, Sergio; Viñes, Francesc; Rodríguez, José A.; ...</p> <p>2015-09-15</p> <p>In this study, the atomic <span class="hlt">structure</span> and <span class="hlt">electronic</span> properties of Cu n nanoclusters (n = 4, 6, 7, and 10) supported on cubic nonpolar δ-MoC(001) and orthorhombic C- or Mo-terminated polar β-Mo 2C(001) surfaces have been investigated by means of periodic density functional theory based calculations. The <span class="hlt">electronic</span> properties have been analyzed by means of the density of states, Bader charges, and <span class="hlt">electron</span> <span class="hlt">localization</span> function plots. The Cu nanoparticles supported on β-Mo 2C(001), either Mo- or C-terminated, tend to present a two-dimensional <span class="hlt">structure</span> whereas a three-dimensional geometry is preferred when supported on δ-MoC(001), indicating that the Mo:C ratio and themore » surface polarity play a key role determining the <span class="hlt">structure</span> of supported clusters. Nevertheless, calculations also reveal important differences between the C- and Mo-terminated β-Mo 2C(001) supports to the point that supported Cu particles exhibit different charge states, which opens a way to control the reactivity of these potential catalysts.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22608825-effect-hydrostatic-pressure-structural-electronic-properties-cd-sub-cr-sub','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22608825-effect-hydrostatic-pressure-structural-electronic-properties-cd-sub-cr-sub"><span>Effect of hydrostatic pressure on the <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties of Cd{sub 0.75}Cr{sub 0.25}S</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>Rani, Anita; Kaur, Kulwinder; Kumar, Ranjan</p> <p></p> <p>In this paper we present the results obtained from first principle calculations of the effect of hydrostatic pressure on the <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties of Cd{sub 1-x}Cr{sub x}S diluted magnetic semiconductor in Zinc Blende (B3) phase at x=0.25. High pressure behavior of Cd{sub 1-x}Cr{sub x}S has been investigated between 0 GPa to 100 GPa The calculations have been performed using Density functional theory as implemented in the Spanish Initiative for <span class="hlt">Electronic</span> Simulations with Thousands of Atoms code using <span class="hlt">local</span> density approximation as exchange-correlation (XC) potential. Calculated <span class="hlt">electronic</span> band <span class="hlt">structures</span> of Cd{sub 1-x}Cr{sub x}S are discussed in terms of contribution ofmore » Cr 3d{sup 5} 4s{sup 1}, Cd 4d{sup 10} 5s{sup 2}, S 3s{sup 2} 3p{sup 4} orbital’s. Study of band <span class="hlt">structures</span> shows half-metallic ferromagnetic nature of Cd{sub 0.75}Cr{sub 0.25}S with 100% spin polarization. Under application of external pressure, the valence band and conduction band are shifted upward which leads to modification of <span class="hlt">electronic</span> <span class="hlt">structure</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014NatCo...5E4976D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014NatCo...5E4976D"><span>High-resolution <span class="hlt">structure</span> of the Shigella type-III secretion needle by solid-state NMR and cryo-<span class="hlt">electron</span> microscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Demers, Jean-Philippe; Habenstein, Birgit; Loquet, Antoine; Kumar Vasa, Suresh; Giller, Karin; Becker, Stefan; Baker, David; Lange, Adam; Sgourakis, Nikolaos G.</p> <p>2014-09-01</p> <p>We introduce a general hybrid approach for determining the <span class="hlt">structures</span> of supramolecular assemblies. Cryo-<span class="hlt">electron</span> microscopy (cryo-EM) data define the overall envelope of the assembly and rigid-body orientation of the subunits while solid-state nuclear magnetic resonance (ssNMR) chemical shifts and distance constraints define the <span class="hlt">local</span> secondary <span class="hlt">structure</span>, protein fold and inter-subunit interactions. Finally, Rosetta <span class="hlt">structure</span> calculations provide a general framework to integrate the different sources of <span class="hlt">structural</span> information. Combining a 7.7-Å cryo-EM density map and 996 ssNMR distance constraints, the <span class="hlt">structure</span> of the type-III secretion system needle of Shigella flexneri is determined to a precision of 0.4 Å. The calculated <span class="hlt">structures</span> are cross-validated using an independent data set of 691 ssNMR constraints and scanning transmission <span class="hlt">electron</span> microscopy measurements. The hybrid model resolves the conformation of the non-conserved N terminus, which occupies a protrusion in the cryo-EM density, and reveals conserved pore residues forming a continuous pattern of electrostatic interactions, thereby suggesting a mechanism for effector protein translocation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=curvature&pg=6&id=EJ736772','ERIC'); return false;" href="https://eric.ed.gov/?q=curvature&pg=6&id=EJ736772"><span><span class="hlt">Local</span> Influence Analysis of Nonlinear <span class="hlt">Structural</span> Equation Models</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>Lee, Sik-Yum; Tang, Nian-Sheng</p> <p>2004-01-01</p> <p>By regarding the latent random vectors as hypothetical missing data and based on the conditional expectation of the complete-data log-likelihood function in the EM algorithm, we investigate assessment of <span class="hlt">local</span> influence of various perturbation schemes in a nonlinear <span class="hlt">structural</span> equation model. The basic building blocks of <span class="hlt">local</span> influence analysis…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22479720-atomic-electronic-structure-exfoliated-black-phosphorus','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22479720-atomic-electronic-structure-exfoliated-black-phosphorus"><span>Atomic and <span class="hlt">electronic</span> <span class="hlt">structure</span> of exfoliated black phosphorus</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, Ryan J.; Topsakal, Mehmet; Jeong, Jong Seok</p> <p>2015-11-15</p> <p>Black phosphorus, a layered two-dimensional crystal with tunable <span class="hlt">electronic</span> properties and high hole mobility, is quickly emerging as a promising candidate for future <span class="hlt">electronic</span> and photonic devices. Although theoretical studies using ab initio calculations have tried to predict its atomic and <span class="hlt">electronic</span> <span class="hlt">structure</span>, uncertainty in its fundamental properties due to a lack of clear experimental evidence continues to stymie our full understanding and application of this novel material. In this work, aberration-corrected scanning transmission <span class="hlt">electron</span> microscopy and ab initio calculations are used to study the crystal <span class="hlt">structure</span> of few-layer black phosphorus. Directly interpretable annular dark-field images provide a three-dimensional atomic-resolutionmore » view of this layered material in which its stacking order and all three lattice parameters can be unambiguously identified. In addition, <span class="hlt">electron</span> energy-loss spectroscopy (EELS) is used to measure the conduction band density of states of black phosphorus, which agrees well with the results of density functional theory calculations performed for the experimentally determined crystal. Furthermore, experimental EELS measurements of interband transitions and surface plasmon excitations are also consistent with simulated results. Finally, the effects of oxidation on both the atomic and <span class="hlt">electronic</span> <span class="hlt">structure</span> of black phosphorus are analyzed to explain observed device degradation. The transformation of black phosphorus into amorphous PO{sub 3} or H{sub 3}PO{sub 3} during oxidation may ultimately be responsible for the degradation of devices exposed to atmosphere over time.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18698892','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18698892"><span>Beyond electronegativity and <span class="hlt">local</span> hardness: Higher-order equalization criteria for determination of a ground-state <span class="hlt">electron</span> density.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ayers, Paul W; Parr, Robert G</p> <p>2008-08-07</p> <p>Higher-order global softnesses, <span class="hlt">local</span> softnesses, and softness kernels are defined along with their hardness inverses. The <span class="hlt">local</span> hardness equalization principle recently derived by the authors is extended to arbitrary order. The resulting hierarchy of equalization principles indicates that the electronegativity/chemical potential, <span class="hlt">local</span> hardness, and <span class="hlt">local</span> hyperhardnesses all are constant when evaluated for the ground-state <span class="hlt">electron</span> density. The new equalization principles can be used to test whether a trial <span class="hlt">electron</span> density is an accurate approximation to the true ground-state density and to discover molecules with desired reactive properties, as encapsulated by their chemical reactivity indicators.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EPJP..131..369E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EPJP..131..369E"><span>Theoretical and experimental investigations of optical, <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties of the lower-dimensional hybrid [NH3-(CH2)10-NH3]ZnCl4</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>El Mrabet, R.; Kassou, S.; Tahiri, O.; Belaaraj, A.; Guionneau, P.</p> <p>2016-10-01</p> <p>In the current study, a combination between theoretical and experimental studies has been made for the hybrid perovskite [NH3-(CH2)10-NH3]ZnCl4. The density functional theory (DFT) was performed to investigate <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties of the tilted compound. A <span class="hlt">local</span> approximation (LDA) and semi-<span class="hlt">local</span> approach (GGA) were employed. The results are obtained using, respectively, the <span class="hlt">local</span> exchange correlation functional of Perdew-Wang 92 (PW92) and semi <span class="hlt">local</span> functional of Perdew-Burke-Ernzerhof (PBE). The optimized cell parameters are in good agreement with the experimental results. <span class="hlt">Electronic</span> properties have been studied through the calculation of band <span class="hlt">structures</span> and density of state (DOS), while <span class="hlt">structural</span> properties are investigated by geometry optimization of the cell. Fritz-Haber-Institute (FHI) pseudopotentials were employed to perform all calculations. The optical diffuse reflectance spectra was mesured and applied to deduce the refractive index ( n), the extinction coefficient ( k), the absorption coefficient (α), the real and imaginary dielectric permittivity parts (ɛr,ɛi)) and the optical band gap energy Eg. The optical band gap energy value shows good consistent with that obtained from DFT calculations and reveals the insulating behavior of the material.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22852612','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22852612"><span><span class="hlt">Electronic</span> <span class="hlt">structures</span> of WAlO(y) and WAlO(y)(-) (y = 2-4) determined by anion photoelectron spectroscopy and density functional theory calculations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mann, Jennifer E; Waller, Sarah E; Jarrold, Caroline Chick</p> <p>2012-07-28</p> <p>The anion photoelectron spectra of WAlO(y)(-) (y = 2-4) are presented and assigned based on results of density functional theory calculations. The WAlO(2)(-) and WAlO(3)(-) spectra are both broad, with partially resolved vibrational <span class="hlt">structure</span>. In contrast, the WAlO(4)(-) spectrum features well-resolved vibrational <span class="hlt">structure</span> with contributions from three modes. There is reasonable agreement between experiment and theory for all oxides, and calculations are in particular validated by the near perfect agreement between the WAlO(4)(-) photoelectron spectrum and a Franck-Condon simulation based on computationally determined spectroscopic parameters. The <span class="hlt">structures</span> determined from this study suggest strong preferential W-O bond formation, and ionic bonding between Al(+) and WO(y)(-2) for all anions. Neutral species are similarly ionic, with WAlO(2) and WAlO(3) having <span class="hlt">electronic</span> <span class="hlt">structure</span> that suggests Al(+) ionically bound to WO(y)(-) and WAlO(4) being described as Al(+2) ionically bound to WO(4)(-2). The doubly-occupied 3sp hybrid orbital <span class="hlt">localized</span> on the Al center is energetically situated between the bonding O-<span class="hlt">local</span> molecular orbitals and the anti- or non-bonding W-<span class="hlt">local</span> molecular orbitals. The <span class="hlt">structures</span> determined in this study are very similar to <span class="hlt">structures</span> recently determined for the analogous MoAlO(y)(-)/MoAlO(y) cluster series, with subtle differences found in the <span class="hlt">electronic</span> <span class="hlt">structures</span> [S. E. Waller, J. E. Mann, E. Hossain, M. Troyer, and C. C. Jarrold, J. Chem. Phys. 137, 024302 (2012)].</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://adsabs.harvard.edu/abs/2017EPJB...90....5L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJB...90....5L"><span>Engineering the <span class="hlt">electronic</span> <span class="hlt">structure</span> of graphene superlattices via Fermi velocity modulation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lima, Jonas R. F.</p> <p>2017-01-01</p> <p>Graphene superlattices have attracted much research interest in the last years, since it is possible to manipulate the <span class="hlt">electronic</span> properties of graphene in these <span class="hlt">structures</span>. It has been verified that extra Dirac points appear in the <span class="hlt">electronic</span> <span class="hlt">structure</span> of the system. The <span class="hlt">electronic</span> <span class="hlt">structure</span> in the vicinity of these points has been studied for a gapless and gapped graphene superlattice and for a graphene superlattice with a spatially modulated energy gap. In each case a different behavior was obtained. In this work we show that via Fermi velocity engineering it is possible to tune the <span class="hlt">electronic</span> properties of a graphene superlattice to match all the previous cases studied. We also obtained new features of the system never observed before, reveling that the <span class="hlt">electronic</span> <span class="hlt">structure</span> of graphene is very sensitive to the modulation of the Fermi velocity. The results obtained here are relevant for the development of novel graphene-based <span class="hlt">electronic</span> devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JChPh.148k4102J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JChPh.148k4102J"><span>Variational nonadiabatic dynamics in the moving crude adiabatic representation: Further merging of nuclear dynamics and <span class="hlt">electronic</span> <span class="hlt">structure</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Joubert-Doriol, Loïc; Izmaylov, Artur F.</p> <p>2018-03-01</p> <p>A new methodology of simulating nonadiabatic dynamics using frozen-width Gaussian wavepackets within the moving crude adiabatic representation with the on-the-fly evaluation of <span class="hlt">electronic</span> <span class="hlt">structure</span> is presented. The main feature of the new approach is the elimination of any global or <span class="hlt">local</span> model representation of <span class="hlt">electronic</span> potential energy surfaces; instead, the <span class="hlt">electron</span>-nuclear interaction is treated explicitly using the Gaussian integration. As a result, the new scheme does not introduce any uncontrolled approximations. The employed variational principle ensures the energy conservation and leaves the number of <span class="hlt">electronic</span> and nuclear basis functions as the only parameter determining the accuracy. To assess performance of the approach, a model with two <span class="hlt">electronic</span> and two nuclear spacial degrees of freedom containing conical intersections between potential energy surfaces has been considered. Dynamical features associated with nonadiabatic transitions and nontrivial geometric (or Berry) phases were successfully reproduced within a limited basis expansion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22661410-structure-local-hot-bubble','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22661410-structure-local-hot-bubble"><span>THE <span class="hlt">STRUCTURE</span> OF THE <span class="hlt">LOCAL</span> HOT BUBBLE</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, W.; Galeazzi, M.; Uprety, Y.</p> <p></p> <p>Diffuse X-rays from the <span class="hlt">Local</span> Galaxy ( DXL ) is a sounding rocket mission designed to quantify and characterize the contribution of Solar Wind Charge eXchange (SWCX) to the Diffuse X-ray Background and study the properties of the <span class="hlt">Local</span> Hot Bubble (LHB). Based on the results from the DXL mission, we quantified and removed the contribution of SWCX to the diffuse X-ray background measured by the ROSAT All Sky Survey. The “cleaned” maps were used to investigate the physical properties of the LHB. Assuming thermal ionization equilibrium, we measured a highly uniform temperature distributed around kT  = 0.097 keV ± 0.013 keV (FWHM) ± 0.006more » keV (systematic). We also generated a thermal emission measure map and used it to characterize the three-dimensional (3D) <span class="hlt">structure</span> of the LHB, which we found to be in good agreement with the <span class="hlt">structure</span> of the <span class="hlt">local</span> cavity measured from dust and gas.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28520420','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28520420"><span><span class="hlt">Local</span> Descriptors of Dynamic and Nondynamic Correlation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ramos-Cordoba, Eloy; Matito, Eduard</p> <p>2017-06-13</p> <p>Quantitatively accurate <span class="hlt">electronic</span> <span class="hlt">structure</span> calculations rely on the proper description of <span class="hlt">electron</span> correlation. A judicious choice of the approximate quantum chemistry method depends upon the importance of dynamic and nondynamic correlation, which is usually assesed by scalar measures. Existing measures of <span class="hlt">electron</span> correlation do not consider separately the regions of the Cartesian space where dynamic or nondynamic correlation are most important. We introduce real-space descriptors of dynamic and nondynamic <span class="hlt">electron</span> correlation that admit orbital decomposition. Integration of the <span class="hlt">local</span> descriptors yields global numbers that can be used to quantify dynamic and nondynamic correlation. Illustrative examples over different chemical systems with varying <span class="hlt">electron</span> correlation regimes are used to demonstrate the capabilities of the <span class="hlt">local</span> descriptors. Since the expressions only require orbitals and occupation numbers, they can be readily applied in the context of <span class="hlt">local</span> correlation methods, hybrid methods, density matrix functional theory, and fractional-occupancy density functional theory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhSS...60..631L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhSS...60..631L"><span><span class="hlt">Electronic</span> <span class="hlt">Structure</span> of GdCuGe Intermetallic Compound</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lukoyanov, A. V.; Knyazev, Yu. V.; Kuz'min, Yu. I.</p> <p>2018-04-01</p> <p>The <span class="hlt">electronic</span> <span class="hlt">structure</span> of GdCuGe intermetallic compound has been studied. Spin-polarized energy spectrum calculations have been performed by the band method with allowance for strong <span class="hlt">electron</span> correlations in the 4 f-shell of gadolinium ions. Antiferromagnetic ordering of GdCuGe at low temperatures has been obtained in a theoretical calculation, with the value of the effective magnetic moment of gadolinium ions reproduced in fair agreement with experimental data. The <span class="hlt">electronic</span> density of states has been analyzed. An optical conductivity spectrum has been calculated for GdCuGe; it reveals specific features that are analogous to the ones discovered previously in the GdCuSi compound with a similar hexagonal <span class="hlt">structure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AcSpA.189..563T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AcSpA.189..563T"><span>Boron difluoride dibenzoylmethane derivatives: <span class="hlt">Electronic</span> <span class="hlt">structure</span> and luminescence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tikhonov, Sergey A.; Vovna, Vitaliy I.; Osmushko, Ivan S.; Fedorenko, Elena V.; Mirochnik, Anatoliy G.</p> <p>2018-01-01</p> <p><span class="hlt">Electronic</span> <span class="hlt">structure</span> and optical properties of boron difluoride dibenzoylmethanate and four of its derivatives have been studied by X-ray photoelectron spectroscopy, absorption and luminescence spectroscopy and quantum chemistry (DFT, TDDFT). The relative quantum luminescence yields have been revealed to correlate with charge transfers of HOMO-LUMO transitions, energy barriers of aromatic substituents rotation and the lifetime of excited states in the investigated complexes. The bathochromic shift of intensive bands in the optical spectra has been observed to occur when the functional groups are introduced into p-positions of phenyl cycles due to destabilizing HOMO levels. Calculated energy intervals between <span class="hlt">electronic</span> levels correlate well with XPS spectra <span class="hlt">structure</span> of valence and core <span class="hlt">electrons</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1328675','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1328675"><span>Automatic Tool for <span class="hlt">Local</span> Assembly <span class="hlt">Structures</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></p> <p></p> <p>Whole community shotgun sequencing of total DNA (i.e. metagenomics) and total RNA (i.e. metatranscriptomics) has provided a wealth of information in the microbial community <span class="hlt">structure</span>, predicted functions, metabolic networks, and is even able to reconstruct complete genomes directly. Here we present ATLAS (Automatic Tool for <span class="hlt">Local</span> Assembly <span class="hlt">Structures</span>) a comprehensive pipeline for assembly, annotation, genomic binning of metagenomic and metatranscriptomic data with an integrated framework for Multi-Omics. This will provide an open source tool for the Multi-Omic community at large.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4720112','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4720112"><span>Free <span class="hlt">electron</span> laser-driven ultrafast rearrangement of the <span class="hlt">electronic</span> <span class="hlt">structure</span> in Ti</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Principi, E.; Giangrisostomi, E.; Cucini, R.; Bencivenga, F.; Battistoni, A.; Gessini, A.; Mincigrucci, R.; Saito, M.; Di Fonzo, S.; D'Amico, F.; Di Cicco, A.; Gunnella, R.; Filipponi, A.; Giglia, A.; Nannarone, S.; Masciovecchio, C.</p> <p>2015-01-01</p> <p>High-energy density extreme ultraviolet radiation delivered by the FERMI seeded free-<span class="hlt">electron</span> laser has been used to create an exotic nonequilibrium state of matter in a titanium sample characterized by a highly excited <span class="hlt">electron</span> subsystem at temperatures in excess of 10 eV and a cold solid-density ion lattice. The obtained transient state has been investigated through ultrafast absorption spectroscopy across the Ti M2,3-edge revealing a drastic rearrangement of the sample <span class="hlt">electronic</span> <span class="hlt">structure</span> around the Fermi level occurring on a time scale of about 100 fs. PMID:26798835</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009PhRvB..79t5116H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009PhRvB..79t5116H"><span>Photoemission study of <span class="hlt">electronic</span> <span class="hlt">structure</span> of the half-metallic ferromagnet Co3Sn2S2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Holder, M.; Dedkov, Yu. S.; Kade, A.; Rosner, H.; Schnelle, W.; Leithe-Jasper, A.; Weihrich, R.; Molodtsov, S. L.</p> <p>2009-05-01</p> <p>Surface <span class="hlt">electronic</span> <span class="hlt">structure</span> of polycrystalline and single-crystalline samples of the half-metallic ferromagnet Co3Sn2S2 was studied by means of angle-resolved and core-level photoemissions. The experiments were performed in temperature regimes both above and below a Curie temperature of 176.9 K. The spectroscopic results are compared to <span class="hlt">local</span>-spin density approximation band-<span class="hlt">structure</span> calculations for the bulk samples. It is found that the surface sensitive experimental data are generally reproduced by the bulk computation suggesting that the theoretically predicted half-metallic properties of Co3Sn2S2 are retained at the surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1637562','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1637562"><span><span class="hlt">Structure</span> of <span class="hlt">electron</span> transfer flavoprotein-ubiquinone oxidoreductase and <span class="hlt">electron</span> transfer to the mitochondrial ubiquinone pool</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Zhang, Jian; Frerman, Frank E.; Kim, Jung-Ja P.</p> <p>2006-01-01</p> <p><span class="hlt">Electron</span> transfer flavoprotein-ubiquinone oxidoreductase (ETF-QO) is a 4Fe4S flavoprotein located in the inner mitochondrial membrane. It catalyzes ubiquinone (UQ) reduction by ETF, linking oxidation of fatty acids and some amino acids to the mitochondrial respiratory chain. Deficiencies in ETF or ETF-QO result in multiple acyl-CoA dehydrogenase deficiency, a human metabolic disease. Crystal <span class="hlt">structures</span> of ETF-QO with and without bound UQ were determined, and they are essentially identical. The molecule forms a single <span class="hlt">structural</span> domain. Three functional regions bind FAD, the 4Fe4S cluster, and UQ and are closely packed and share <span class="hlt">structural</span> elements, resulting in no discrete <span class="hlt">structural</span> domains. The UQ-binding pocket consists mainly of hydrophobic residues, and UQ binding differs from that of other UQ-binding proteins. ETF-QO is a monotopic integral membrane protein. The putative membrane-binding surface contains an α-helix and a β-hairpin, forming a hydrophobic plateau. The UQ—flavin distance (8.5 Å) is shorter than the UQ—cluster distance (18.8 Å), and the very similar redox potentials of FAD and the cluster strongly suggest that the flavin, not the cluster, transfers <span class="hlt">electrons</span> to UQ. Two possible <span class="hlt">electron</span> transfer paths can be envisioned. First, <span class="hlt">electrons</span> from the ETF flavin semiquinone may enter the ETF-QO flavin one by one, followed by rapid equilibration with the cluster. Alternatively, <span class="hlt">electrons</span> may enter via the cluster, followed by equilibration between centers. In both cases, when ETF-QO is reduced to a two-<span class="hlt">electron</span> reduced state (one <span class="hlt">electron</span> at each redox center), the enzyme is primed to reduce UQ to ubiquinol via FAD. PMID:17050691</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17050691','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17050691"><span><span class="hlt">Structure</span> of <span class="hlt">electron</span> transfer flavoprotein-ubiquinone oxidoreductase and <span class="hlt">electron</span> transfer to the mitochondrial ubiquinone pool.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Jian; Frerman, Frank E; Kim, Jung-Ja P</p> <p>2006-10-31</p> <p><span class="hlt">Electron</span> transfer flavoprotein-ubiquinone oxidoreductase (ETF-QO) is a 4Fe4S flavoprotein located in the inner mitochondrial membrane. It catalyzes ubiquinone (UQ) reduction by ETF, linking oxidation of fatty acids and some amino acids to the mitochondrial respiratory chain. Deficiencies in ETF or ETF-QO result in multiple acyl-CoA dehydrogenase deficiency, a human metabolic disease. Crystal <span class="hlt">structures</span> of ETF-QO with and without bound UQ were determined, and they are essentially identical. The molecule forms a single <span class="hlt">structural</span> domain. Three functional regions bind FAD, the 4Fe4S cluster, and UQ and are closely packed and share <span class="hlt">structural</span> elements, resulting in no discrete <span class="hlt">structural</span> domains. The UQ-binding pocket consists mainly of hydrophobic residues, and UQ binding differs from that of other UQ-binding proteins. ETF-QO is a monotopic integral membrane protein. The putative membrane-binding surface contains an alpha-helix and a beta-hairpin, forming a hydrophobic plateau. The UQ-flavin distance (8.5 A) is shorter than the UQ-cluster distance (18.8 A), and the very similar redox potentials of FAD and the cluster strongly suggest that the flavin, not the cluster, transfers <span class="hlt">electrons</span> to UQ. Two possible <span class="hlt">electron</span> transfer paths can be envisioned. First, <span class="hlt">electrons</span> from the ETF flavin semiquinone may enter the ETF-QO flavin one by one, followed by rapid equilibration with the cluster. Alternatively, <span class="hlt">electrons</span> may enter via the cluster, followed by equilibration between centers. In both cases, when ETF-QO is reduced to a two-<span class="hlt">electron</span> reduced state (one <span class="hlt">electron</span> at each redox center), the enzyme is primed to reduce UQ to ubiquinol via FAD.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1248914-effect-atomic-scale-defects-dopants-phosphorene-electronic-structure-quantum-transport-properties','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1248914-effect-atomic-scale-defects-dopants-phosphorene-electronic-structure-quantum-transport-properties"><span>Effect of atomic-scale defects and dopants on phosphorene <span class="hlt">electronic</span> <span class="hlt">structure</span> and quantum transport properties</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Lopez-Bezanilla, Alejandro</p> <p>2016-01-20</p> <p>By means of a multi-scale first-principles approach, a description of the <span class="hlt">local</span> <span class="hlt">electronic</span> <span class="hlt">structure</span> of 2D and narrow phosphorene sheets with various types of modifications is presented. Firtly, a rational argument based on the geometry of the pristine and modified P network, and supported by the Wannier functions formalism is introduced to describe a hybridization model of the P atomic orbitals. Ab initio calculations show that non-isoelectronic foreign atoms form quasi-bound states at varying energy levels and create different polarization states depending on the number of valence <span class="hlt">electrons</span> between P and the doping atom. The quantum transport properties of modifiedmore » phosphorene ribbons are further described with great accuracy. The distortions on the <span class="hlt">electronic</span> bands induced by the external species lead to strong backscattering effects on the propagating charge carriers. Depending on the energy of the charge carrier and the type of doping, the conduction may range from the diffusive to the <span class="hlt">localized</span> regime. Interstitial defects at vacant sites lead to homogeneous transport fingerprints across different types of doping atoms. We suggest that the relatively low values of charge mobility reported in experimental measurements may have its origin in the presence of defects.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhyB..536..816S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhyB..536..816S"><span><span class="hlt">Electronic</span> <span class="hlt">structures</span> and superconductivity in LuTE2Si2 phases (TE = d-<span class="hlt">electron</span> transition metal)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Samsel-Czekała, M.; Chajewski, G.; Wiśniewski, P.; Romanova, T.; Hackemer, A.; Gorzelniak, R.; Pikul, A. P.; Kaczorowski, D.</p> <p>2018-05-01</p> <p>In the course of our search for unconventional superconductors amidst the 1:2:2 phases, we have re-investigated the LuTE2Si2 compounds with TE = Fe, Co, Ni, Ru, Pd and Pt. In this paper, we present the results of our fully relativistic ab initio calculations of the band <span class="hlt">structures</span>, performed using the full-potential <span class="hlt">local</span>-orbital code. The theoretical data are supplemented by the results of low-temperature electrical transport and specific heat measurements performed down to 0.35 K. All the materials studied but LuPt2Si2 crystallize with the body-centered tetragonal ThCr2Si2-type <span class="hlt">structure</span> (space group I4/mmm). Their Fermi surfaces exhibit a three-dimensional multi-band character. In turn, the Pt-bearing compound adopts the primitive tetragonal CaBe2Ge2-type <span class="hlt">structure</span> (space group P4/nmm), and its Fermi surface consists of predominantly quasi-two-dimensional sheets. Bulk superconductivity was found only in LuPd2Si2 and LuPt2Si2 (independent of the <span class="hlt">structure</span> type and dimensionality of the Fermi surface). The key superconducting characteristics indicate a fully-gapped BCS type character. Though the <span class="hlt">electronic</span> <span class="hlt">structure</span> of LuFe2Si2 closely resembles that of the unconventional superconductor YFe2Ge2, this Lu-based silicide exhibits neither superconductivity nor spin fluctuations at least down to 0.35 K.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MPLB...3250107H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MPLB...3250107H"><span>The <span class="hlt">structural</span>, <span class="hlt">electronic</span> and optical properties of Au-ZnO interface <span class="hlt">structure</span> from the first-principles calculation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huo, Jin-Rong; Li, Lu; Cheng, Hai-Xia; Wang, Xiao-Xu; Zhang, Guo-Hua; Qian, Ping</p> <p>2018-03-01</p> <p>The interface <span class="hlt">structure</span>, <span class="hlt">electronic</span> and optical properties of Au-ZnO are studied using the first-principles calculation based on density functional theory (DFT). Given the interfacial distance, bonding configurations and terminated surface, we built the optimal interface <span class="hlt">structure</span> and calculated the <span class="hlt">electronic</span> and optical properties of the interface. The total density of states, partial <span class="hlt">electronic</span> density of states, electric charge density and atomic populations (Mulliken) are also displayed. The results show that the <span class="hlt">electrons</span> converge at O atoms at the interface, leading to a stronger binding of interfaces and thereby affecting the optical properties of interface <span class="hlt">structures</span>. In addition, we present the binding energies of different interface <span class="hlt">structures</span>. When the interface <span class="hlt">structure</span> of Au-ZnO gets changed, furthermore, varying optical properties are exhibited.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998PCM....25...83V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998PCM....25...83V"><span><span class="hlt">Electron</span>-beam induced amorphization of stishovite: Silicon-coordination change observed using Si K-edge extended <span class="hlt">electron</span> energy-loss fine <span class="hlt">structure</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van Aken, P. A.; Sharp, T. G.; Seifert, F.</p> <p></p> <p>The analysis of the extended energy-loss fine <span class="hlt">structure</span> (EXELFS) of the Si K-edge for sixfold-coordinated Si in synthetic stishovite and fourfold-coordinated Si in natural α-quartz is reported by using <span class="hlt">electron</span> energy-loss spectroscopy (EELS) in combination with transmission <span class="hlt">electron</span> microscopy (TEM). The stishovite Si K-edge EXELFS spectra were measured as a time-dependent series to document irradiation-induced amorphization. The amorphization was also investigated through the change in Si K- and O K-edge energy-loss near edge <span class="hlt">structure</span> (ELNES). For α-quartz, in contrast to stishovite, <span class="hlt">electron</span> irradiation-induced vitrification, verified by selected area <span class="hlt">electron</span> diffraction (SAED), produced no detectable changes of the EXELFS. The Si K-edge EXELFS were analysed with the classical extended X-ray absorption fine <span class="hlt">structure</span> (EXAFS) treatment and compared to ab initio curve-waved multiple-scattering (MS) calculations of EXAFS spectra for stishovite and α-quartz. Highly accurate information on the <span class="hlt">local</span> atomic environment of the silicon atoms during the irradiation-induced amorphization of stishovite is obtained from the EXELFS <span class="hlt">structure</span> parameters (Si-O bond distances, coordination numbers and Debye-Waller factors). The mean Si-O bond distance R and mean Si coordination number N changes from R=0.1775 nm and N=6 for stishovite through a disordered intermediate state (R 0.172 nm and N 5) to R 0.167 nm and N 4.5 for a nearly amorphous state similar to α-quartz (R=0.1609 nm and N=4). During the amorphization process, the Debye-Waller factor (DWF) passes through a maximum value of as it changes from for sixfold to for fourfold coordination of Si. This increase in Debye-Waller factor indicates an increase in mean-square relative displacement (MSRD) between the central silicon atom and its oxygen neighbours that is consistent with the presence of an intermediate <span class="hlt">structural</span> state with fivefold coordination of Si. The distribution of coordination states can be estimated by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..MAR.K7010H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..MAR.K7010H"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of PPP@ZnO from all-<span class="hlt">electron</span> quasiarticle calculations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Höffling, Benjamin; Nabok, Dimitri; Draxl, Claudia; Condensed Matter Theory Group, Humboldt University Berlin Team</p> <p></p> <p>We investigate the <span class="hlt">electronic</span> properties of poly(para-phenylene) (PPP) adsorbed on the non-polar (001) surface of rocksalt (rs) ZnO using all-<span class="hlt">electron</span> density functional theory (DFT) as well as quasiparticle (QP) calculations within the GW approach. A particular focus is put on the <span class="hlt">electronic</span> band discontinuities at the interface, where we investigate the impact of quantum confinement, molecular polarization, and charge rearrangement. For our prototypical system, PPP@ZnO, we find a type-I heterostructure. Comparison of the band offsets derived from a QP-treatment of the hybrid system with predictions based on mesoscopic methods, like the Shockley-Anderson model or alignment via the electrostatic potential, reveals the inadequacy of these simple approaches for the prediction of the <span class="hlt">electronic</span> <span class="hlt">structure</span> of such inorganic/organic heterosystems. Finally, we explore the optical excitations of the interface compared to the features of the pristine components and discuss the methodological implications for the ab-initio treatment of interface <span class="hlt">electronics</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1417747-all-electron-quasiparticle-self-consistent-gw-band-structures-srtio3-including-lattice-polarization-corrections-different-phases','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1417747-all-electron-quasiparticle-self-consistent-gw-band-structures-srtio3-including-lattice-polarization-corrections-different-phases"><span>All-<span class="hlt">electron</span> quasiparticle self-consistent GW band <span class="hlt">structures</span> for SrTiO 3 including lattice polarization corrections in different phases</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>Bhandari, Churna; van Schilfgaarde, Mark; Kotani, Takao</p> <p></p> <p>The <span class="hlt">electronic</span> band <span class="hlt">structure</span> of SrTiO3 is investigated in the all-<span class="hlt">electron</span> quasiparticle self-consistent GW (QSGW) approximation. Unlike previous pseudopotential-based QSGW or single-shot G0W0 calculations, the gap is found to be significantly overestimated compared to experiment. After putting in a correction for the underestimate of the screening by the random phase approximation in terms of a 0.8Σ approach, the gap is still overestimated. The 0.8Σ approach is discussed and justified in terms of various recent literature results including <span class="hlt">electron</span>-hole corrections. Adding a lattice polarization correction (LPC) in the q→0 limit for the screening of W, agreement with experiment is recovered. Themore » LPC is alternatively estimated using a polaron model. Here, we apply our approach to the cubic and tetragonal phases as well as a hypothetical layered postperovskite <span class="hlt">structure</span> and find that the <span class="hlt">local</span> density approximation (LDA) to GW gap correction is almost independent of <span class="hlt">structure</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1417747-all-electron-quasiparticle-self-consistent-gw-band-structures-srtio3-including-lattice-polarization-corrections-different-phases','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1417747-all-electron-quasiparticle-self-consistent-gw-band-structures-srtio3-including-lattice-polarization-corrections-different-phases"><span>All-<span class="hlt">electron</span> quasiparticle self-consistent GW band <span class="hlt">structures</span> for SrTiO 3 including lattice polarization corrections in different phases</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Bhandari, Churna; van Schilfgaarde, Mark; Kotani, Takao; ...</p> <p>2018-01-23</p> <p>The <span class="hlt">electronic</span> band <span class="hlt">structure</span> of SrTiO3 is investigated in the all-<span class="hlt">electron</span> quasiparticle self-consistent GW (QSGW) approximation. Unlike previous pseudopotential-based QSGW or single-shot G0W0 calculations, the gap is found to be significantly overestimated compared to experiment. After putting in a correction for the underestimate of the screening by the random phase approximation in terms of a 0.8Σ approach, the gap is still overestimated. The 0.8Σ approach is discussed and justified in terms of various recent literature results including <span class="hlt">electron</span>-hole corrections. Adding a lattice polarization correction (LPC) in the q→0 limit for the screening of W, agreement with experiment is recovered. Themore » LPC is alternatively estimated using a polaron model. Here, we apply our approach to the cubic and tetragonal phases as well as a hypothetical layered postperovskite <span class="hlt">structure</span> and find that the <span class="hlt">local</span> density approximation (LDA) to GW gap correction is almost independent of <span class="hlt">structure</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5040477','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5040477"><span>The <span class="hlt">local</span> spiral <span class="hlt">structure</span> of the Milky Way</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Xu, Ye; Reid, Mark; Dame, Thomas; Menten, Karl; Sakai, Nobuyuki; Li, Jingjing; Brunthaler, Andreas; Moscadelli, Luca; Zhang, Bo; Zheng, Xingwu</p> <p>2016-01-01</p> <p>The nature of the spiral <span class="hlt">structure</span> of the Milky Way has long been debated. Only in the last decade have astronomers been able to accurately measure distances to a substantial number of high-mass star-forming regions, the classic tracers of spiral <span class="hlt">structure</span> in galaxies. We report distance measurements at radio wavelengths using the Very Long Baseline Array for eight regions of massive star formation near the <span class="hlt">Local</span> spiral arm of the Milky Way. Combined with previous measurements, these observations reveal that the <span class="hlt">Local</span> Arm is larger than previously thought, and both its pitch angle and star formation rate are comparable to those of the Galaxy’s major spiral arms, such as Sagittarius and Perseus. Toward the constellation Cygnus, sources in the <span class="hlt">Local</span> Arm extend for a great distance along our line of sight and roughly along the solar orbit. Because of this orientation, these sources cluster both on the sky and in velocity to form the complex and long enigmatic Cygnus X region. We also identify a spur that branches between the <span class="hlt">Local</span> and Sagittarius spiral arms. PMID:27704048</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JaJAP..57cEA03A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JaJAP..57cEA03A"><span>Advanced understanding on <span class="hlt">electronic</span> <span class="hlt">structure</span> of molecular semiconductors and their interfaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Akaike, Kouki</p> <p>2018-03-01</p> <p>Understanding the <span class="hlt">electronic</span> <span class="hlt">structure</span> of organic semiconductors and their interfaces is critical to optimizing functionalities for <span class="hlt">electronics</span> applications, by rational chemical design and appropriate combination of device constituents. The unique <span class="hlt">electronic</span> <span class="hlt">structure</span> of a molecular solid is characterized as (i) anisotropic electrostatic fields that originate from molecular quadrupoles, (ii) interfacial energy-level lineup governed by simple electrostatics, and (iii) weak intermolecular interactions that make not only <span class="hlt">structural</span> order but also energy distributions of the frontier orbitals sensitive to atmosphere and interface growth. This article shows an overview on these features with reference to the improved understanding of the orientation-dependent <span class="hlt">electronic</span> <span class="hlt">structure</span>, comprehensive mechanisms of molecular doping, and energy-level alignment. Furthermore, the engineering of ionization energy by the control of the electrostatic fields and work function of practical electrodes by contact-induced doping is briefly described for the purpose of highlighting how the <span class="hlt">electronic</span> <span class="hlt">structure</span> impacts the performance of organic devices.</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('http://adsabs.harvard.edu/abs/2017ApPhL.111h4102K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhL.111h4102K"><span>The impact of adsorption on the <span class="hlt">localization</span> of spins in graphene oxide and reduced graphene oxide, observed with <span class="hlt">electron</span> paramagnetic resonance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kempiński, Mateusz; Florczak, Patryk; Jurga, Stefan; Śliwińska-Bartkowiak, Małgorzata; Kempiński, Wojciech</p> <p>2017-08-01</p> <p>We report the observations of <span class="hlt">electronic</span> properties of graphene oxide and reduced graphene oxide, performed with <span class="hlt">electron</span> paramagnetic resonance technique in a broad temperature range. Both materials were examined in pure form and saturated with air, helium, and heavy water molecules. We show that spin <span class="hlt">localization</span> strongly depends on the type and amount of molecules adsorbed at the graphene layer edges (and possible in-plane defects). Physical and chemical states of edges play crucial role in electrical transport within graphene-based materials, with hopping as the leading mechanism of charge carrier transport. Presented results are a good basis to understand the <span class="hlt">electronic</span> properties of other carbon <span class="hlt">structures</span> made of graphene-like building blocks. Most active carbons show some degree of functionalization and are known of having good adsorptive properties; thus, controlling both phenomena is important for many applications. Sample treatment with temperature, vacuum, and various adsorbents allowed for the observation of a possible metal-insulator transition and sorption pumping effects. The influence of adsorption on the <span class="hlt">localization</span> phenomena in graphene would be very important if to consider the graphene-based material as possible candidates for the future spintronics that works in ambient conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870046465&hterms=whole+vibration&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dwhole%2Bvibration','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870046465&hterms=whole+vibration&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dwhole%2Bvibration"><span>Effects of <span class="hlt">local</span> vibrations on the dynamics of space truss <span class="hlt">structures</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Warnaar, Dirk B.; Mcgowan, Paul E.</p> <p>1987-01-01</p> <p>The paper discusses the influence of <span class="hlt">local</span> member vibrations on the dynamics of repetitive space truss <span class="hlt">structures</span>. Several focus problems wherein <span class="hlt">local</span> member vibration modes are in the frequency range of the global truss modes are discussed. Special attention is given to defining methods that can be used to identify the global modes of a truss <span class="hlt">structure</span> amidst many <span class="hlt">local</span> modes. Significant interactions between the motions of <span class="hlt">local</span> member vibrations and the global behavior are shown to occur in truss <span class="hlt">structures</span> when: (1) the natural frequencies of the individual members for clamped-clamped boundary conditions are in the vicinity of the global truss frequency; and (2) the total mass of the individual members represents a large portion of the mass of the whole <span class="hlt">structure</span>. The analysis is carried out with a <span class="hlt">structural</span> analysis code which uses exact member theory. The modeling detail required using conventional finite element codes to adequately represent such a class of problems is examined. The paper concludes with some practical considerations for the design and dynamic testing of <span class="hlt">structures</span> which might exhibit such behavior.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3737575','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3737575"><span><span class="hlt">Localizing</span> Target <span class="hlt">Structures</span> in Ultrasound Video</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kwitt, R.; Vasconcelos, N.; Razzaque, S.; Aylward, S.</p> <p>2013-01-01</p> <p>The problem of <span class="hlt">localizing</span> specific anatomic <span class="hlt">structures</span> using ultrasound (US) video is considered. This involves automatically determining when an US probe is acquiring images of a previously defined object of interest, during the course of an US examination. <span class="hlt">Localization</span> using US is motivated by the increased availability of portable, low-cost US probes, which inspire applications where inexperienced personnel and even first-time users acquire US data that is then sent to experts for further assessment. This process is of particular interest for routine examinations in underserved populations as well as for patient triage after natural disasters and large-scale accidents, where experts may be in short supply. The proposed <span class="hlt">localization</span> approach is motivated by research in the area of dynamic texture analysis and leverages several recent advances in the field of activity recognition. For evaluation, we introduce an annotated and publicly available database of US video, acquired on three phantoms. Several experiments reveal the challenges of applying video analysis approaches to US images and demonstrate that good <span class="hlt">localization</span> performance is possible with the proposed solution. PMID:23746488</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4652865','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4652865"><span>Workshop on Measurement Needs for <span class="hlt">Local-Structure</span> Determination in Inorganic Materials</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Levin, Igor; Vanderah, Terrell</p> <p>2008-01-01</p> <p>The functional responses (e.g., dielectric, magnetic, catalytic, etc.) of many industrially-relevant materials are controlled by their <span class="hlt">local</span> structure—a term that refers to the atomic arrangements on a scale ranging from atomic (sub-nanometer) to several nanometers. Thus, accurate knowledge of <span class="hlt">local</span> <span class="hlt">structure</span> is central to understanding the properties of nanostructured materials, thereby placing the problem of determining atomic positions on the nanoscale—the so-called “nanostructure problem”—at the center of modern materials development. Today, multiple experimental techniques exist for probing <span class="hlt">local</span> atomic arrangements; nonetheless, finding accurate comprehensive, and robust <span class="hlt">structural</span> solutions for the nanostructured materials still remains a formidable challenge because any one of these methods yields only a partial view of the <span class="hlt">local</span> <span class="hlt">structure</span>. The primary goal of this 2-day NIST-sponsored workshop was to bring together experts in the key experimental and theoretical areas relevant to <span class="hlt">local-structure</span> determination to devise a strategy for the collaborative effort required to develop a comprehensive measurement solution on the <span class="hlt">local</span> scale. The participants unanimously agreed that solving the nanostructure problem—an ultimate frontier in materials characterization—necessitates a coordinated interdisciplinary effort that transcends the existing capabilities of any single institution, including national laboratories, centers, and user facilities. The discussions converged on an institute dedicated to <span class="hlt">local</span> <span class="hlt">structure</span> determination as the most viable organizational platform for successfully addressing the nanostructure problem. The proposed “institute” would provide an intellectual infrastructure for <span class="hlt">local</span> <span class="hlt">structure</span> determination by (1) developing and maintaining relevant computer software integrated in an open-source global optimization framework (Fig. 2), (2) connecting industrial and academic users with experts in measurement techniques, (3</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21546948-effect-nonthermal-electrons-propagation-characteristics-stability-two-dimensional-nonlinear-electrostatic-coherent-structures-relativistic-electron-positron-ion-plasmas','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21546948-effect-nonthermal-electrons-propagation-characteristics-stability-two-dimensional-nonlinear-electrostatic-coherent-structures-relativistic-electron-positron-ion-plasmas"><span>Effect of nonthermal <span class="hlt">electrons</span> on the propagation characteristics and stability of two-dimensional nonlinear electrostatic coherent <span class="hlt">structures</span> in relativistic <span class="hlt">electron</span> positron ion plasmas</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>Masood, W.; National Centre for Physics; Rizvi, H.</p> <p>2011-06-15</p> <p>Two-dimensional propagation of nonlinear ion acoustic shock and solitary waves in an unmagnetized plasma consisting of nonthermal <span class="hlt">electrons</span>, Boltzmannian positrons, and singly charged hot ions streaming with relativistic velocities are investigated. The system of fluid equations is reduced to Kadomtsev-Petviashvili-Burgers and Kadomtsev-Petviashvili (KP) equations in the limit of small amplitude perturbation. The dependence of the ion acoustic shock and solitary waves on various plasma parameters are explored in detail. Interestingly, it is observed that increasing the nonthermal <span class="hlt">electron</span> population increases the wave dispersion which enervates the strength of the ion acoustic shock wave; however, the same effect leads to anmore » enhancement of the soliton amplitude due to the absence of dissipation in the KP equation. The present investigation may be useful to understand the two-dimensional propagation characteristics of small but finite amplitude <span class="hlt">localized</span> shock and solitary <span class="hlt">structures</span> in planetary magnetospheres and auroral plasmas where nonthermal populations of <span class="hlt">electrons</span> have been observed by several satellite missions.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22494585-electronic-structures-magnetic-optical-properties-metal-phthalocyanine-complexes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22494585-electronic-structures-magnetic-optical-properties-metal-phthalocyanine-complexes"><span><span class="hlt">Electronic</span> <span class="hlt">structures</span> and magnetic/optical properties of metal phthalocyanine complexes</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>Baba, Shintaro; Suzuki, Atsushi, E-mail: suzuki@mat.usp.ac.jp; Oku, Takeo</p> <p>2016-02-01</p> <p><span class="hlt">Electronic</span> <span class="hlt">structures</span> and magnetic / optical properties of metal phthalocyanine complexes were studied by quantum calculations using density functional theory. Effects of central metal and expansion of π orbital on aromatic ring as conjugation system on the <span class="hlt">electronic</span> <span class="hlt">structures</span>, magnetic, optical properties and vibration modes of infrared and Raman spectra of metal phthalocyanines were investigated. <span class="hlt">Electron</span> and charge density distribution and energy levels near frontier orbital and excited states were influenced by the deformed <span class="hlt">structures</span> varied with central metal and charge. The magnetic parameters of chemical shifts in {sup 13}C-nuclear magnetic resonance ({sup 13}C-NMR), principle g-tensor, A-tensor, V-tensor of electricmore » field gradient and asymmetry parameters derived from the deformed <span class="hlt">structures</span> with magnetic interaction of nuclear quadruple interaction based on <span class="hlt">electron</span> and charge density distribution with a bias of charge near ligand under crystal field.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1214426-electron-localization-mixed-valence-diniobium-benzene-complex','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1214426-electron-localization-mixed-valence-diniobium-benzene-complex"><span><span class="hlt">Electron</span> <span class="hlt">localization</span> in a mixed-valence diniobium benzene complex</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Gianetti, Thomas L.; Nocton, Grégory; Minasian, Stefan G.; ...</p> <p>2014-11-11</p> <p>Reaction of the neutral diniobium benzene complex {[Nb(BDI)N tBu] 2(μ-C 6H 6)} (BDI = N,N'-diisopropylbenzene-β-diketiminate) with Ag[B(C 6F 5) 4] results in a single <span class="hlt">electron</span> oxidation to produce a cationic diniobium arene complex, {[Nb(BDI)N tBu] 2(μ-C 6H 6)}{B(C 6F 5) 4}. Investigation of the solid state and solution phase <span class="hlt">structure</span> using single-crystal X-ray diffraction, cyclic voltammetry, magnetic susceptibility, and multinuclear NMR spectroscopy indicates that the oxidation results in an asymmetric molecule with two chemically inequivalent Nb atoms. Further characterization using density functional theory (DFT) calculations, UV-visible, Nb L 3,2-edge X-ray absorption near-edge <span class="hlt">structure</span> (XANES), and EPR spectroscopies supports assignment ofmore » a diniobium complex, in which one Nb atom carries a single unpaired <span class="hlt">electron</span> that is not largely delocalized on the second Nb atom. During the oxidative transformation, one <span class="hlt">electron</span> is removed from the δ-bonding HOMO, which causes a destabilization of the molecule and formation of an asymmetric product. Subsequent reactivity studies indicate that the oxidized product allows access to metal-based chemistry with substrates that did not exhibit reactivity with the starting neutral complex.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24120524','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24120524"><span>Water channel <span class="hlt">structures</span> analysed by <span class="hlt">electron</span> crystallography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tani, Kazutoshi; Fujiyoshi, Yoshinori</p> <p>2014-05-01</p> <p>The mechanisms underlying water transport through aquaporin (AQP) have been debated for two decades. The water permeation phenomenon of AQP seems inexplicable because the Grotthuss mechanism does not allow for simultaneous fast water permeability and inhibition of proton transfer through the hydrogen bonds of water molecules. The AQP1 <span class="hlt">structure</span> determined by <span class="hlt">electron</span> crystallography provided the first insights into the proton exclusion mechanism despite fast water permeation. Although several studies have provided clues about the mechanism based on the AQP <span class="hlt">structure</span>, each proposed mechanism remains incomplete. The present review is focused on AQP function and <span class="hlt">structure</span> solved by <span class="hlt">electron</span> crystallography in an attempt to fill the gaps between the findings in the absence and presence of lipids. Many AQP <span class="hlt">structures</span> can be superimposed regardless of the determination method. The AQP fold is preserved even under conditions lacking lipids, but the water arrangement in the channel pore differs. The differences might be explained by dipole moments formed by the two short helices in the lipid bilayer. In addition, <span class="hlt">structure</span> analyses of double-layered two-dimensional crystals of AQP suggest an array formation and cell adhesive function. <span class="hlt">Electron</span> crystallography findings not only have contributed to resolve some of the water permeation mechanisms, but have also elucidated the multiple functions of AQPs in the membrane. The roles of AQPs in the brain remain obscure, but their multiple activities might be important in the regulation of brain and other biological functions. This article is part of a Special Issue entitled Aquaporins. © 2013.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26ES..131a2004R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26ES..131a2004R"><span>Detecting aroma changes of <span class="hlt">local</span> flavored green tea (Camellia sinensis) using <span class="hlt">electronic</span> nose</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ralisnawati, D.; Sukartiko, A. C.; Suryandono, A.; Triyana, K.</p> <p>2018-03-01</p> <p>Indonesia is currently the sixth largest tea producer in the world. However, consumption of the product in the country was considered low. Besides tea, the country also has various <span class="hlt">local</span> flavor ingredients that are potential to be developed. The addition of <span class="hlt">local</span> flavored ingredients such as ginger, lemon grass, and lime leaves on green tea products is gaining acceptance from consumers and producers. The aroma of <span class="hlt">local</span> flavored green tea was suspected to changes during storage, while its sensory testing has some limitations. Therefore, the study aimed to detect aroma changes of <span class="hlt">local</span> flavors added in green tea using <span class="hlt">electronic</span> nose (e-nose), an instrument developed to mimic the function of the human nose. The test was performed on a four-gram sample. The data was collected with 120 seconds of sensing time and 60 seconds of blowing time. Principal Component Analysis (PCA) was used to find out the aroma changes of <span class="hlt">local</span> flavored green tea during storage. We observed that <span class="hlt">electronic</span> nose could detect aroma changes of ginger flavored green tea from day 0 to day 6 with variance percentage 99.6%. Variance proportion of aroma changes of lemon grass flavored green tea from day 0 to day 6 was 99.3%. Variance proportion of aroma changes of lime leaves flavored green tea from day 0 to day 6 was 99.4%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JETP..123..864L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JETP..123..864L"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of nitrides PuN and UN</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lukoyanov, A. V.; Anisimov, V. I.</p> <p>2016-11-01</p> <p>The <span class="hlt">electronic</span> <span class="hlt">structure</span> of uranium and plutonium nitrides in ambient conditions and under pressure is investigated using the LDA + U + SO band method taking into account the spin-orbit coupling and the strong correlations of 5 f <span class="hlt">electrons</span> of actinoid ions. The parameters of these interactions for the equilibrium cubic <span class="hlt">structure</span> are calculated additionally. The application of pressure reduces the magnetic moment in PuN due to predominance of the f 6 configuration and the jj-type coupling. An increase in the occupancy of the 5 f state in UN leads to a decrease in the magnetic moment, which is also detected in the trigonal <span class="hlt">structure</span> of the UN x β phase (La2O3-type <span class="hlt">structure</span>). The theoretical results are in good agreement with the available experimental data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4867223','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4867223"><span><span class="hlt">Electronic</span> <span class="hlt">Structure</span> Contributions to Reactivity in Xanthine Oxidase Family Enzymes</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Stein, Benjamin W.; Kirk, Martin L.</p> <p>2016-01-01</p> <p>We review the xanthine oxidase (XO) family of pyranopterin molybdenum enzymes with a specific emphasis on <span class="hlt">electronic</span> <span class="hlt">structure</span> contributions to reactivity. In addition to xanthine and aldehyde oxidoreductases, which catalyze the 2-<span class="hlt">electron</span> oxidation of aromatic heterocycles and aldehyde substrates, this mini-review highlights recent work on the closely related carbon monoxide dehydrogenase (CODH) that catalyzes the oxidation of CO using a unique Mo-Cu heterobimetallic active site. A primary focus of this mini-review relates to how spectroscopy and computational methods have been used to develop an understanding of critical relationships between geometric <span class="hlt">structure</span>, <span class="hlt">electronic</span> <span class="hlt">structure</span>, and catalytic function. PMID:25425163</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25425163','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25425163"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> contributions to reactivity in xanthine oxidase family enzymes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Stein, Benjamin W; Kirk, Martin L</p> <p>2015-03-01</p> <p>We review the xanthine oxidase (XO) family of pyranopterin molybdenum enzymes with a specific emphasis on <span class="hlt">electronic</span> <span class="hlt">structure</span> contributions to reactivity. In addition to xanthine and aldehyde oxidoreductases, which catalyze the two-<span class="hlt">electron</span> oxidation of aromatic heterocycles and aldehyde substrates, this mini-review highlights recent work on the closely related carbon monoxide dehydrogenase (CODH) that catalyzes the oxidation of CO using a unique Mo-Cu heterobimetallic active site. A primary focus of this mini-review relates to how spectroscopy and computational methods have been used to develop an understanding of critical relationships between geometric <span class="hlt">structure</span>, <span class="hlt">electronic</span> <span class="hlt">structure</span>, and catalytic function.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26138268','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26138268"><span>Ultra-<span class="hlt">structural</span> hair alterations in Friedreich's ataxia: A scanning <span class="hlt">electron</span> microscopic investigation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Turkmenoglu, F Pinar; Kasirga, U Baran; Celik, H Hamdi</p> <p>2015-08-01</p> <p>Friedreich's ataxia (FRDA) is an autosomal recessive inherited disorder involving progressive damage to the central and peripheral nervous systems and cardiomyopathy. FRDA is caused by the silencing of the FXN gene and reduced levels of the encoded protein, frataxin. Frataxin is a mitochondrial protein that functions primarily in iron-sulfur cluster synthesis. Skin disorders including hair abnormalities have previously been reported in patients with mitochondrial disorders. However, to our knowledge, ultra-<span class="hlt">structural</span> hair alterations in FRDA were not demonstrated. The purpose of this study was to determine ultra-<span class="hlt">structural</span> alterations in the hairs of FRDA patients as well as carriers. Hair specimen from four patients, who are in different stages of the disease, and two carriers were examined by scanning <span class="hlt">electron</span> microscope. Thin and weak hair follicles with absence of homogeneities on the cuticular surface, <span class="hlt">local</span> damages of the cuticular layer, cuticular fractures were detected in both carriers and patients, but these alterations were much more prominent in the hair follicles of patients. In addition, erosions on the surface of the cuticle and <span class="hlt">local</span> deep cavities just under the cuticular level were observed only in patients. Indistinct cuticular pattern, pores on the cuticular surface, and presence of concavities on the hair follicle were also detected in patients in later stages of the disease. According to our results, progression of the disease increased the alterations on hair <span class="hlt">structure</span>. We suggest that ultra-<span class="hlt">structural</span> alterations observed in hair samples might be due to oxidative stress caused by deficient frataxin expression in mitochondria. © 2015 Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2396686','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2396686"><span>Paired β-sheet <span class="hlt">structure</span> of an Aβ(1-40) amyloid fibril revealed by <span class="hlt">electron</span> microscopy</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Sachse, Carsten; Fändrich, Marcus; Grigorieff, Nikolaus</p> <p>2008-01-01</p> <p>Alzheimer's disease is a neurodegenerative disorder that is characterized by the cerebral deposition of amyloid fibrils formed by Aβ peptide. Despite their prevalence in Alzheimer's and other neurodegenerative diseases, important details of the <span class="hlt">structure</span> of amyloid fibrils remain unknown. Here, we present a three-dimensional <span class="hlt">structure</span> of a mature amyloid fibril formed by Aβ(1-40) peptide, determined by <span class="hlt">electron</span> cryomicroscopy at ≈8-Å resolution. The fibril consists of two protofilaments, each containing ≈5-nm-long regions of β-sheet <span class="hlt">structure</span>. A <span class="hlt">local</span> twofold symmetry within each region suggests that pairs of β-sheets are formed from equivalent parts of two Aβ(1-40) peptides contained in each protofilament. The pairing occurs via tightly packed interfaces, reminiscent of recently reported steric zipper <span class="hlt">structures</span>. However, unlike these previous <span class="hlt">structures</span>, the β-sheet pairing is observed within an amyloid fibril and includes significantly longer amino acid sequences. PMID:18483195</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24401958','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24401958"><span>Excess <span class="hlt">electrons</span> in ice: a density functional theory study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bhattacharya, Somesh Kr; Inam, Fakharul; Scandolo, Sandro</p> <p>2014-02-21</p> <p>We present a density functional theory study of the <span class="hlt">localization</span> of excess <span class="hlt">electrons</span> in the bulk and on the surface of crystalline and amorphous water ice. We analyze the initial stages of <span class="hlt">electron</span> solvation in crystalline and amorphous ice. In the case of crystalline ice we find that excess <span class="hlt">electrons</span> favor surface states over bulk states, even when the latter are <span class="hlt">localized</span> at defect sites. In contrast, in amorphous ice excess <span class="hlt">electrons</span> find it equally favorable to <span class="hlt">localize</span> in bulk and in surface states which we attribute to the preexisting precursor states in the disordered <span class="hlt">structure</span>. In all cases excess <span class="hlt">electrons</span> are found to occupy the vacuum regions of the molecular network. The <span class="hlt">electron</span> <span class="hlt">localization</span> in the bulk of amorphous ice is assisted by its distorted hydrogen bonding network as opposed to the crystalline phase. Although qualitative, our results provide a simple interpretation of the large differences observed in the dynamics and <span class="hlt">localization</span> of excess <span class="hlt">electrons</span> in crystalline and amorphous ice films on metals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhDT.......143P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhDT.......143P"><span><span class="hlt">Structure</span> and <span class="hlt">Electronic</span> Properties of Crystalline and Amorphous Zinc Indium Tin Oxide 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>Proffit, Diana Elizabeth</p> <p></p> <p>The <span class="hlt">local</span> <span class="hlt">structures</span> and surface <span class="hlt">electronic</span> properties of crystalline (c-) and amorphous (a-) Zn and Sn codoped In2O3 (ZITO) films were studied. X-ray absorption spectroscopy (XAS) measurements confirm that Zn and Sn dopants occupy In sites in the bixbyite <span class="hlt">structure</span> of c-ZITO. Also, Zn dopants are generally under-coordinated and some compensated Sn dopants are over-coordinated, as demonstrated by the trend in coordination numbers (CN) of CNSn>CNIn>CNZn. Aliovalent Sn dopants form Frank-Kostlin clusters, (2Sn•InO'' i)x , which can act as donors when reduced. XAS and anomalous X-ray scattering studies on a-ZITO show that the <span class="hlt">local</span> <span class="hlt">structure</span> in a-ZITO is somewhat different than that in c-ZITO, particularly around Zn. The Zn-O bond length is significantly smaller than in c-ZITO and Zn is 4-fold coordinated. The smaller coordination numbers in a-ZITO follow the same trend as in c-ZITO. Unlike in c-ZITO, variations in the Sn/Zn ratio do not alter the electrical properties of a-ZITO, although variations in deposition oxygen pressure do. The 3-D geometrical arrangement linking <span class="hlt">local</span> <span class="hlt">structure</span> units seems to play a key role in charge balancing ZITO. As measured by in situ grazing incidence wide angle X-ray scattering, ZITO crystallizes at a higher temperature than In2 O3 and Sn-doped In2O3. The difference is attributed to a higher activation energy, which may result from the unique <span class="hlt">structure</span> around Zn in a-ZITO. Increasing the codoping level consistently increases crystallization temperature. For a given codoping level, the crystallization temperature during deposition is lower than that during post-deposition annealing. X-ray and ultraviolet photoelectron spectroscopy measurements show that a-ZITO and c-ZITO thin films have similar surface <span class="hlt">electronic</span> properties. In situ a-ZITO and c-ZITO films have low ionization potentials that are similar to In2O3. However, dry-air-annealed in situ films, ex situ films, and bulk ceramics have higher ionization potentials that are</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoRL..45.1237B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoRL..45.1237B"><span><span class="hlt">Localized</span> Oscillatory Energy Conversion in Magnetopause Reconnection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Burch, J. L.; Ergun, R. E.; Cassak, P. A.; Webster, J. M.; Torbert, R. B.; Giles, B. L.; Dorelli, J. C.; Rager, A. C.; Hwang, K.-J.; Phan, T. D.; Genestreti, K. J.; Allen, R. C.; Chen, L.-J.; Wang, S.; Gershman, D.; Le Contel, O.; Russell, C. T.; Strangeway, R. J.; Wilder, F. D.; Graham, D. B.; Hesse, M.; Drake, J. F.; Swisdak, M.; Price, L. M.; Shay, M. A.; Lindqvist, P.-A.; Pollock, C. J.; Denton, R. E.; Newman, D. L.</p> <p>2018-02-01</p> <p>Data from the NASA Magnetospheric Multiscale mission are used to investigate asymmetric magnetic reconnection at the dayside boundary between the Earth's magnetosphere and the solar wind. High-resolution measurements of plasmas and fields are used to identify highly <span class="hlt">localized</span> ( 15 <span class="hlt">electron</span> Debye lengths) standing wave <span class="hlt">structures</span> with large electric field amplitudes (up to 100 mV/m). These wave <span class="hlt">structures</span> are associated with spatially oscillatory energy conversion, which appears as alternatingly positive and negative values of J · E. For small guide magnetic fields the wave <span class="hlt">structures</span> occur in the <span class="hlt">electron</span> stagnation region at the magnetosphere edge of the <span class="hlt">electron</span> diffusion region. For larger guide fields the <span class="hlt">structures</span> also occur near the reconnection X-line. This difference is explained in terms of channels for the out-of-plane current (agyrotropic <span class="hlt">electrons</span> at the stagnation point and guide field-aligned <span class="hlt">electrons</span> at the X-line).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1416370-femtosecond-mega-electron-volt-electron-microdiffraction','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1416370-femtosecond-mega-electron-volt-electron-microdiffraction"><span>Femtosecond mega-<span class="hlt">electron</span>-volt <span class="hlt">electron</span> microdiffraction</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Shen, X.; Li, R. K.; Lundstrom, U.; ...</p> <p>2017-09-01</p> <p>To understand and control the basic functions of physical, chemical and biological processes from micron to nano-meter scale, an instrument capable of visualizing transient <span class="hlt">structural</span> changes of inhomogeneous materials with atomic spatial and temporal resolutions, is required. One such technique is femtosecond <span class="hlt">electron</span> microdiffraction, in which a short <span class="hlt">electron</span> pulse with femtosecond-scale duration is focused into a micron-scale spot and used to obtain diffraction images to resolve ultrafast <span class="hlt">structural</span> dynamics over a <span class="hlt">localized</span> crystalline domain. In this letter, we report the experimental demonstration of time-resolved mega-<span class="hlt">electron</span>-volt <span class="hlt">electron</span> microdiffraction which achieves a 5 μm root-mean-square (rms) beam size on the samplemore » and a 110 fs rms temporal resolution. Using pulses of 10k <span class="hlt">electrons</span> at 4.2 MeV energy with a normalized emittance 3 nm-rad, we obtained high quality diffraction from a single 10 μm paraffin ( C 44 H 90) crystal. The phonon softening mode in optical-pumped polycrystalline Bi was also time-resolved, demonstrating the temporal resolution limits of the instrument. In conclusion, this new characterization capability will open many research opportunities in material and biological sciences.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1416370-femtosecond-mega-electron-volt-electron-microdiffraction','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1416370-femtosecond-mega-electron-volt-electron-microdiffraction"><span>Femtosecond mega-<span class="hlt">electron</span>-volt <span class="hlt">electron</span> microdiffraction</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>Shen, X.; Li, R. K.; Lundstrom, U.</p> <p></p> <p>To understand and control the basic functions of physical, chemical and biological processes from micron to nano-meter scale, an instrument capable of visualizing transient <span class="hlt">structural</span> changes of inhomogeneous materials with atomic spatial and temporal resolutions, is required. One such technique is femtosecond <span class="hlt">electron</span> microdiffraction, in which a short <span class="hlt">electron</span> pulse with femtosecond-scale duration is focused into a micron-scale spot and used to obtain diffraction images to resolve ultrafast <span class="hlt">structural</span> dynamics over a <span class="hlt">localized</span> crystalline domain. In this letter, we report the experimental demonstration of time-resolved mega-<span class="hlt">electron</span>-volt <span class="hlt">electron</span> microdiffraction which achieves a 5 μm root-mean-square (rms) beam size on the samplemore » and a 110 fs rms temporal resolution. Using pulses of 10k <span class="hlt">electrons</span> at 4.2 MeV energy with a normalized emittance 3 nm-rad, we obtained high quality diffraction from a single 10 μm paraffin ( C 44 H 90) crystal. The phonon softening mode in optical-pumped polycrystalline Bi was also time-resolved, demonstrating the temporal resolution limits of the instrument. In conclusion, this new characterization capability will open many research opportunities in material and biological sciences.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22490851-geometric-electronic-structures-potassium-adsorbed-rubrene-complexes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22490851-geometric-electronic-structures-potassium-adsorbed-rubrene-complexes"><span>Geometric and <span class="hlt">electronic</span> <span class="hlt">structures</span> of potassium-adsorbed rubrene complexes</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, Tsung-Lung, E-mail: quantum@mail.ncyu.edu.tw; Lu, Wen-Cai, E-mail: wencailu@jlu.edu.cn; State Key Laboratory of Theoretical and Computational Chemistry, Institute of Theoretical Chemistry, Jilin University, Changchun, Jilin 130021</p> <p>2015-06-28</p> <p>The geometric and <span class="hlt">electronic</span> <span class="hlt">structures</span> of potassium-adsorbed rubrene complexes are studied in this article. It is found that the potassium-rubrene (K{sub 1}RUB) complexes inherit the main symmetry characteristics from their pristine counterparts and are thus classified into D{sub 2}- and C{sub 2h}-like complexes according to the relative orientations of the four phenyl side groups. The geometric <span class="hlt">structures</span> of K{sub 1}RUB are governed by two general effects on the total energy: Deformation of the carbon frame of the pristine rubrene increases the total energy, while proximity of the potassium ion to the phenyl ligands decreases the energy. Under these general rules,more » the <span class="hlt">structures</span> of D{sub 2}- and C{sub 2h}-like K{sub 1}RUB, however, exhibit their respective peculiarities. These peculiarities can be illustrated by their energy profiles of equilibrium <span class="hlt">structures</span>. For the potassium adsorption-sites, the D{sub 2}-like complexes show minimum-energy basins, whereas the C{sub 2h}-like ones have single-point minimum-energies. If the potassium atom ever has the energy to diffuse from the minimum-energy site, the potassium diffusion path on the D{sub 2}-like complexes is most likely along the backbone in contrast to the C{sub 2h}-like ones. Although the <span class="hlt">electronic</span> <span class="hlt">structures</span> of the minimum-energy <span class="hlt">structures</span> of D{sub 2}- and C{sub 2h}-like K{sub 1}RUB are very alike, decompositions of their total spectra reveal insights into the <span class="hlt">electronic</span> <span class="hlt">structures</span>. First, the spectral shapes are mainly determined by the facts that, in comparison with the backbone carbons, the phenyl carbons have more uniform chemical environments and far less contributions to the <span class="hlt">electronic</span> <span class="hlt">structures</span> around the valence-band edge. Second, the <span class="hlt">electron</span> dissociated from the potassium atom mainly remains on the backbone and has little effects on the <span class="hlt">electronic</span> <span class="hlt">structures</span> of the phenyl groups. Third, the two phenyls on the same side of the backbone as the potassium atom have more similar chemical</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('http://adsabs.harvard.edu/abs/2017PhRvB..96l5410T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvB..96l5410T"><span>Visualizing buried silicon atoms at the Cd-Si(111)-7 ×7 interface with <span class="hlt">localized</span> <span class="hlt">electrons</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tao, Min-Long; Xiao, Hua-Fang; Sun, Kai; Tu, Yu-Bing; Yuan, Hong-Kuan; Xiong, Zu-Hong; Wang, Jun-Zhong; Xue, Qi-Kun</p> <p>2017-09-01</p> <p>We report the atomic-scale imaging of the buried Cd-Si(111)-7 ×7 interface with a low temperature scanning tunneling microscopy (STM). The Cd(0001) films grown on Si(111)-7 ×7 reveal the <span class="hlt">electronic</span> growth mode, and manifest a series of quantum-well states. In the low-bias STM images, not only the 7 ×7 reconstruction but also individual Si adatoms buried by thick Cd islands are clearly visible. The two successive layers of Cd islands exhibit the distinct contrasts due to the quantum size effect. Moreover, we found a small gap appeared at Fermi level owing to the Anderson <span class="hlt">localization</span> induced by interface scattering. The perfect transparency of Cd films can be attributed to the anisotropic <span class="hlt">electron</span> motion, i.e., lateral <span class="hlt">electron</span> <span class="hlt">localization</span> and transverse motion like free-<span class="hlt">electron</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2108434','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2108434"><span>FINE <span class="hlt">STRUCTURAL</span> <span class="hlt">LOCALIZATION</span> OF ACYLTRANSFERASES</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Higgins, Joan A.; Barrnett, Russell J.</p> <p>1971-01-01</p> <p>A study of the fine <span class="hlt">structural</span> <span class="hlt">localization</span> of the acyltransferases of the monoglyceride and α-glycerophosphate pathways for triglyceride synthesis in the intestinal absorptive cell is reported. Glutaraldehyde-fixed tissue was found to synthesize diglyceride and triglyceride from monopalmitin and palmityl CoA, and parallel morphological studies showed the appearance of lipid droplets in the smooth endoplasmic reticulum of the absorptive cell. Glutaraldehyde-fixed tissue also synthesized triglyceride from α-glycerophosphate, although this enzyme system was more susceptible to fixation than the monoglyceride pathway acyltransferases. Cytochemical methods for the <span class="hlt">localization</span> of free CoA were based (a) on the formation of the insoluble lanthanium mercaptide of CoA and (b) on the reduction of ferricyanide by CoA to yield ferrocyanide which forms an insoluble precipitate with manganous ions. By these methods the monoglyceride pathway acyltransferases were found to be located mainly on the inner surface of the smooth endoplasmic reticulum. The α-glycerophosphate pathway acyltransferases were <span class="hlt">localized</span> mainly on the rough endoplasmic reticulum. Activity limited to the outer cisternae of the Golgi membranes occurred with both pathways. The possible organization of triglyceride absorption and chylomicron synthesis is discussed in view of these results. PMID:5563442</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1438776-chebyshev-polynomial-filtered-subspace-iteration-discontinuous-galerkin-method-large-scale-electronic-structure-calculations','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1438776-chebyshev-polynomial-filtered-subspace-iteration-discontinuous-galerkin-method-large-scale-electronic-structure-calculations"><span>Chebyshev polynomial filtered subspace iteration in the discontinuous Galerkin method for large-scale <span class="hlt">electronic</span> <span class="hlt">structure</span> calculations</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Banerjee, Amartya S.; Lin, Lin; Hu, Wei; ...</p> <p>2016-10-21</p> <p>The Discontinuous Galerkin (DG) <span class="hlt">electronic</span> <span class="hlt">structure</span> method employs an adaptive <span class="hlt">local</span> basis (ALB) set to solve the Kohn-Sham equations of density functional theory in a discontinuous Galerkin framework. The adaptive <span class="hlt">local</span> basis is generated on-the-fly to capture the <span class="hlt">local</span> material physics and can systematically attain chemical accuracy with only a few tens of degrees of freedom per atom. A central issue for large-scale calculations, however, is the computation of the <span class="hlt">electron</span> density (and subsequently, ground state properties) from the discretized Hamiltonian in an efficient and scalable manner. We show in this work how Chebyshev polynomial filtered subspace iteration (CheFSI) canmore » be used to address this issue and push the envelope in large-scale materials simulations in a discontinuous Galerkin framework. We describe how the subspace filtering steps can be performed in an efficient and scalable manner using a two-dimensional parallelization scheme, thanks to the orthogonality of the DG basis set and block-sparse <span class="hlt">structure</span> of the DG Hamiltonian matrix. The on-the-fly nature of the ALB functions requires additional care in carrying out the subspace iterations. We demonstrate the parallel scalability of the DG-CheFSI approach in calculations of large-scale twodimensional graphene sheets and bulk three-dimensional lithium-ion electrolyte systems. In conclusion, employing 55 296 computational cores, the time per self-consistent field iteration for a sample of the bulk 3D electrolyte containing 8586 atoms is 90 s, and the time for a graphene sheet containing 11 520 atoms is 75 s.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Sci...356..953S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Sci...356..953S"><span>Observation of Anderson <span class="hlt">localization</span> in disordered nanophotonic <span class="hlt">structures</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sheinfux, Hanan Herzig; Lumer, Yaakov; Ankonina, Guy; Genack, Azriel Z.; Bartal, Guy; Segev, Mordechai</p> <p>2017-06-01</p> <p>Anderson <span class="hlt">localization</span> is an interference effect crucial to the understanding of waves in disordered media. However, <span class="hlt">localization</span> is expected to become negligible when the features of the disordered <span class="hlt">structure</span> are much smaller than the wavelength. Here we experimentally demonstrate the <span class="hlt">localization</span> of light in a disordered dielectric multilayer with an average layer thickness of 15 nanometers, deep into the subwavelength regime. We observe strong disorder-induced reflections that show that the interplay of <span class="hlt">localization</span> and evanescence can lead to a substantial decrease in transmission, or the opposite feature of enhanced transmission. This deep-subwavelength Anderson <span class="hlt">localization</span> exhibits extreme sensitivity: Varying the thickness of a single layer by 2 nanometers changes the reflection appreciably. This sensitivity, approaching the atomic scale, holds the promise of extreme subwavelength sensing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012IJT....33.2339H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012IJT....33.2339H"><span>Full-Potential Calculation of <span class="hlt">Structural</span>, <span class="hlt">Electronic</span>, and Thermodynamic Properties of Fluoroperovskite { CsMF}3 (M = Be and Mg)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harmel, M.; Khachai, H.; Ameri, A.; Baki, N.; Haddou, A.; Khalfa, M.; Abbar, B.; Omran, S. Bin; Uğur, G.; Uğur, Ş.; Khenata, R.</p> <p>2012-12-01</p> <p>The <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties of the cubic fluoroperoveskite { CsBeF}3 and { CsMgF}3 have been investigated using the full-potential-linearized augmented plane wave method within the density functional theory. The exchange-correlation potential was treated with the <span class="hlt">local</span> density approximation and the generalized gradient approximation. The calculations of the <span class="hlt">electronic</span> band <span class="hlt">structures</span> show that { CsBeF}_{3 } has an indirect bandgap, whereas { CsMgF}3 has a direct bandgap. Through the quasi-harmonic Debye model, in which the phononic effects are considered, the effect of pressure P and temperature T on the lattice parameter, bulk modulus, thermal expansion coefficient, Debye temperature, and the heat capacity for { CsBeF}3 and { CsMgF}3 compounds are investigated for the first time.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008PhDT.......185B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008PhDT.......185B"><span><span class="hlt">Local</span> bonding <span class="hlt">structure</span> of tellurium and antimony in the phase change chalcogenides germanium-antimony-tellurium: A nuclear magnetic resonance study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bobela, David C.</p> <p></p> <p>Recent technological applications of some chalcogenide materials, compounds containing a group VI atom, have prompted studies of the <span class="hlt">local</span> atomic <span class="hlt">structure</span> of the amorphous phase. In the case of Ge2Sb2Te 5, metastability in the <span class="hlt">local</span> bonding <span class="hlt">structure</span> is responsible for its usefulness as a phase-change memory material. There is no consensus on the exact phase-change mechanism, which is partly due to the inadequacy of standard scattering techniques to probe the <span class="hlt">structure</span> of the amorphous phase. Nuclear magnetic resonance methods, on the other hand, are well suited to study <span class="hlt">local</span> <span class="hlt">structural</span> order even in the absence of a periodic lattice. In this technique, <span class="hlt">structural</span> information is encoded as an oscillating voltage caused by the nuclear spin. For the tellurium isotope, 125Te (spin = 1/2 in the ground state), the dominant interaction comes from the core and valence <span class="hlt">electrons</span> that carry angular momentum. This interaction is helpful in identifying Te sites of different <span class="hlt">local</span> coordination since the number of neighboring atoms should markedly change the <span class="hlt">local</span> <span class="hlt">electronic</span> <span class="hlt">structure</span>. The antimony isotope 125Sb has a spin = 5/2 in the ground state and possesses an asymmetric nuclear charge. This quadrupole moment will interact with an electric field gradient at the nuclear site, which is provided by an asymmetric <span class="hlt">electron</span> cloud surrounding the nucleus. The frequency-space spectra will reflect the strength of the interaction as well as the symmetry of the <span class="hlt">local</span> <span class="hlt">electronic</span> environment. This work investigates the nuclear magnetic resonance spectrum of 125Te and 125Sb in the crystalline and amorphous forms of several GexSbyTe 1-x-y compounds where 0 < (x, y) < 1. Results from the crystalline phase 125Te data show a trend in the spectral position that can be related to the tellurium bonded to three and six neighbors. In the amorphous phase, the same trend is observed, and the nuclear magnetic resonance fingerprint of two-fold and three-fold coordinated tellurium is obtained. It</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27884635','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27884635"><span>Understand protein functions by comparing the similarity of <span class="hlt">local</span> <span class="hlt">structural</span> environments.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Jiawen; Xie, Zhong-Ru; Wu, Yinghao</p> <p>2017-02-01</p> <p>The three-dimensional <span class="hlt">structures</span> of proteins play an essential role in regulating binding between proteins and their partners, offering a direct relationship between <span class="hlt">structures</span> and functions of proteins. It is widely accepted that the function of a protein can be determined if its <span class="hlt">structure</span> is similar to other proteins whose functions are known. However, it is also observed that proteins with similar global <span class="hlt">structures</span> do not necessarily correspond to the same function, while proteins with very different folds can share similar functions. This indicates that function similarity is originated from the <span class="hlt">local</span> <span class="hlt">structural</span> information of proteins instead of their global shapes. We assume that proteins with similar <span class="hlt">local</span> environments prefer binding to similar types of molecular targets. In order to testify this assumption, we designed a new <span class="hlt">structural</span> indicator to define the similarity of <span class="hlt">local</span> environment between residues in different proteins. This indicator was further used to calculate the probability that a given residue binds to a specific type of <span class="hlt">structural</span> neighbors, including DNA, RNA, small molecules and proteins. After applying the method to a large-scale non-redundant database of proteins, we show that the positive signal of binding probability calculated from the <span class="hlt">local</span> <span class="hlt">structural</span> indicator is statistically meaningful. In summary, our studies suggested that the <span class="hlt">local</span> environment of residues in a protein is a good indicator to recognize specific binding partners of the protein. The new method could be a potential addition to a suite of existing template-based approaches for protein function prediction. Copyright © 2016 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29266939','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29266939"><span>A <span class="hlt">Structural</span> Model of a P450-Ferredoxin Complex from Orientation-Selective Double <span class="hlt">Electron-Electron</span> Resonance Spectroscopy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bowen, Alice M; Johnson, Eachan O D; Mercuri, Francesco; Hoskins, Nicola J; Qiao, Ruihong; McCullagh, James S O; Lovett, Janet E; Bell, Stephen G; Zhou, Weihong; Timmel, Christiane R; Wong, Luet Lok; Harmer, Jeffrey R</p> <p>2018-02-21</p> <p>Cytochrome P450 (CYP) monooxygenases catalyze the oxidation of chemically inert carbon-hydrogen bonds in diverse endogenous and exogenous organic compounds by atmospheric oxygen. This C-H bond oxy-functionalization activity has huge potential in biotechnological applications. Class I CYPs receive the two <span class="hlt">electrons</span> required for oxygen activation from NAD(P)H via a ferredoxin reductase and ferredoxin. The interaction of Class I CYPs with their cognate ferredoxin is specific. In order to reconstitute the activity of diverse CYPs, <span class="hlt">structural</span> characterization of CYP-ferredoxin complexes is necessary, but little <span class="hlt">structural</span> information is available. Here we report a <span class="hlt">structural</span> model of such a complex (CYP199A2-HaPux) in frozen solution derived from distance and orientation restraints gathered by the EPR technique of orientation-selective double <span class="hlt">electron-electron</span> resonance (os-DEER). The long-lived oscillations in the os-DEER spectra were well modeled by a single orientation of the CYP199A2-HaPux complex. The <span class="hlt">structure</span> is different from the two known Class I CYP-Fdx <span class="hlt">structures</span>: CYP11A1-Adx and CYP101A1-Pdx. At the protein interface, HaPux residues in the [Fe 2 S 2 ] cluster-binding loop and the α3 helix and the C-terminus residue interact with CYP199A2 residues in the proximal loop and the C helix. These residue contacts are consistent with biochemical data on CYP199A2-ferredoxin binding and <span class="hlt">electron</span> transfer. <span class="hlt">Electron</span>-tunneling calculations indicate an efficient <span class="hlt">electron</span>-transfer pathway from the [Fe 2 S 2 ] cluster to the heme. This new <span class="hlt">structural</span> model of a CYP-Fdx complex provides the basis for tailoring CYP enzymes for which the cognate ferredoxin is not known, to accept <span class="hlt">electrons</span> from HaPux and display monooxygenase activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MAR.S8005L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MAR.S8005L"><span><span class="hlt">Electronic</span> <span class="hlt">Structure</span> Approach to Tunable <span class="hlt">Electronic</span> Properties of Hybrid Organic-Inorganic Perovskites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Garnett; Huhn, William; Mitzi, David B.; Kanai, Yosuke; Blum, Volker</p> <p></p> <p>We present a study of the <span class="hlt">electronic</span> <span class="hlt">structure</span> of layered hybrid organic-inorganic perovskite (HOIP) materials using all-<span class="hlt">electron</span> density-functional theory. Varying the nature of the organic and inorganic layers should enable systematically fine-tuning the carrier properties of each component. Using the HSE06 hybrid density functional including spin-orbit coupling (SOC), we validate the principle of tuning subsystem-specific parts of the <span class="hlt">electron</span> band <span class="hlt">structures</span> and densities of states in CH3NH3PbX3 (X=Cl, Br, I) compared to a modified organic component in layered (C6H5C2H4NH3) 2PbX4 (X=Cl, Br, I) and C20H22S4N2PbX4 (X=Cl, Br, I). We show that tunable shifts of <span class="hlt">electronic</span> levels indeed arise by varying Cl, Br, I as the inorganic components, and CH3NH3+ , C6H5C2H4NH3+ , C20H22S4N22 + as the organic components. SOC is found to play an important role in splitting the conduction bands of the HOIP compounds investigated here. The frontier orbitals of the halide shift, increasing the gap, when Cl is substituted for Br and I.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JMMM..456..257K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JMMM..456..257K"><span><span class="hlt">Electron</span> drag in ferromagnetic <span class="hlt">structures</span> separated by an insulating interface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kozub, V. I.; Muradov, M. I.; Galperin, Y. M.</p> <p>2018-06-01</p> <p>We consider <span class="hlt">electron</span> drag in a system of two ferromagnetic layers separated by an insulating interface. The source of it is expected to be magnon-<span class="hlt">electron</span> interactions. Namely, we assume that the external voltage is applied to the "active" layer stimulating electric current through this layer. In its turn, the scattering of the current-carrying <span class="hlt">electrons</span> by magnons leads to a magnon drag current within this layer. The 3-magnons interactions between magnons in the two layers (being of non-<span class="hlt">local</span> nature) lead to magnon drag within the "passive" layer which, correspondingly, produce <span class="hlt">electron</span> drag current via processes of magnon-<span class="hlt">electron</span> scattering. We estimate the drag current and compare it to the phonon-induced one.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29257877','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29257877"><span>Growth Behavior and <span class="hlt">Electronic</span> <span class="hlt">Structure</span> of Noble Metal-Doped Germanium Clusters.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mahtout, Sofiane; Siouani, Chaouki; Rabilloud, Franck</p> <p>2018-01-18</p> <p><span class="hlt">Structures</span>, energetics, and <span class="hlt">electronic</span> properties of noble metal-doped germanium (MGe n with M = Cu, Ag, Au; n = 1-19) clusters are systematically investigated by using the density functional theory (DFT) approach. The endohedral <span class="hlt">structures</span> in which the metal atom is encapsulated inside of a germanium cage appear at n = 10 when the dopant is Cu and n = 12 for M = Ag and Au. While Cu doping enhances the stability of the corresponding germanium frame, the binding energies of AgGe n and AuGe n are always lower than those of pure germanium clusters. Our results highlight the great stability of the CuGe 10 cluster in a D 4d <span class="hlt">structure</span> and, to a lesser extent, that of AgGe 15 and AuGe 15 , which exhibits a hollow cage-like geometry. The sphere-type geometries obtained for n = 10-15 present a peculiar <span class="hlt">electronic</span> <span class="hlt">structure</span> in which the valence <span class="hlt">electrons</span> of the noble metal and Ge atoms are delocalized and exhibit a shell <span class="hlt">structure</span> associated with the quasi-spherical geometry. It is found that the coinage metal is able to give both s- and d-type <span class="hlt">electrons</span> to be reorganized together with the valence <span class="hlt">electrons</span> of Ge atoms through a pooling of <span class="hlt">electrons</span>. The cluster size dependence of the stability, the frontier orbital energy gap, the vertical ionization potentials, and <span class="hlt">electron</span> affinities are given.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29227682','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29227682"><span>Self-Attractive Hartree Decomposition: Partitioning <span class="hlt">Electron</span> Density into Smooth <span class="hlt">Localized</span> Fragments.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhu, Tianyu; de Silva, Piotr; Van Voorhis, Troy</p> <p>2018-01-09</p> <p>Chemical bonding plays a central role in the description and understanding of chemistry. Many methods have been proposed to extract information about bonding from quantum chemical calculations, the majority of them resorting to molecular orbitals as basic descriptors. Here, we present a method called self-attractive Hartree (SAH) decomposition to unravel pairs of <span class="hlt">electrons</span> directly from the <span class="hlt">electron</span> density, which unlike molecular orbitals is a well-defined observable that can be accessed experimentally. The key idea is to partition the density into a sum of one-<span class="hlt">electron</span> fragments that simultaneously maximize the self-repulsion and maintain regular shapes. This leads to a set of rather unusual equations in which every <span class="hlt">electron</span> experiences self-attractive Hartree potential in addition to an external potential common for all the <span class="hlt">electrons</span>. The resulting symmetry breaking and <span class="hlt">localization</span> are surprisingly consistent with chemical intuition. SAH decomposition is also shown to be effective in visualization of single/multiple bonds, lone pairs, and unusual bonds due to the smooth nature of fragment densities. Furthermore, we demonstrate that it can be used to identify specific chemical bonds in molecular complexes and provides a simple and accurate electrostatic model of hydrogen bonding.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25207936','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25207936"><span>Writing silica <span class="hlt">structures</span> in liquid with scanning transmission <span class="hlt">electron</span> microscopy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>van de Put, Marcel W P; Carcouët, Camille C M C; Bomans, Paul H H; Friedrich, Heiner; de Jonge, Niels; Sommerdijk, Nico A J M</p> <p>2015-02-04</p> <p>Silica nanoparticles are imaged in solution with scanning transmission <span class="hlt">electron</span> microscopy (STEM) using a liquid cell with silicon nitride (SiN) membrane windows. The STEM images reveal that silica <span class="hlt">structures</span> are deposited in well-defined patches on the upper SiN membranes upon <span class="hlt">electron</span> beam irradiation. The thickness of the deposits is linear with the applied <span class="hlt">electron</span> dose. Scanning <span class="hlt">electron</span> microscopy (SEM) and atomic force microscopy (AFM) demonstrate that the deposited patches are a result of the merging of the original 20 nm-diameter nanoparticles, and that the related surface roughness depends on the <span class="hlt">electron</span> dose rate used. Using this approach, sub-micrometer scale <span class="hlt">structures</span> are written on the SiN in liquid by controlling the <span class="hlt">electron</span> exposure as function of the lateral position. © 2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900001140','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900001140"><span>Global/<span class="hlt">local</span> stress analysis of composite <span class="hlt">structures</span>. M.S. Thesis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ransom, Jonathan B.</p> <p>1989-01-01</p> <p>A method for performing a global/<span class="hlt">local</span> stress analysis is described and its capabilities are demonstrated. The method employs spline interpolation functions which satisfy the linear plate bending equation to determine displacements and rotations from a global model which are used as boundary conditions for the <span class="hlt">local</span> model. Then, the <span class="hlt">local</span> model is analyzed independent of the global model of the <span class="hlt">structure</span>. This approach can be used to determine <span class="hlt">local</span>, detailed stress states for specific <span class="hlt">structural</span> regions using independent, refined <span class="hlt">local</span> models which exploit information from less-refined global models. The method presented is not restricted to having a priori knowledge of the location of the regions requiring <span class="hlt">local</span> detailed stress analysis. This approach also reduces the computational effort necessary to obtain the detailed stress state. Criteria for applying the method are developed. The effectiveness of the method is demonstrated using a classical stress concentration problem and a graphite-epoxy blade-stiffened panel with a discontinuous stiffener.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140000894','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140000894"><span>Kinetic Model of Electric Potentials in <span class="hlt">Localized</span> Collisionless Plasma <span class="hlt">Structures</span> under Steady Quasi-gyrotropic Conditions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schindler, K.; Birn, J.; Hesse, M.</p> <p>2012-01-01</p> <p><span class="hlt">Localized</span> plasma <span class="hlt">structures</span>, such as thin current sheets, generally are associated with <span class="hlt">localized</span> magnetic and electric fields. In space plasmas <span class="hlt">localized</span> electric fields not only play an important role for particle dynamics and acceleration but may also have significant consequences on larger scales, e.g., through magnetic reconnection. Also, it has been suggested that <span class="hlt">localized</span> electric fields generated in the magnetosphere are directly connected with quasi-steady auroral arcs. In this context, we present a two-dimensional model based on Vlasov theory that provides the electric potential for a large class of given magnetic field profiles. The model uses an expansion for small deviation from gyrotropy and besides quasineutrality it assumes that <span class="hlt">electrons</span> and ions have the same number of particles with their generalized gyrocenter on any given magnetic field line. Specializing to one dimension, a detailed discussion concentrates on the electric potential shapes (such as "U" or "S" shapes) associated with magnetic dips, bumps, and steps. Then, it is investigated how the model responds to quasi-steady evolution of the plasma. Finally, the model proves useful in the interpretation of the electric potentials taken from two existing particle simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=molecular+AND+electronics&pg=5&id=EJ774966','ERIC'); return false;" href="https://eric.ed.gov/?q=molecular+AND+electronics&pg=5&id=EJ774966"><span>Computational Chemistry Using Modern <span class="hlt">Electronic</span> <span class="hlt">Structure</span> Methods</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>Bell, Stephen; Dines, Trevor J.; Chowdhry, Babur Z.; Withnall, Robert</p> <p>2007-01-01</p> <p>Various modern <span class="hlt">electronic</span> <span class="hlt">structure</span> methods are now days used to teach computational chemistry to undergraduate students. Such quantum calculations can now be easily used even for large size molecules.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MolPh.116..449D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MolPh.116..449D"><span><span class="hlt">Electronic</span> <span class="hlt">structures</span> of Al-Si clusters and the magic number <span class="hlt">structure</span> Al8Si4</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Du, Ning; Su, Mingzhi; Chen, Hongshan</p> <p>2018-02-01</p> <p>The low-energy <span class="hlt">structures</span> of Al8Sim (m = 1-6) have been determined by using the genetic algorithm combined with density functional theory and the Second-order Moller-Plesset perturbation theory (MP2) models. The results show that the close-packed <span class="hlt">structures</span> are preferable in energy for Al-Si clusters and in most cases there exist a few isomers with close energies. The valence molecular orbitals, the orbital level <span class="hlt">structures</span> and the <span class="hlt">electron</span> localisation function (ELF) consistently demonstrate that the <span class="hlt">electronic</span> <span class="hlt">structures</span> of Al-Si clusters can be described by the jellium model. Al8Si4 corresponds to a magic number <span class="hlt">structure</span> with pronounced stability and large energy gap; the 40 valence <span class="hlt">electrons</span> form closed 1S21P61D102S21F142P6 shells. The ELF attractors also suggest weak covalent Si-Si, Si-Al and Al-Al bonding, and doping Si in aluminium clusters promotes the covalent interaction between Al atoms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhyE...93..265L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhyE...93..265L"><span>The <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties of metal atoms adsorbed on graphene</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Wenjiang; Zhang, Cheng; Deng, Mingsen; Cai, Shaohong</p> <p>2017-09-01</p> <p>Based on density functional theory (DFT), we studied the <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties of seven different metal atoms adsorbed on graphene (M + graphene). The geometries, adsorption energies, density of states (DOS), band <span class="hlt">structures</span>, <span class="hlt">electronic</span> dipole moment, magnetic moment and work function (WF) of M + graphene were calculated. The adsorption energies ΔE indicated that Li, Na, K, Ca and Fe adsorbed on graphene were tending to form stable <span class="hlt">structures</span>. However, diffusion would occur on Cu and Ag adsorbed on graphene. In addition, the <span class="hlt">electronic</span> <span class="hlt">structure</span> near the Fermi level of graphene was significantly affected by Fe (Cu and Ag), compared with Li (Na, K and Ca). The <span class="hlt">electronic</span> dipole moment and magnetic moment of M + graphene were sensitive to the adsorbed metal atoms. Moreover, we found electropositive (electronegative) adsorption can decrease (increase) the WF of the surface. Specially, the WF of Ag + graphene and Fe + graphene would increase because surface dipole moment make a contribution to <span class="hlt">electron</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12719593','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12719593"><span>The vaccinia virus I3L gene product is <span class="hlt">localized</span> to a complex endoplasmic reticulum-associated <span class="hlt">structure</span> that contains the viral parental DNA.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Welsch, Sonja; Doglio, Laura; Schleich, Sibylle; Krijnse Locker, Jacomine</p> <p>2003-05-01</p> <p>The vaccinia virus (VV) I3L gene product is a single-stranded DNA-binding protein made early in infection that <span class="hlt">localizes</span> to the cytoplasmic sites of viral DNA replication (S. C. Rochester and P. Traktman, J. Virol. 72:2917-2926, 1998). Surprisingly, when replication was blocked, the protein <span class="hlt">localized</span> to distinct cytoplasmic spots (A. Domi and G. Beaud, J. Gen. Virol. 81:1231-1235, 2000). Here these I3L-positive spots were characterized in more detail. By using an anti-I3L peptide antibody we confirmed that the protein <span class="hlt">localized</span> to the cytoplasmic sites of viral DNA replication by both immunofluorescence and <span class="hlt">electron</span> microscopy (EM). Before replication had started or when replication was inhibited with hydroxyurea or cytosine arabinoside, I3L <span class="hlt">localized</span> to distinct cytoplasmic punctate <span class="hlt">structures</span> of homogeneous size. We show that these <span class="hlt">structures</span> are not incoming cores or cytoplasmic sites of VV early mRNA accumulation. Instead, morphological and quantitative data indicate that they are specialized sites where the parental DNA accumulates after its release from incoming viral cores. By EM, these sites appeared as complex, <span class="hlt">electron</span>-dense <span class="hlt">structures</span> that were intimately associated with the cellular endoplasmic reticulum (ER). By double labeling of cryosections we show that they contain DNA and a viral early protein, the gene product of E8R. Since E8R is a membrane protein that is able to bind to DNA, the <span class="hlt">localization</span> of this protein to the I3L puncta suggests that they are composed of membranes. The results are discussed in relation to our previous data showing that the process of viral DNA replication also occurs in close association with the ER.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16867310','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16867310"><span>Site-specific <span class="hlt">electronic</span> <span class="hlt">structure</span> analysis by channeling EELS and first-principles calculations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tatsumi, Kazuyoshi; Muto, Shunsuke; Yamamoto, Yu; Ikeno, Hirokazu; Yoshioka, Satoru; Tanaka, Isao</p> <p>2006-01-01</p> <p>Site-specific <span class="hlt">electronic</span> <span class="hlt">structures</span> were investigated by <span class="hlt">electron</span> energy loss spectroscopy (EELS) under <span class="hlt">electron</span> channeling conditions. The Al-K and Mn-L(2,3) <span class="hlt">electron</span> energy loss near-edge <span class="hlt">structure</span> (ELNES) of, respectively, NiAl2O4 and Mn3O4 were measured. Deconvolution of the raw spectra with the instrumental resolution function restored the blunt and hidden fine features, which allowed us to interpret the experimental spectral features by comparing with theoretical spectra obtained by first-principles calculations. The present method successfully revealed the <span class="hlt">electronic</span> <span class="hlt">structures</span> specific to the differently coordinated cationic sites.</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://ntrs.nasa.gov/search.jsp?R=20020022517&hterms=balance+sheet&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dbalance%2Bsheet','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020022517&hterms=balance+sheet&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dbalance%2Bsheet"><span><span class="hlt">Electron</span> Heat Flux in Pressure Balance <span class="hlt">Structures</span> at Ulysses</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yamauchi, Yohei; Suess, Steven T.; Sakurai, Takashi; Whitaker, Ann F. (Technical Monitor)</p> <p>2001-01-01</p> <p>Pressure balance <span class="hlt">structures</span> (PBSs) are a common feature in the high-latitude solar wind near solar minimum. Rom previous studies, PBSs are believed to be remnants of coronal plumes and be related to network activity such as magnetic reconnection in the photosphere. We investigated the magnetic <span class="hlt">structures</span> of the PBSs, applying a minimum variance analysis to Ulysses/Magnetometer data. At 2001 AGU Spring meeting, we reported that PBSs have <span class="hlt">structures</span> like current sheets or plasmoids, and suggested that they are associated with network activity at the base of polar plumes. In this paper, we have analyzed high-energy <span class="hlt">electron</span> data at Ulysses/SWOOPS to see whether bi-directional <span class="hlt">electron</span> flow exists and confirm the conclusions more precisely. As a result, although most events show a typical flux directed away from the Sun, we have obtained evidence that some PBSs show bi-directional <span class="hlt">electron</span> flux and others show an isotropic distribution of <span class="hlt">electron</span> pitch angles. The evidence shows that plasmoids are flowing away from the Sun, changing their flow direction dynamically in a way not caused by Alfven waves. From this, we have concluded that PBSs are generated due to network activity at the base of polar plumes and their magnetic <span class="hlt">structures</span> axe current sheets or plasmoids.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990041055&hterms=diamond+structure&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Ddiamond%2Bstructure','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990041055&hterms=diamond+structure&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Ddiamond%2Bstructure"><span>Fine <span class="hlt">Structure</span> in the Secondary <span class="hlt">Electron</span> Emission Peak for Diamond Crystal with (100) Negative <span class="hlt">Electron</span> Affinity Surface</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Asnin, V. M.; Krainsky, I. L.</p> <p>1998-01-01</p> <p>A fine <span class="hlt">structure</span> was discovered in the low-energy peak of the secondary <span class="hlt">electron</span> emission spectra of the diamond surface with negative <span class="hlt">electron</span> affinity. We studied this <span class="hlt">structure</span> for the (100) surface of the natural type-IIb diamond crystal. We have found that the low-energy peak consists of a total of four maxima. The relative energy positions of three of them could be related to the <span class="hlt">electron</span> energy minima near the bottom of the conduction band. The fourth peak, having the lowest energy, was attributed to the breakup of the bulk exciton at the surface during the process of secondary <span class="hlt">electron</span> emission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1961c0020S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1961c0020S"><span>β-armchair antimony nanotube: <span class="hlt">Structure</span>, stability and <span class="hlt">electronic</span> properties</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Singh, Shilpa; Gupta, Sanjeev K.; Sonvane, Yogesh; Gajjar, P. N.</p> <p>2018-05-01</p> <p>In the present work, we have used density functional theory (DFT) to investigate the <span class="hlt">structure</span>, stability and <span class="hlt">electronic</span> properties of β-armchair antimony nanotube (ASbNT). We have calculated formation energy and found that β-armchair antimony nanotube (ASbNT) is energetically less stable than β-antimonene. The result shows that β-ASbNT of higher diameter are more stable than nanotubes of lower diameter while <span class="hlt">electronic</span> band <span class="hlt">structure</span> shows semiconducting nature of these nanotubes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730008847','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730008847"><span>Test report: Shock test of the <span class="hlt">electron</span>/proton spectrometer <span class="hlt">structural</span> test unit</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vincent, D. L.</p> <p>1972-01-01</p> <p>A shock test of the <span class="hlt">electron</span>-proton spectrometer <span class="hlt">structural</span> test unit was conducted. The purpose of the shock test was to verify the <span class="hlt">structural</span> integrity of the <span class="hlt">electron</span>-spectrometer design and to obtain data on the shock response of the <span class="hlt">electronics</span> and <span class="hlt">electronic</span> housing. The test equipment is described and typical shock response data are provided.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JAP...111j3110T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JAP...111j3110T"><span>First-principles analysis of <span class="hlt">structural</span> and opto-<span class="hlt">electronic</span> properties of indium tin oxide</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tripathi, Madhvendra Nath; Shida, Kazuhito; Sahara, Ryoji; Mizuseki, Hiroshi; Kawazoe, Yoshiyuki</p> <p>2012-05-01</p> <p>Density functional theory (DFT) and DFT + U (DFT with on-site Coulomb repulsion corrections) calculations have been carried out to study the <span class="hlt">structural</span> and opto-<span class="hlt">electronic</span> properties of indium tin oxide (ITO) for both the oxidized and reduced environment conditions. Some of the results obtained by DFT calculations differ from the experimental observations, such as uncertain indication for the site preference of tin atom to replace indium atom at b-site or d-site, underestimation of <span class="hlt">local</span> inward relaxation in the first oxygen polyhedra around tin atom, and also the improper estimation of <span class="hlt">electronic</span> density of states and hence resulting in an inappropriate optical spectra of ITO. These discrepancies of theoretical outcomes with experimental observations in ITO arise mainly due to the underestimation of the cationic 4d levels within standard DFT calculations. Henceforth, the inclusion of on-site corrections within DFT + U framework significantly modifies the theoretical results in better agreement to the experimental observations. Within this framework, our calculations show that the indium b-site is preferential site over d-site for tin atom substitution in indium oxide under both the oxidized and reduced conditions. Moreover, the calculated average inward relaxation value of 0.16 Å around tin atom is in good agreement with the experimental value of 0.18 Å. Furthermore, DFT + U significantly modify the <span class="hlt">electronic</span> <span class="hlt">structure</span> and consequently induce modifications in the calculated optical spectra of ITO.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29064254','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29064254"><span>Strain-Dependent Edge <span class="hlt">Structures</span> in MoS2 Layers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tinoco, Miguel; Maduro, Luigi; Masaki, Mukai; Okunishi, Eiji; Conesa-Boj, Sonia</p> <p>2017-11-08</p> <p>Edge <span class="hlt">structures</span> are low-dimensional defects unavoidable in layered materials of the transition metal dichalcogenides (TMD) family. Among the various types of such <span class="hlt">structures</span>, the armchair (AC) and zigzag (ZZ) edge types are the most common. It has been predicted that the presence of intrinsic strain <span class="hlt">localized</span> along these edges <span class="hlt">structures</span> can have direct implications for the customization of their <span class="hlt">electronic</span> properties. However, pinning down the relation between <span class="hlt">local</span> <span class="hlt">structure</span> and <span class="hlt">electronic</span> properties at these edges is challenging. Here, we quantify the <span class="hlt">local</span> strain field that arises at the edges of MoS 2 flakes by combining aberration-corrected transmission <span class="hlt">electron</span> microscopy (TEM) with the geometrical-phase analysis (GPA) method. We also provide further insight on the possible effects of such edge strain on the resulting <span class="hlt">electronic</span> behavior by means of <span class="hlt">electron</span> energy loss spectroscopy (EELS) measurements. Our results reveal that the two-dominant edge <span class="hlt">structures</span>, ZZ and AC, induce the formation of different amounts of <span class="hlt">localized</span> strain fields. We also show that by varying the free edge curvature from concave to convex, compressive strain turns into tensile strain. These results pave the way toward the customization of edge <span class="hlt">structures</span> in MoS 2 , which can be used to engineer the properties of layered materials and thus contribute to the optimization of the next generation of atomic-scale <span class="hlt">electronic</span> devices built upon them.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22432573','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22432573"><span><span class="hlt">Structural</span> complexities in the active layers of organic <span class="hlt">electronics</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, Stephanie S; Loo, Yueh-Lin</p> <p>2010-01-01</p> <p>The field of organic <span class="hlt">electronics</span> has progressed rapidly in recent years. However, understanding the direct <span class="hlt">structure</span>-function relationships between the morphology in electrically active layers and the performance of devices composed of these materials has proven difficult. The morphology of active layers in organic <span class="hlt">electronics</span> is inherently complex, with heterogeneities existing across multiple length scales, from subnanometer to micron and millimeter range. A major challenge still facing the organic <span class="hlt">electronics</span> community is understanding how the morphology across all of the length scales in active layers collectively determines the device performance of organic <span class="hlt">electronics</span>. In this review we highlight experiments that have contributed to the elucidation of <span class="hlt">structure</span>-function relationships in organic <span class="hlt">electronics</span> and also point to areas in which knowledge of such relationships is still lacking. Such knowledge will lead to the ability to select active materials on the basis of their inherent properties for the fabrication of devices with prespecified characteristics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1336131-atomistic-interrogation-bn-co-dopant-structures-electronic-effects-graphene','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1336131-atomistic-interrogation-bn-co-dopant-structures-electronic-effects-graphene"><span>Atomistic Interrogation of B–N Co-dopant <span class="hlt">Structures</span> and Their <span class="hlt">Electronic</span> Effects in Graphene</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Schiros, Theanne; Nordlund, Dennis; Palova, Lucia; ...</p> <p>2016-06-21</p> <p>Chemical doping has been demonstrated to be an effective method for producing high-quality, large-area graphene with controlled carrier concentrations and an atomically tailored work function. Furthermore, the emergent optoelectronic properties and surface reactivity of carbon nanostructures are dictated by the microstructure of atomic dopants. Co-doping of graphene with boron and nitrogen offers the possibility to further tune the <span class="hlt">electronic</span> properties of graphene at the atomic level, potentially creating p- and n-type domains in a single carbon sheet, opening a gap between valence and conduction bands in the 2-D semimetal. When using a suite of high-resolution synchrotron-based X-ray techniques, scanning tunnelingmore » microscopy, and density functional theory based computation we visualize and characterize B–N dopant bond <span class="hlt">structures</span> and their <span class="hlt">electronic</span> effects at the atomic level in single-layer graphene grown on a copper substrate. We find there is a thermodynamic driving force for B and N atoms to cluster into BNC <span class="hlt">structures</span> in graphene, rather than randomly distribute into isolated B and N graphitic dopants, although under the present growth conditions, kinetics limit segregation of large B–N domains. We also observe that the doping effect of these BNC <span class="hlt">structures</span>, which open a small band gap in graphene, follows the B:N ratio (B > N, p-type; B < N, n-type; B=N, neutral). We attribute this to the comparable <span class="hlt">electron</span>-withdrawing and -donating effects, respectively, of individual graphitic B and N dopants, although <span class="hlt">local</span> electrostatics also play a role in the work function change.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3382195','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3382195"><span><span class="hlt">Local</span> <span class="hlt">Structural</span> Differences in Homologous Proteins: Specificities in Different SCOP Classes</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Joseph, Agnel Praveen; Valadié, Hélène; Srinivasan, Narayanaswamy; de Brevern, Alexandre G.</p> <p>2012-01-01</p> <p>The constant increase in the number of solved protein <span class="hlt">structures</span> is of great help in understanding the basic principles behind protein folding and evolution. 3-D <span class="hlt">structural</span> knowledge is valuable in designing and developing methods for comparison, modelling and prediction of protein <span class="hlt">structures</span>. These approaches for <span class="hlt">structure</span> analysis can be directly implicated in studying protein function and for drug design. The backbone of a protein <span class="hlt">structure</span> favours certain <span class="hlt">local</span> conformations which include α-helices, β-strands and turns. Libraries of limited number of <span class="hlt">local</span> conformations (<span class="hlt">Structural</span> Alphabets) were developed in the past to obtain a useful categorization of backbone conformation. Protein Block (PB) is one such <span class="hlt">Structural</span> Alphabet that gave a reasonable <span class="hlt">structure</span> approximation of 0.42 Å. In this study, we use PB description of <span class="hlt">local</span> <span class="hlt">structures</span> to analyse conformations that are preferred sites for <span class="hlt">structural</span> variations and insertions, among group of related folds. This knowledge can be utilized in improving tools for <span class="hlt">structure</span> comparison that work by analysing <span class="hlt">local</span> <span class="hlt">structure</span> similarities. Conformational differences between homologous proteins are known to occur often in the regions comprising turns and loops. Interestingly, these differences are found to have specific preferences depending upon the <span class="hlt">structural</span> classes of proteins. Such class-specific preferences are mainly seen in the all-β class with changes involving short helical conformations and hairpin turns. A test carried out on a benchmark dataset also indicates that the use of knowledge on the class specific variations can improve the performance of a PB based <span class="hlt">structure</span> comparison approach. The preference for the indel sites also seem to be confined to a few backbone conformations involving β-turns and helix C-caps. These are mainly associated with short loops joining the regular secondary <span class="hlt">structures</span> that mediate a reversal in the chain direction. Rare β-turns of type I’ and II’ are also</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3197218','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3197218"><span>Advances in <span class="hlt">structural</span> and functional analysis of membrane proteins by <span class="hlt">electron</span> crystallography</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Wisedchaisri, Goragot; Reichow, Steve L.; Gonen, Tamir</p> <p>2011-01-01</p> <p>Summary <span class="hlt">Electron</span> crystallography is a powerful technique for the study of membrane protein <span class="hlt">structure</span> and function in the lipid environment. When well-ordered two-dimensional crystals are obtained the <span class="hlt">structure</span> of both protein and lipid can be determined and lipid-protein interactions analyzed. Protons and ionic charges can be visualized by <span class="hlt">electron</span> crystallography and the protein of interest can be captured for <span class="hlt">structural</span> analysis in a variety of physiologically distinct states. This review highlights the strengths of <span class="hlt">electron</span> crystallography and the momentum that is building up in automation and the development of high throughput tools and methods for <span class="hlt">structural</span> and functional analysis of membrane proteins by <span class="hlt">electron</span> crystallography. PMID:22000511</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1183830-hierarchical-heterogeneity-ceo-tio-interface-electronic-geometric-structural-influence-photocatalytic-activity-oxide-oxide-nanostructures','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1183830-hierarchical-heterogeneity-ceo-tio-interface-electronic-geometric-structural-influence-photocatalytic-activity-oxide-oxide-nanostructures"><span>Hierarchical Heterogeneity at the CeO x –TiO 2 Interface: <span class="hlt">Electronic</span> and Geometric <span class="hlt">Structural</span> Influence on the Photocatalytic Activity of Oxide on Oxide Nanostructures</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Luo, Si; Nguyen-Phan, Thuy-Duong; Johnston-Peck, Aaron C.; ...</p> <p>2015-01-13</p> <p>Mixed oxide interfaces are critical for delivering active components of demanding catalytic processes such as the photo-catalytic splitting of water. We have studied CeO xTiO₂ catalysts with low ceria loadings of 1 wt%, 3 wt% and 6 wt% that were prepared with wet impregnation methods to favor a strong interaction between CeO x and TiO₂. In these materials the interfaces between CeO x-TiO₂ have been sequentially loaded (1%, 3% and 6%), with and without Pt (0.5 wt%). The <span class="hlt">structure</span> and properties of the catalysts were characterized using several X-ray and <span class="hlt">electron</span> based techniques including XRD, XPS, UPS, NEXAFS, UV-Vis andmore » HR-STEM/STEM-EELS, to unravel the <span class="hlt">local</span> morphology, bulk <span class="hlt">structure</span>, surface states and <span class="hlt">electronic</span> <span class="hlt">structure</span>. The combination of all these techniques allow us to analyze in a systematic way the complete <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties that prevail at the CeO x-TiO₂ interface. Fluorite <span class="hlt">structured</span> nano crystallites of ceria on anatase-<span class="hlt">structured</span> titania were identified by both XRD and NEXAFS. A sequential increasing of the CeO x loading led to the formation of clusters, then plates and finally nano particles in a hierarchical manner on the TiO₂ support. The <span class="hlt">electronic</span> <span class="hlt">structures</span> of these catalysts indicate that the interaction between TiO₂ and CeO₂ is closely related to the <span class="hlt">local</span> morphology of nanostructured CeO₂. Ce³⁺ cations were detected at the surface of CeO₂ and at the interface of the two oxides. In addition, the titania is perturbed by the interaction with ceria and also with Pt. The photocatalytic activity for the splitting of H₂O using UV light was measured for these materials and correlated with our understanding of the <span class="hlt">electronic</span> and <span class="hlt">structural</span> properties. Optimal catalytic performance and photo response results were found for the 1 wt% CeO x-TiO₂ catalyst where low dimensional geometry of the ceria provided ideal <span class="hlt">electronic</span> and geometrical properties. The <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..MAR.P1345D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..MAR.P1345D"><span><span class="hlt">Electronic</span> <span class="hlt">Structure</span> Calculation of Permanent Magnets using the KKR Green's Function Method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Doi, Shotaro; Akai, Hisazumi</p> <p>2014-03-01</p> <p><span class="hlt">Electronic</span> <span class="hlt">structure</span> and magnetic properties of permanent magnetic materials, especially Nd2Fe14B, are investigated theoretically using the KKR Green's function method. Important physical quantities in magnetism, such as magnetic moment, Curie temperature, and anisotropy constant, which are obtained from <span class="hlt">electronics</span> <span class="hlt">structure</span> calculations in both cases of atomic-sphere-approximation and full-potential treatment, are compared with past band <span class="hlt">structure</span> calculations and experiments. The site preference of heavy rare-earth impurities are also evaluated through the calculation of formation energy with the use of coherent potential approximations. Further, the development of <span class="hlt">electronic</span> <span class="hlt">structure</span> calculation code using the screened KKR for large super-cells, which is aimed at studying the <span class="hlt">electronic</span> <span class="hlt">structure</span> of realistic microstructures (e.g. grain boundary phase), is introduced with some test calculations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1393357','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1393357"><span>A geometric initial guess for <span class="hlt">localized</span> <span class="hlt">electronic</span> orbitals in modular biological systems</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>Beckman, P. G.; Fattebert, J. L.; Lau, E. Y.</p> <p></p> <p>Recent first-principles molecular dynamics algorithms using <span class="hlt">localized</span> <span class="hlt">electronic</span> orbitals have achieved O(N) complexity and controlled accuracy in simulating systems with finite band gaps. However, accurately deter- mining the centers of these <span class="hlt">localized</span> orbitals during simulation setup may require O(N 3) operations, which is computationally infeasible for many biological systems. We present an O(N) approach for approximating orbital centers in proteins, DNA, and RNA which uses non-<span class="hlt">localized</span> solutions for a set of fixed-size subproblems to create a set of geometric maps applicable to larger systems. This scalable approach, used as an initial guess in the O(N) first-principles molecular dynamics code MGmol,more » facilitates first-principles simulations in biological systems of sizes which were previously impossible.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5343910','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5343910"><span>Recognition of <span class="hlt">Local</span> DNA <span class="hlt">Structures</span> by p53 Protein</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Brázda, Václav; Coufal, Jan</p> <p>2017-01-01</p> <p>p53 plays critical roles in regulating cell cycle, apoptosis, senescence and metabolism and is commonly mutated in human cancer. These roles are achieved by interaction with other proteins, but particularly by interaction with DNA. As a transcription factor, p53 is well known to bind consensus target sequences in linear B-DNA. Recent findings indicate that p53 binds with higher affinity to target sequences that form cruciform DNA <span class="hlt">structure</span>. Moreover, p53 binds very tightly to non-B DNA <span class="hlt">structures</span> and <span class="hlt">local</span> DNA <span class="hlt">structures</span> are increasingly recognized to influence the activity of wild-type and mutant p53. Apart from cruciform <span class="hlt">structures</span>, p53 binds to quadruplex DNA, triplex DNA, DNA loops, bulged DNA and hemicatenane DNA. In this review, we describe <span class="hlt">local</span> DNA <span class="hlt">structures</span> and summarize information about interactions of p53 with these <span class="hlt">structural</span> DNA motifs. These recent data provide important insights into the complexity of the p53 pathway and the functional consequences of wild-type and mutant p53 activation in normal and tumor cells. PMID:28208646</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhyS...90c5805K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhyS...90c5805K"><span><span class="hlt">Electron</span> spin relaxation in two polymorphic <span class="hlt">structures</span> of GaN</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kang, Nam Lyong</p> <p>2015-03-01</p> <p>The relaxation process of <span class="hlt">electron</span> spin in systems of <span class="hlt">electrons</span> interacting with piezoelectric deformation phonons that are mediated through spin-orbit interactions was interpreted from a microscopic point of view using the formula for the <span class="hlt">electron</span> spin relaxation times derived by a projection-reduction method. The <span class="hlt">electron</span> spin relaxation times in two polymorphic <span class="hlt">structures</span> of GaN were calculated. The piezoelectric material constant for the wurtzite <span class="hlt">structure</span> obtained by a comparison with a previously reported experimental result was {{P}pe}=1.5 × {{10}29} eV {{m}-1}. The temperature and magnetic field dependence of the relaxation times for both wurtzite and zinc-blende <span class="hlt">structures</span> were similar, but the relaxation times in zinc-blende GaN were smaller and decreased more rapidly with increasing temperature and magnetic field than that in wurtzite GaN. This study also showed that the <span class="hlt">electron</span> spin relaxation for wurtzite GaN at low density could be explained by the Elliot-Yafet process but not for zinc-blende GaN in the metallic regime.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EPJB...89...98M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EPJB...89...98M"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> of uracil-like nucleobases adsorbed on Si(001): uracil, thymine and 5-fluorouracil</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Molteni, Elena; Onida, Giovanni; Cappellini, Giancarlo</p> <p>2016-04-01</p> <p>We study the <span class="hlt">electronic</span> properties of the Si(001):Uracil, Si(001):Thymine, and Si(001):5-Fluorouracil systems, focusing on the Si dimer-bridging configuration with adsorption governed by carbonyl groups. While the overall <span class="hlt">structural</span> and <span class="hlt">electronic</span> properties are similar, with small differences due to chemical substitutions, much larger effects on the surface band dispersion and bandgap show up as a function of the molecular orientation with respect to the surface. An off-normal orientation of the molecular planes is favored, showing larger bandgap and lower total energy than the upright position. We also analyze the <span class="hlt">localization</span> of gap-edge occupied and unoccupied surface states. Supplementary material in the form of one pdf file available from the Journal web page at http://dx.doi.org/10.1140/epjb/e2016-70011-1</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPCM...30i5704B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPCM...30i5704B"><span><span class="hlt">Electronic</span> <span class="hlt">structure</span> and magnetic properties of Pr-Co intermetallics: ab initio FP-LAPW calculations and correlation with experiments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bakkari, Karim; Fersi, Riadh; Kebir Hlil, El; Bessais, Lotfi; Thabet Mliki, Najeh</p> <p>2018-03-01</p> <p>First-principle calculations combining density functional theory and the full-potential linearized augmented plane wave (FP-LAPW) method are performed to investigate the <span class="hlt">electronic</span> and magnetic <span class="hlt">structure</span> of Pr2Co7 in its two polymorphic forms, (2:7 H) and (2:7 R), for the first time. This type of calculation was also performed for PrCo5 and PrCo2 intermetallics. We have computed the valence density of states separately for spin-up and spin-down states in order to investigate the <span class="hlt">electronic</span> band <span class="hlt">structure</span>. This is governed by the strong contribution of the partial DOS of 3d-Co bands compared to the partial DOS of the 4f-Pr bands. Such a high ferromagnetic state is discussed in terms of the strong spin polarization observed in the total DOS. The magnetic moments carried by the Co and Pr atoms located in several sites for all compounds are computed. These results mainly indicate that cobalt atoms make a dominant contribution to the magnetic moments. The notable difference in the atomic moments of Pr and Co atoms between different <span class="hlt">structural</span> slabs is explained in terms of the magnetic characteristics of the PrCo2 and PrCo5 compounds and the <span class="hlt">local</span> chemical environments of the Pr and Co atoms in different <span class="hlt">structural</span> slabs of Pr2Co7. From spin-polarized calculations we have simulated the 3d and 4f band population to estimate the <span class="hlt">local</span> magnetic moments. These results are in accordance with the magnetic moments calculated using the FP-LAPW method. In addition, the exchange interactions J ij are calculated and used as input for M(T) simulations. Involving the data obtained from the <span class="hlt">electronic</span> <span class="hlt">structure</span> calculations, the appropriate Padé Table is applied to simulate the magnetization M(T) and to estimate the mean-field Curie temperature. We report a fairly good agreement between the ab initio calculation of magnetization and Curie temperature with the experimental data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5677355','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5677355"><span>Monaural Sound <span class="hlt">Localization</span> Based on Reflective <span class="hlt">Structure</span> and Homomorphic Deconvolution</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, Yeonseok; Choi, Anthony</p> <p>2017-01-01</p> <p>The asymmetric <span class="hlt">structure</span> around the receiver provides a particular time delay for the specific incoming propagation. This paper designs a monaural sound <span class="hlt">localization</span> system based on the reflective <span class="hlt">structure</span> around the microphone. The reflective plates are placed to present the direction-wise time delay, which is naturally processed by convolutional operation with a sound source. The received signal is separated for estimating the dominant time delay by using homomorphic deconvolution, which utilizes the real cepstrum and inverse cepstrum sequentially to derive the propagation response’s autocorrelation. Once the <span class="hlt">localization</span> system accurately estimates the information, the time delay model computes the corresponding reflection for <span class="hlt">localization</span>. Because of the <span class="hlt">structure</span> limitation, two stages of the <span class="hlt">localization</span> process perform the estimation procedure as range and angle. The software toolchain from propagation physics and algorithm simulation realizes the optimal 3D-printed <span class="hlt">structure</span>. The acoustic experiments in the anechoic chamber denote that 79.0% of the study range data from the isotropic signal is properly detected by the response value, and 87.5% of the specific direction data from the study range signal is properly estimated by the response time. The product of both rates shows the overall hit rate to be 69.1%. PMID:28946625</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=ab-initio&pg=2&id=EJ161081','ERIC'); return false;" href="https://eric.ed.gov/?q=ab-initio&pg=2&id=EJ161081"><span>Instructional Approach to Molecular <span class="hlt">Electronic</span> <span class="hlt">Structure</span> Theory</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>Dykstra, Clifford E.; Schaefer, Henry F.</p> <p>1977-01-01</p> <p>Describes a graduate quantum mechanics projects in which students write a computer program that performs ab initio calculations on the <span class="hlt">electronic</span> <span class="hlt">structure</span> of a simple molecule. Theoretical potential energy curves are produced. (MLH)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JMOp...65.1535Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JMOp...65.1535Z"><span><span class="hlt">Electronically</span> controlled spoof <span class="hlt">localized</span> surface plasmons on the corrugated ring with a shorting pin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Chao; Zhou, Yong Jin</p> <p>2018-07-01</p> <p>We have demonstrated that spoof <span class="hlt">localized</span> surface plasmons (LSPs) can be controlled by loading a shorting pin into the corrugated ring resonator in the microwave and terahertz (THz) frequencies. <span class="hlt">Electronical</span> switchability and tunability of spoof LSPs have been achieved by mounting Schottky barrier diodes and varactor diodes across the slit around the shorting pin in the ground plane. An <span class="hlt">electronically</span> tunable band-pass filter has been demostrated in the microwave frequencies. Such <span class="hlt">electronically</span> controlled spoof LSPs devices can find more applications for highly integrated plasmonic circuits in microwave and THz frequencies.</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('https://www.osti.gov/pages/biblio/1372697-molecular-electronic-structures-m2o7-mn-tc-re','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1372697-molecular-electronic-structures-m2o7-mn-tc-re"><span>Molecular and <span class="hlt">electronic</span> <span class="hlt">structures</span> of M 2O 7 (M = Mn, Tc, Re)</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Lawler, Keith V.; Childs, Bradley C.; Mast, Daniel S.; ...</p> <p>2017-02-21</p> <p>The molecular and <span class="hlt">electronic</span> <span class="hlt">structures</span> for the Group 7b heptoxides were investigated by computational methods as both isolated molecules and in the solid-state. The metal-oxygen-metal bending angle of the single molecule increased with increasing atomic number, with Re 2O 7 preferring a linear <span class="hlt">structure</span>. Natural bond orbital and <span class="hlt">localized</span> orbital bonding analyses indicate that there is a three-center covalent bond between the metal atoms and the bridging oxygen, and the increasing ionic character of the bonds favors larger bond angles. The calculations accurately reproduce the experimental crystal <span class="hlt">structures</span> within a few percent. Analysis of the band <span class="hlt">structures</span> and density ofmore » states shows similar bonding for all of the solid-state heptoxides, including the presence of the three-center covalent bond. DFT+U simulations show that PBE-D3 underpredicts the band gap by ~0.2 eV due to an under-correlation of the metal d conducting states. As a result, homologue and compression studies show that Re 2O 7 adopts a polymeric <span class="hlt">structure</span> because the Re-oxide tetrahedra are easily distorted by packing stresses to form additional three-center covalent bonds.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97x5118E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97x5118E"><span>Spin <span class="hlt">localization</span>, magnetic ordering, and <span class="hlt">electronic</span> properties of strongly correlated Ln2O3 sesquioxides (Ln=La, Ce, Pr, Nd)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>El-Kelany, Kh. E.; Ravoux, C.; Desmarais, J. K.; Cortona, P.; Pan, Y.; Tse, J. S.; Erba, A.</p> <p>2018-06-01</p> <p>Lanthanide sesquioxides are strongly correlated materials characterized by highly <span class="hlt">localized</span> unpaired <span class="hlt">electrons</span> in the f band. Theoretical descriptions based on standard density functional theory (DFT) formulations are known to be unable to correctly describe their peculiar <span class="hlt">electronic</span> and magnetic features. In this study, <span class="hlt">electronic</span> and magnetic properties of the first four lanthanide sesquioxides in the series are characterized through a reliable description of spin <span class="hlt">localization</span> as ensured by hybrid functionals of the DFT, which include a fraction of nonlocal Fock exchange. Because of the high <span class="hlt">localization</span> of the f <span class="hlt">electrons</span>, multiple metastable <span class="hlt">electronic</span> configurations are possible for their ground state depending on the specific partial occupation of the f orbitals: the most stable configuration is here found and characterized for all systems. Magnetic ordering is explicitly investigated, and the higher stability of an antiferromagnetic configuration with respect to the ferromagnetic one is predicted. The critical role of the fraction of exchange on the description of their <span class="hlt">electronic</span> properties (notably, on spin <span class="hlt">localization</span> and on the <span class="hlt">electronic</span> band gap) is addressed. In particular, a recently proposed theoretical approach based on a self-consistent definition—through the material dielectric response—of the optimal fraction of exchange in hybrid functionals is applied to these strongly correlated materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvB..96w5133M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvB..96w5133M"><span>Configuration-specific <span class="hlt">electronic</span> <span class="hlt">structure</span> of strongly interacting interfaces: TiOPc on Cu(110)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Maughan, Bret; Zahl, Percy; Sutter, Peter; Monti, Oliver L. A.</p> <p>2017-12-01</p> <p>We use low-temperature scanning tunneling microscopy in combination with angle-resolved ultraviolet and two-photon photoemission spectroscopy to investigate the interfacial <span class="hlt">electronic</span> <span class="hlt">structure</span> of titanyl phthalocyanine (TiOPc) on Cu(110). We show that the presence of two unique molecular adsorption configurations is crucial for a molecular-level analysis of the hybridized interfacial <span class="hlt">electronic</span> <span class="hlt">structure</span>. Specifically, thermally induced self-assembly exposes marked adsorbate-configuration-specific contributions to the interfacial <span class="hlt">electronic</span> <span class="hlt">structure</span>. The results of this work demonstrate an avenue towards understanding and controlling interfacial <span class="hlt">electronic</span> <span class="hlt">structure</span> in chemisorbed films even for the case of complex film <span class="hlt">structure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21115172','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21115172"><span>Present and future of membrane protein <span class="hlt">structure</span> determination by <span class="hlt">electron</span> crystallography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ubarretxena-Belandia, Iban; Stokes, David L</p> <p>2010-01-01</p> <p>Membrane proteins are critical to cell physiology, playing roles in signaling, trafficking, transport, adhesion, and recognition. Despite their relative abundance in the proteome and their prevalence as targets of therapeutic drugs, <span class="hlt">structural</span> information about membrane proteins is in short supply. This chapter describes the use of <span class="hlt">electron</span> crystallography as a tool for determining membrane protein <span class="hlt">structures</span>. <span class="hlt">Electron</span> crystallography offers distinct advantages relative to the alternatives of X-ray crystallography and NMR spectroscopy. Namely, membrane proteins are placed in their native membranous environment, which is likely to favor a native conformation and allow changes in conformation in response to physiological ligands. Nevertheless, there are significant logistical challenges in finding appropriate conditions for inducing membrane proteins to form two-dimensional arrays within the membrane and in using <span class="hlt">electron</span> cryo-microscopy to collect the data required for <span class="hlt">structure</span> determination. A number of developments are described for high-throughput screening of crystallization trials and for automated imaging of crystals with the <span class="hlt">electron</span> microscope. These tools are critical for exploring the necessary range of factors governing the crystallization process. There have also been recent software developments to facilitate the process of <span class="hlt">structure</span> determination. However, further innovations in the algorithms used for processing images and <span class="hlt">electron</span> diffraction are necessary to improve throughput and to make <span class="hlt">electron</span> crystallography truly viable as a method for determining atomic <span class="hlt">structures</span> of membrane proteins. Copyright © 2010 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3121533','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3121533"><span>Present and future of membrane protein <span class="hlt">structure</span> determination by <span class="hlt">electron</span> crystallography</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ubarretxena-Belandia, Iban; Stokes, David L.</p> <p>2011-01-01</p> <p>Membrane proteins are critical to cell physiology, playing roles in signaling, trafficking, transport, adhesion, and recognition. Despite their relative abundance in the proteome and their prevalence as targets of therapeutic drugs, <span class="hlt">structural</span> information about membrane proteins is in short supply. This review describes the use of <span class="hlt">electron</span> crystallography as a tool for determining membrane protein <span class="hlt">structures</span>. <span class="hlt">Electron</span> crystallography offers distinct advantages relative to the alternatives of X-ray crystallography and NMR spectroscopy. Namely, membrane proteins are placed in their native membranous environment, which is likely to favor a native conformation and allow changes in conformation in response to physiological ligands. Nevertheless, there are significant logistical challenges in finding appropriate conditions for inducing membrane proteins to form two-dimensional arrays within the membrane and in using <span class="hlt">electron</span> cryo-microscopy to collect the data required for <span class="hlt">structure</span> determination. A number of developments are described for high-throughput screening of crystallization trials and for automated imaging of crystals with the <span class="hlt">electron</span> microscope. These tools are critical for exploring the necessary range of factors governing the crystallization process. There have also been recent software developments to facilitate the process of <span class="hlt">structure</span> determination. However, further innovations in the algorithms used for processing images and <span class="hlt">electron</span> diffraction are necessary to improve throughput and to make <span class="hlt">electron</span> crystallography truly viable as a method for determining atomic <span class="hlt">structures</span> of membrane proteins. PMID:21115172</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PrSS...90....1T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PrSS...90....1T"><span>Silicene on Ag(1 1 1): Geometric and <span class="hlt">electronic</span> <span class="hlt">structures</span> of a new honeycomb material of Si</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Takagi, Noriaki; Lin, Chun-Liang; Kawahara, Kazuaki; Minamitani, Emi; Tsukahara, Noriyuki; Kawai, Maki; Arafune, Ryuichi</p> <p>2015-02-01</p> <p>Silicene, a two-dimensional honeycomb sheet consisting of Si atoms, has attracted much attention as a new low-dimensional material because it gains various fascinating characteristics originating from the combination of Dirac fermion features with spin-orbit coupling. The novel properties such as the quantum spin Hall effect and the compatibility with the current Si device technologies have fueled competition to realize the silicene. This review article focuses on the geometric and <span class="hlt">electronic</span> <span class="hlt">structures</span> of silicene grown on Ag(1 1 1) investigated by scanning tunneling microcopy (STM), low energy <span class="hlt">electron</span> diffraction (LEED) and density functional theory (DFT) calculations. The silicene on Ag(1 1 1) takes <span class="hlt">locally</span>-buckled <span class="hlt">structure</span> in which the Si atoms are displaced perpendicularly to the basal plane. As a result, several superstructures such as 4 × 4,√{ 13 } ×√{ 13 } R 13.9 °, 4 /√{ 3 } × 4 /√{ 3 } , and etc. emerge. The atomic arrangement of the 4 × 4 silicene has been determined by STM, DFT calculations and LEED dynamical analysis, while the other superstructures remain to be fully-resolved. In the 4 × 4 silicene, Si atoms are arranged to form a buckled honeycomb <span class="hlt">structure</span> where six Si atoms of 18 Si atoms in the unit cell are displaced vertically. The displacements lead to the vertical shift of the substrate Ag atoms, indicating the non-negligible coupling at the interface between the silicene layer and the substrate. The interface coupling significantly modifies the <span class="hlt">electronic</span> <span class="hlt">structure</span> of the 4 × 4 silicene. No Landau level sequences were observed by scanning tunneling spectroscopy (STS) with magnetic fields applied perpendicularly to the sample surface. The DFT calculations showed that the π and π∗ bands derived from the Si 3pz are hybridized with the Ag <span class="hlt">electronic</span> states, leading to the drastic modification in the band <span class="hlt">structure</span> and then the absence of Dirac fermion features together with the two-dimensionality in the <span class="hlt">electronic</span> states</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22230825-hybrid-preconditioning-iterative-diagonalization-ill-conditioned-generalized-eigenvalue-problems-electronic-structure-calculations','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22230825-hybrid-preconditioning-iterative-diagonalization-ill-conditioned-generalized-eigenvalue-problems-electronic-structure-calculations"><span>Hybrid preconditioning for iterative diagonalization of ill-conditioned generalized eigenvalue problems in <span class="hlt">electronic</span> <span class="hlt">structure</span> calculations</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>Cai, Yunfeng, E-mail: yfcai@math.pku.edu.cn; Department of Computer Science, University of California, Davis 95616; Bai, Zhaojun, E-mail: bai@cs.ucdavis.edu</p> <p>2013-12-15</p> <p>The iterative diagonalization of a sequence of large ill-conditioned generalized eigenvalue problems is a computational bottleneck in quantum mechanical methods employing a nonorthogonal basis for ab initio <span class="hlt">electronic</span> <span class="hlt">structure</span> calculations. We propose a hybrid preconditioning scheme to effectively combine global and <span class="hlt">locally</span> accelerated preconditioners for rapid iterative diagonalization of such eigenvalue problems. In partition-of-unity finite-element (PUFE) pseudopotential density-functional calculations, employing a nonorthogonal basis, we show that the hybrid preconditioned block steepest descent method is a cost-effective eigensolver, outperforming current state-of-the-art global preconditioning schemes, and comparably efficient for the ill-conditioned generalized eigenvalue problems produced by PUFE as the <span class="hlt">locally</span> optimal blockmore » preconditioned conjugate-gradient method for the well-conditioned standard eigenvalue problems produced by planewave methods.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM33C2674T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM33C2674T"><span>Effect of plasma density around Io on <span class="hlt">local</span> <span class="hlt">electron</span> heating in the Io plasma torus</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsuchiya, F.; Yoshioka, K.; Kagitani, M.; Kimura, T.; Murakami, G.; Yamazaki, A.; Misawa, H.; Kasaba, Y.; Yoshikawa, I.; Sakanoi, T.; Koga, R.; Ryo, A.; Suzuki, F.; Hikida, R.</p> <p>2017-12-01</p> <p>HISAKI observation of Io plasma torus (IPT) with extreme ultraviolet (EUV) wavelength range is a useful probe to access plasma environment in inner magnetosphere of Jupiter. Emissions from sulfur and oxygen ions in EUV range are caused by <span class="hlt">electron</span> impact excitation and their intensity is well correlated with the abundance of hot <span class="hlt">electron</span> in IPT. Previous observation showed that the brightness was enhanced downstream of the satellite Io, indicating that efficient <span class="hlt">electron</span> heating takes place at Io and/or just downstream of Io. Detailed analysis of the emission intensity shows that the brightness depends on the magnetic longitude at Io and primary and secondary peaks appear in the longitude ranges of 100-130 and 250-340 degrees, respectively. The peak position and amplitude are slightly different between dawn and dusk sides. Here, we introduce inhomogeneous IPT density model in order to investigate relation between the emission intensity and <span class="hlt">local</span> plasma density around Io in detail. An empirical IPT model is used for spatial distribution of ion and <span class="hlt">electron</span> densities in the meridional plane. To include longitude and <span class="hlt">local</span> time asymmetry in IPT, we consider (1)dawnward shift of IPT due to global convection electric field, (2) offset of Jupiter's dipole magnetic field, and (3) tilt of IPT with respect to Io's orbital plane. The modeled <span class="hlt">electron</span> density at the position of Io as a function of magnetic longitude at Io shows similar profile with the ion emission intensity derived from the observation. This result suggests that energy extracted around Io and/or efficiency of <span class="hlt">electron</span> heating is closely related to the plasma density around Io and longitude and <span class="hlt">local</span> time dependences is explained by the spatial inhomogeneity of plasma density in IPT. A part of the energy extracted around Io could be transferred to the Jovian ionosphere along the magnetic field line and cause bright aurora spots and strong radio emissions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=gas+AND+liquid&pg=5&id=EJ106421','ERIC'); return false;" href="https://eric.ed.gov/?q=gas+AND+liquid&pg=5&id=EJ106421"><span><span class="hlt">Structure</span> of Wet Specimens in <span class="hlt">Electron</span> Microscopy</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>Parsons, D. F.</p> <p>1974-01-01</p> <p>Discussed are past work and recent advances in the use of <span class="hlt">electron</span> microscopes for viewing <span class="hlt">structures</span> immersed in gas and liquid. Improved environmental chambers make it possible to examine wet specimens easily. (Author/RH)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22658020-real-space-visualization-conformation-independent-oligothiophene-electronic-structure','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22658020-real-space-visualization-conformation-independent-oligothiophene-electronic-structure"><span>Real-space visualization of conformation-independent oligothiophene <span class="hlt">electronic</span> <span class="hlt">structure</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>Taber, Benjamen N.; Kislitsyn, Dmitry A.; Gervasi, Christian F.</p> <p>2016-05-21</p> <p>We present scanning tunneling microscopy and spectroscopy (STM/STS) investigations of the <span class="hlt">electronic</span> <span class="hlt">structures</span> of different alkyl-substituted oligothiophenes on the Au(111) surface. STM imaging showed that on Au(111), oligothiophenes adopted distinct straight and bent conformations. By combining STS maps with STM images, we visualize, in real space, particle-in-a-box-like oligothiophene molecular orbitals. We demonstrate that different planar conformers with significant geometrical distortions of oligothiophene backbones surprisingly exhibit very similar <span class="hlt">electronic</span> <span class="hlt">structures</span>, indicating a low degree of conformation-induced <span class="hlt">electronic</span> disorder. The agreement of these results with gas-phase density functional theory calculations implies that the oligothiophene interaction with the Au(111) surface is generally insensitivemore » to molecular conformation.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22000511','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22000511"><span>Advances in <span class="hlt">structural</span> and functional analysis of membrane proteins by <span class="hlt">electron</span> crystallography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wisedchaisri, Goragot; Reichow, Steve L; Gonen, Tamir</p> <p>2011-10-12</p> <p><span class="hlt">Electron</span> crystallography is a powerful technique for the study of membrane protein <span class="hlt">structure</span> and function in the lipid environment. When well-ordered two-dimensional crystals are obtained the <span class="hlt">structure</span> of both protein and lipid can be determined and lipid-protein interactions analyzed. Protons and ionic charges can be visualized by <span class="hlt">electron</span> crystallography and the protein of interest can be captured for <span class="hlt">structural</span> analysis in a variety of physiologically distinct states. This review highlights the strengths of <span class="hlt">electron</span> crystallography and the momentum that is building up in automation and the development of high throughput tools and methods for <span class="hlt">structural</span> and functional analysis of membrane proteins by <span class="hlt">electron</span> crystallography. Copyright © 2011 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5333154','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5333154"><span><span class="hlt">Local</span> <span class="hlt">structures</span> around the substituted elements in mixed layered oxides</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Akama, Shota; Kobayashi, Wataru; Amaha, Kaoru; Niwa, Hideharu; Nitani, Hiroaki; Moritomo, Yutaka</p> <p>2017-01-01</p> <p>The chemical substitution of a transition metal (M) is an effective method to improve the functionality of a material, such as its electrochemical, magnetic, and dielectric properties. The substitution, however, causes <span class="hlt">local</span> lattice distortion because the difference in the ionic radius (r) modifies the <span class="hlt">local</span> interatomic distances. Here, we systematically investigated the <span class="hlt">local</span> <span class="hlt">structures</span> in the pure (x = 0.0) and mixed (x = 0.05 or 0.1) layered oxides, Na(M1−xM′x)O2 (M and M′ are the majority and minority transition metals, respectively), by means of extended X-ray absorption fine <span class="hlt">structure</span> (EXAFS) analysis. We found that the <span class="hlt">local</span> interatomic distance (dM-O) around the minority element approaches that around the majority element to reduces the <span class="hlt">local</span> lattice distortion. We further found that the valence of the minority Mn changes so that its ionic radius approaches that of the majority M. PMID:28252008</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1913617K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1913617K"><span>Adjoint-tomography for a <span class="hlt">Local</span> Surface <span class="hlt">Structure</span>: Methodology and a Blind Test</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kubina, Filip; Michlik, Filip; Moczo, Peter; Kristek, Jozef; Stripajova, Svetlana</p> <p>2017-04-01</p> <p>We have developed a multiscale full-waveform adjoint-tomography method for <span class="hlt">local</span> surface sedimentary <span class="hlt">structures</span> with complicated interference wavefields. The <span class="hlt">local</span> surface sedimentary basins and valleys are often responsible for anomalous earthquake ground motions and corresponding damage in earthquakes. In many cases only relatively small number of records of a few <span class="hlt">local</span> earthquakes is available for a site of interest. Consequently, prediction of earthquake ground motion at the site has to include numerical modeling for a realistic model of the <span class="hlt">local</span> <span class="hlt">structure</span>. Though limited, the information about the <span class="hlt">local</span> <span class="hlt">structure</span> encoded in the records is important and irreplaceable. It is therefore reasonable to have a method capable of using the limited information in records for improving a model of the <span class="hlt">local</span> <span class="hlt">structure</span>. A <span class="hlt">local</span> surface <span class="hlt">structure</span> and its interference wavefield require a specific multiscale approach. In order to verify our inversion method, we performed a blind test. We obtained synthetic seismograms at 8 receivers for 2 <span class="hlt">local</span> sources, complete description of the sources, positions of the receivers and material parameters of the bedrock. We considered the simplest possible starting model - a homogeneous halfspace made of the bedrock. Using our inversion method we obtained an inverted model. Given the starting model, synthetic seismograms simulated for the inverted model are surprisingly close to the synthetic seismograms simulated for the true <span class="hlt">structure</span> in the target frequency range up to 4.5 Hz. We quantify the level of agreement between the true and inverted seismograms using the L2 and time-frequency misfits, and, more importantly for earthquake-engineering applications, also using the goodness-of-fit criteria based on the earthquake-engineering characteristics of earthquake ground motion. We also verified the inverted model for other source-receiver configurations not used in the inversion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3224362','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3224362"><span>Deciphering the shape and deformation of secondary <span class="hlt">structures</span> through <span class="hlt">local</span> conformation analysis</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>Background Protein deformation has been extensively analysed through global methods based on RMSD, torsion angles and Principal Components Analysis calculations. Here we use a <span class="hlt">local</span> approach, able to distinguish among the different backbone conformations within loops, α-helices and β-strands, to address the question of secondary <span class="hlt">structures</span>' shape variation within proteins and deformation at interface upon complexation. Results Using a <span class="hlt">structural</span> alphabet, we translated the 3 D <span class="hlt">structures</span> of large sets of protein-protein complexes into sequences of <span class="hlt">structural</span> letters. The shape of the secondary <span class="hlt">structures</span> can be assessed by the <span class="hlt">structural</span> letters that modeled them in the <span class="hlt">structural</span> sequences. The distribution analysis of the <span class="hlt">structural</span> letters in the three protein compartments (surface, core and interface) reveals that secondary <span class="hlt">structures</span> tend to adopt preferential conformations that differ among the compartments. The <span class="hlt">local</span> description of secondary <span class="hlt">structures</span> highlights that curved conformations are preferred on the surface while straight ones are preferred in the core. Interfaces display a mixture of <span class="hlt">local</span> conformations either preferred in core or surface. The analysis of the <span class="hlt">structural</span> letters transition occurring between protein-bound and unbound conformations shows that the deformation of secondary <span class="hlt">structure</span> is tightly linked to the compartment preference of the <span class="hlt">local</span> conformations. Conclusion The conformation of secondary <span class="hlt">structures</span> can be further analysed and detailed thanks to a <span class="hlt">structural</span> alphabet which allows a better description of protein surface, core and interface in terms of secondary <span class="hlt">structures</span>' shape and deformation. Induced-fit modification tendencies described here should be valuable information to identify and characterize regions under strong <span class="hlt">structural</span> constraints for functional reasons. PMID:21284872</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21284872','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21284872"><span>Deciphering the shape and deformation of secondary <span class="hlt">structures</span> through <span class="hlt">local</span> conformation analysis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Baussand, Julie; Camproux, Anne-Claude</p> <p>2011-02-01</p> <p>Protein deformation has been extensively analysed through global methods based on RMSD, torsion angles and Principal Components Analysis calculations. Here we use a <span class="hlt">local</span> approach, able to distinguish among the different backbone conformations within loops, α-helices and β-strands, to address the question of secondary <span class="hlt">structures</span>' shape variation within proteins and deformation at interface upon complexation. Using a <span class="hlt">structural</span> alphabet, we translated the 3 D <span class="hlt">structures</span> of large sets of protein-protein complexes into sequences of <span class="hlt">structural</span> letters. The shape of the secondary <span class="hlt">structures</span> can be assessed by the <span class="hlt">structural</span> letters that modeled them in the <span class="hlt">structural</span> sequences. The distribution analysis of the <span class="hlt">structural</span> letters in the three protein compartments (surface, core and interface) reveals that secondary <span class="hlt">structures</span> tend to adopt preferential conformations that differ among the compartments. The <span class="hlt">local</span> description of secondary <span class="hlt">structures</span> highlights that curved conformations are preferred on the surface while straight ones are preferred in the core. Interfaces display a mixture of <span class="hlt">local</span> conformations either preferred in core or surface. The analysis of the <span class="hlt">structural</span> letters transition occurring between protein-bound and unbound conformations shows that the deformation of secondary <span class="hlt">structure</span> is tightly linked to the compartment preference of the <span class="hlt">local</span> conformations. The conformation of secondary <span class="hlt">structures</span> can be further analysed and detailed thanks to a <span class="hlt">structural</span> alphabet which allows a better description of protein surface, core and interface in terms of secondary <span class="hlt">structures</span>' shape and deformation. Induced-fit modification tendencies described here should be valuable information to identify and characterize regions under strong <span class="hlt">structural</span> constraints for functional reasons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvM...2d4203S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvM...2d4203S"><span><span class="hlt">Electronic</span> and <span class="hlt">structural</span> properties of B i2S e3:Cu</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sobczak, Kamil; Strak, Pawel; Kempisty, Pawel; Wolos, Agnieszka; Hruban, Andrzej; Materna, Andrzej; Borysiuk, Jolanta</p> <p>2018-04-01</p> <p><span class="hlt">Electronic</span> and <span class="hlt">structural</span> properties of B i2S e3 and its extension to copper doped B i2S e3:Cu were studied using combined ab initio simulations and transmission <span class="hlt">electron</span> microscopy based techniques, including <span class="hlt">electron</span> energy loss spectroscopy, energy filtered transmission <span class="hlt">electron</span> microscopy, and energy dispersive x-ray spectroscopy. The stability of the mixed phases was investigated for substitutional and intercalation changes of basic B i2S e3 <span class="hlt">structure</span>. Four systems were compared: B i2S e3 , <span class="hlt">structures</span> obtaining by Cu intercalation of the van der Waals gap, by substitution of Bi by Cu in quintuple layers, and C u2Se . The <span class="hlt">structures</span> were identified and their <span class="hlt">electronic</span> properties were obtained. Transmission <span class="hlt">electron</span> microscopy measurements of B i2S e3 and the B i2S e3:Cu system identified the first <span class="hlt">structure</span> as uniform and the second as composite, consisting of a nonuniform lower-Cu-content matrix and randomly distributed high-Cu-concentration precipitates. Critical comparison of the ab initio and experimental data identified the matrix as having a B i2S e3 dominant part with randomly distributed Cu-intercalated regions having 1Cu-B i2S e3 <span class="hlt">structure</span>. The precipitates were determined to have 3Cu-B i2S e3 <span class="hlt">structure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22489725-sparse-mapsa-systematic-infrastructure-reduced-scaling-electronic-structure-methods-efficient-simple-linear-scaling-local-mp2-method-uses-intermediate-basis-pair-natural-orbitals','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22489725-sparse-mapsa-systematic-infrastructure-reduced-scaling-electronic-structure-methods-efficient-simple-linear-scaling-local-mp2-method-uses-intermediate-basis-pair-natural-orbitals"><span>Sparse maps—A systematic infrastructure for reduced-scaling <span class="hlt">electronic</span> <span class="hlt">structure</span> methods. I. An efficient and simple linear scaling <span class="hlt">local</span> MP2 method that uses an intermediate basis of pair natural orbitals</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>Pinski, Peter; Riplinger, Christoph; Neese, Frank, E-mail: evaleev@vt.edu, E-mail: frank.neese@cec.mpg.de</p> <p>2015-07-21</p> <p>In this work, a systematic infrastructure is described that formalizes concepts implicit in previous work and greatly simplifies computer implementation of reduced-scaling <span class="hlt">electronic</span> <span class="hlt">structure</span> methods. The key concept is sparse representation of tensors using chains of sparse maps between two index sets. Sparse map representation can be viewed as a generalization of compressed sparse row, a common representation of a sparse matrix, to tensor data. By combining few elementary operations on sparse maps (inversion, chaining, intersection, etc.), complex algorithms can be developed, illustrated here by a linear-scaling transformation of three-center Coulomb integrals based on our compact code library that implementsmore » sparse maps and operations on them. The sparsity of the three-center integrals arises from spatial <span class="hlt">locality</span> of the basis functions and domain density fitting approximation. A novel feature of our approach is the use of differential overlap integrals computed in linear-scaling fashion for screening products of basis functions. Finally, a robust linear scaling domain based <span class="hlt">local</span> pair natural orbital second-order Möller-Plesset (DLPNO-MP2) method is described based on the sparse map infrastructure that only depends on a minimal number of cutoff parameters that can be systematically tightened to approach 100% of the canonical MP2 correlation energy. With default truncation thresholds, DLPNO-MP2 recovers more than 99.9% of the canonical resolution of the identity MP2 (RI-MP2) energy while still showing a very early crossover with respect to the computational effort. Based on extensive benchmark calculations, relative energies are reproduced with an error of typically <0.2 kcal/mol. The efficiency of the <span class="hlt">local</span> MP2 (LMP2) method can be drastically improved by carrying out the LMP2 iterations in a basis of pair natural orbitals. While the present work focuses on <span class="hlt">local</span> <span class="hlt">electron</span> correlation, it is of much broader applicability to computation with sparse</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26203015','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26203015"><span>Sparse maps—A systematic infrastructure for reduced-scaling <span class="hlt">electronic</span> <span class="hlt">structure</span> methods. I. An efficient and simple linear scaling <span class="hlt">local</span> MP2 method that uses an intermediate basis of pair natural orbitals.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pinski, Peter; Riplinger, Christoph; Valeev, Edward F; Neese, Frank</p> <p>2015-07-21</p> <p>In this work, a systematic infrastructure is described that formalizes concepts implicit in previous work and greatly simplifies computer implementation of reduced-scaling <span class="hlt">electronic</span> <span class="hlt">structure</span> methods. The key concept is sparse representation of tensors using chains of sparse maps between two index sets. Sparse map representation can be viewed as a generalization of compressed sparse row, a common representation of a sparse matrix, to tensor data. By combining few elementary operations on sparse maps (inversion, chaining, intersection, etc.), complex algorithms can be developed, illustrated here by a linear-scaling transformation of three-center Coulomb integrals based on our compact code library that implements sparse maps and operations on them. The sparsity of the three-center integrals arises from spatial <span class="hlt">locality</span> of the basis functions and domain density fitting approximation. A novel feature of our approach is the use of differential overlap integrals computed in linear-scaling fashion for screening products of basis functions. Finally, a robust linear scaling domain based <span class="hlt">local</span> pair natural orbital second-order Möller-Plesset (DLPNO-MP2) method is described based on the sparse map infrastructure that only depends on a minimal number of cutoff parameters that can be systematically tightened to approach 100% of the canonical MP2 correlation energy. With default truncation thresholds, DLPNO-MP2 recovers more than 99.9% of the canonical resolution of the identity MP2 (RI-MP2) energy while still showing a very early crossover with respect to the computational effort. Based on extensive benchmark calculations, relative energies are reproduced with an error of typically <0.2 kcal/mol. The efficiency of the <span class="hlt">local</span> MP2 (LMP2) method can be drastically improved by carrying out the LMP2 iterations in a basis of pair natural orbitals. While the present work focuses on <span class="hlt">local</span> <span class="hlt">electron</span> correlation, it is of much broader applicability to computation with sparse tensors in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014Nanos...6.6458D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014Nanos...6.6458D"><span>Crystal <span class="hlt">structure</span> and <span class="hlt">electronic</span> properties of a thiolate-protected Au24 nanocluster</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Das, Anindita; Li, Tao; Li, Gao; Nobusada, Katsuyuki; Zeng, Chenjie; Rosi, Nathaniel L.; Jin, Rongchao</p> <p>2014-05-01</p> <p>Solving the total <span class="hlt">structures</span> of gold nanoclusters is of critical importance for understanding their <span class="hlt">electronic</span>, optical and catalytic properties. Herein, we report the X-ray <span class="hlt">structure</span> of a charge-neutral Au24(SCH2Ph-tBu)20 nanocluster. This <span class="hlt">structure</span> features a bi-tetrahedral Au8 kernel protected by four tetrameric staple-like motifs. <span class="hlt">Electronic</span> <span class="hlt">structure</span> analysis is further carried out and the optical absorption spectrum is interpreted. The Au24(SCH2Ph-tBu)20, Au23(S-c-C6H11)16 and Au25(SCH2CH2Ph)18 nanoclusters constitute the first crystallographically characterized ``trio''.Solving the total <span class="hlt">structures</span> of gold nanoclusters is of critical importance for understanding their <span class="hlt">electronic</span>, optical and catalytic properties. Herein, we report the X-ray <span class="hlt">structure</span> of a charge-neutral Au24(SCH2Ph-tBu)20 nanocluster. This <span class="hlt">structure</span> features a bi-tetrahedral Au8 kernel protected by four tetrameric staple-like motifs. <span class="hlt">Electronic</span> <span class="hlt">structure</span> analysis is further carried out and the optical absorption spectrum is interpreted. The Au24(SCH2Ph-tBu)20, Au23(S-c-C6H11)16 and Au25(SCH2CH2Ph)18 nanoclusters constitute the first crystallographically characterized ``trio''. <span class="hlt">Electronic</span> supplementary information (ESI) available: Experimental and supporting Fig. S1-S3. CCDC NUMBER(1000102). For ESI and crystallographic data in CIF or other <span class="hlt">electronic</span> format see DOI: 10.1039/c4nr01350f</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPSJ...87d1005H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPSJ...87d1005H"><span><span class="hlt">Structural</span> predictions for Correlated <span class="hlt">Electron</span> Materials Using the Functional Dynamical Mean Field Theory Approach</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haule, Kristjan</p> <p>2018-04-01</p> <p>The Dynamical Mean Field Theory (DMFT) in combination with the band <span class="hlt">structure</span> methods has been able to address reach physics of correlated materials, such as the fluctuating <span class="hlt">local</span> moments, spin and orbital fluctuations, atomic multiplet physics and band formation on equal footing. Recently it is getting increasingly recognized that more predictive ab-initio theory of correlated systems needs to also address the feedback effect of the correlated <span class="hlt">electronic</span> <span class="hlt">structure</span> on the ionic positions, as the metal-insulator transition is almost always accompanied with considerable <span class="hlt">structural</span> distortions. We will review recently developed extension of merger between the Density Functional Theory (DFT) and DMFT method, dubbed DFT+ embedded DMFT (DFT+eDMFT), whichsuccessfully addresses this challenge. It is based on the stationary Luttinger-Ward functional to minimize the numerical error, it subtracts the exact double-counting of DFT and DMFT, and implements self-consistent forces on all atoms in the unit cell. In a few examples, we will also show how the method elucidated the important feedback effect of correlations on crystal <span class="hlt">structure</span> in rare earth nickelates to explain the mechanism of the metal-insulator transition. The method showed that such feedback effect is also essential to understand the dynamic stability of the high-temperature body-centered cubic phase of elemental iron, and in particular it predicted strong enhancement of the <span class="hlt">electron</span>-phonon coupling over DFT values in FeSe, which was very recently verified by pioneering time-domain experiment.</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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