Sample records for ultra-high precision ccd

  1. Design Method For Ultra-High Resolution Linear CCD Imagers

    NASA Astrophysics Data System (ADS)

    Sheu, Larry S.; Truong, Thanh; Yuzuki, Larry; Elhatem, Abdul; Kadekodi, Narayan

    1984-11-01

    This paper presents the design method to achieve ultra-high resolution linear imagers. This method utilizes advanced design rules and novel staggered bilinear photo sensor arrays with quadrilinear shift registers. Design constraint in the detector arrays and shift registers are analyzed. Imager architecture to achieve ultra-high resolution is presented. The characteristics of MTF, aliasing, speed, transfer efficiency and fine photolithography requirements associated with this architecture are also discussed. A CCD imager with advanced 1.5 um minimum feature size was fabricated. It is intended as a test vehicle for the next generation small sampling pitch ultra-high resolution CCD imager. Standard double-poly, two-phase shift registers were fabricated at an 8 um pitch using the advanced design rules. A special process step that blocked the source-drain implant from the shift register area was invented. This guaranteed excellent performance of the shift registers regardless of the small poly overlaps. A charge transfer efficiency of better than 0.99995 and maximum transfer speed of 8 MHz were achieved. The imager showed excellent performance. The dark current was less than 0.2 mV/ms, saturation 250 mV, adjacent photoresponse non-uniformity ± 4% and responsivity 0.7 V/ μJ/cm2 for the 8 μm x 6 μm photosensor size. The MTF was 0.6 at 62.5 cycles/mm. These results confirm the feasibility of the next generation ultra-high resolution CCD imagers.

  2. Test of CCD Precision Limits for Differential Photometry

    NASA Technical Reports Server (NTRS)

    Borucki, W. J.; Dunham, E. W.; Wei, M. Z.; Robinson, L. B.; Ford, C. H.; Granados, A. F.

    1995-01-01

    Results of tests to demonstrate the very high differential-photometric stability of CCD light sensors are presented. The measurements reported here demonstrate that in a controlled laboratory environment, a front-illuminated CCD can provide differential-photometric measurements with reproducible precision approaching one part in 105. Practical limitations to the precision of differential-photometric measurements with CCDs and implications for spaceborne applications are discussed.

  3. Test of CCD Precision Limits for Differential Photometry

    NASA Technical Reports Server (NTRS)

    Robinson, L. B.; Wei, M. Z.; Borucki, W. J.; Dunham, E. W.; Ford, C. H.; Granados, A. F.

    1995-01-01

    Results of tests to demonstrate the very high differential-photometric stability of CCD light sensors are presented. The measurements reported here demonstrate that in a controlled laboratory environment, a front-illuminated CCD can provide differential-photometric measurements with reproducible precision approaching one part in 10(exp 5). Practical limitations to the precision of differential-photometric measurements with CCDs and implications for spaceborne applications are discussed.

  4. Precision optical slit for high heat load or ultra high vacuum

    DOEpatents

    Andresen, Nord C.; DiGennaro, Richard S.; Swain, Thomas L.

    1995-01-01

    This invention relates generally to slits used in optics that must be precisely aligned and adjusted. The optical slits of the present invention are useful in x-ray optics, x-ray beam lines, optical systems in which the entrance slit is critical for high wavelength resolution. The invention is particularly useful in ultra high vacuum systems where lubricants are difficult to use and designs which avoid the movement of metal parts against one another are important, such as monochrometers for high wavelength resolution with ultra high vacuum systems. The invention further relates to optical systems in which temperature characteristics of the slit materials is important. The present invention yet additionally relates to precision slits wherein the opposing edges of the slit must be precisely moved relative to a center line between the edges with each edge retaining its parallel orientation with respect to the other edge and/or the center line.

  5. Precision optical slit for high heat load or ultra high vacuum

    DOEpatents

    Andresen, N.C.; DiGennaro, R.S.; Swain, T.L.

    1995-01-24

    This invention relates generally to slits used in optics that must be precisely aligned and adjusted. The optical slits of the present invention are useful in x-ray optics, x-ray beam lines, optical systems in which the entrance slit is critical for high wavelength resolution. The invention is particularly useful in ultra high vacuum systems where lubricants are difficult to use and designs which avoid the movement of metal parts against one another are important, such as monochromators for high wavelength resolution with ultra high vacuum systems. The invention further relates to optical systems in which temperature characteristics of the slit materials is important. The present invention yet additionally relates to precision slits wherein the opposing edges of the slit must be precisely moved relative to a center line between the edges with each edge retaining its parallel orientation with respect to the other edge and/or the center line. 21 figures.

  6. Measurement precision and noise analysis of CCD cameras

    NASA Astrophysics Data System (ADS)

    Wu, ZhenSen; Li, Zhiyang; Zhang, Ping

    1993-09-01

    CHINA The lirait precision of CCD camera with 1O. bit analogue to digital conversion is estimated in this paper . The noise effect on ineasurenent precision and the noise characteristics are analyzed in details. The noise process means are also discussed and the diagram of noise properties is given in this paper.

  7. Review on the progress of ultra-precision machining technologies

    NASA Astrophysics Data System (ADS)

    Yuan, Julong; Lyu, Binghai; Hang, Wei; Deng, Qianfa

    2017-06-01

    Ultra-precision machining technologies are the essential methods, to obtain the highest form accuracy and surface quality. As more research findings are published, such technologies now involve complicated systems engineering and been widely used in the production of components in various aerospace, national defense, optics, mechanics, electronics, and other high-tech applications. The conception, applications and history of ultra-precision machining are introduced in this article, and the developments of ultra-precision machining technologies, especially ultra-precision grinding, ultra-precision cutting and polishing are also reviewed. The current state and problems of this field in China are analyzed. Finally, the development trends of this field and the coping strategies employed in China to keep up with the trends are discussed.

  8. High-Voltage Clock Driver for Photon-Counting CCD Characterization

    NASA Technical Reports Server (NTRS)

    Baker, Robert

    2013-01-01

    A document discusses the CCD97 from e2v technologies as it is being evaluated at Goddard Space Flight Center's Detector Characterization Laboratory (DCL) for possible use in ultra-low background noise space astronomy applications, such as Terrestrial Planet Finder Coronagraph (TPF-C). The CCD97 includes a photoncounting mode where the equivalent output noise is less than one electron. Use of this mode requires a clock signal at a voltage level greater than the level achievable by the existing CCD (charge-coupled-device) electronics. A high-voltage waveform generator has been developed in code 660/601 to support the CCD97 evaluation. The unit generates required clock waveforms at voltage levels from -20 to +50 V. It deals with standard and arbitrary waveforms and supports pixel rates from 50 to 500 kHz. The system is designed to interface with existing Leach CCD electronics.

  9. Precise CCD positions of Himalia using Gaia DR1 in 2015-2016

    NASA Astrophysics Data System (ADS)

    Peng, H. W.; Peng, Q. Y.; Wang, N.

    2017-05-01

    In order to obtain high-precision CCD positions of Himalia, the sixth Jovian satellite, a total of 598 CCD observations have been obtained during the years 2015-2016. The observations were made by using the 2.4 and 1 m telescopes administered by Yunnan Observatories over 27 nights. Several factors that would influence the positional precision of Himalia were analysed, including the reference star catalogue used, the geometric distortion and the phase effect. By taking advantage of its unprecedented positional precision, the recently released catalogue Gaia Data Release 1 was chosen to match reference stars in the CCD frames of both Himalia and open clusters, which were observed for deriving the geometric distortion. The latest version of sofa library was used to calculate the positions of reference stars. The theoretical positions of Himalia were retrieved from the Jet Propulsion Laboratory Horizons System that includes the satellite ephemeris JUP300, while the positions of Jupiter were based on the planetary ephemeris DE431. Our results showed that the means of observed minus computed (O - C) residuals are 0.071 and -0.001 arcsec in right ascension and declination, respectively. Their standard deviations are estimated at about 0.03 arcsec in each direction.

  10. Ultra precision machining

    NASA Astrophysics Data System (ADS)

    Debra, Daniel B.; Hesselink, Lambertus; Binford, Thomas

    1990-05-01

    There are a number of fields that require or can use to advantage very high precision in machining. For example, further development of high energy lasers and x ray astronomy depend critically on the manufacture of light weight reflecting metal optical components. To fabricate these optical components with machine tools they will be made of metal with mirror quality surface finish. By mirror quality surface finish, it is meant that the dimensions tolerances on the order of 0.02 microns and surface roughness of 0.07. These accuracy targets fall in the category of ultra precision machining. They cannot be achieved by a simple extension of conventional machining processes and techniques. They require single crystal diamond tools, special attention to vibration isolation, special isolation of machine metrology, and on line correction of imperfection in the motion of the machine carriages on their way.

  11. Is flat fielding safe for precision CCD astronomy?

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

    Baumer, Michael; Davis, Christopher P.; Roodman, Aaron

    The ambitious goals of precision cosmology with wide-field optical surveys such as the Dark Energy Survey (DES) and the Large Synoptic Survey Telescope (LSST) demand precision CCD astronomy as their foundation. This in turn requires an understanding of previously uncharacterized sources of systematic error in CCD sensors, many of which manifest themselves as static effective variations in pixel area. Such variation renders a critical assumption behind the traditional procedure of flat fielding—that a sensor's pixels comprise a uniform grid—invalid. In this work, we present a method to infer a curl-free model of a sensor's underlying pixel grid from flat-field images,more » incorporating the superposition of all electrostatic sensor effects—both known and unknown—present in flat-field data. We use these pixel grid models to estimate the overall impact of sensor systematics on photometry, astrometry, and PSF shape measurements in a representative sensor from the Dark Energy Camera (DECam) and a prototype LSST sensor. Applying the method to DECam data recovers known significant sensor effects for which corrections are currently being developed within DES. For an LSST prototype CCD with pixel-response non-uniformity (PRNU) of 0.4%, we find the impact of "improper" flat fielding on these observables is negligible in nominal .7'' seeing conditions. Furthermore, these errors scale linearly with the PRNU, so for future LSST production sensors, which may have larger PRNU, our method provides a way to assess whether pixel-level calibration beyond flat fielding will be required.« less

  12. Is flat fielding safe for precision CCD astronomy?

    DOE PAGES

    Baumer, Michael; Davis, Christopher P.; Roodman, Aaron

    2017-07-06

    The ambitious goals of precision cosmology with wide-field optical surveys such as the Dark Energy Survey (DES) and the Large Synoptic Survey Telescope (LSST) demand precision CCD astronomy as their foundation. This in turn requires an understanding of previously uncharacterized sources of systematic error in CCD sensors, many of which manifest themselves as static effective variations in pixel area. Such variation renders a critical assumption behind the traditional procedure of flat fielding—that a sensor's pixels comprise a uniform grid—invalid. In this work, we present a method to infer a curl-free model of a sensor's underlying pixel grid from flat-field images,more » incorporating the superposition of all electrostatic sensor effects—both known and unknown—present in flat-field data. We use these pixel grid models to estimate the overall impact of sensor systematics on photometry, astrometry, and PSF shape measurements in a representative sensor from the Dark Energy Camera (DECam) and a prototype LSST sensor. Applying the method to DECam data recovers known significant sensor effects for which corrections are currently being developed within DES. For an LSST prototype CCD with pixel-response non-uniformity (PRNU) of 0.4%, we find the impact of "improper" flat fielding on these observables is negligible in nominal .7'' seeing conditions. Furthermore, these errors scale linearly with the PRNU, so for future LSST production sensors, which may have larger PRNU, our method provides a way to assess whether pixel-level calibration beyond flat fielding will be required.« less

  13. Aspects of ultra-high-precision diamond machining of RSA 443 optical aluminium

    NASA Astrophysics Data System (ADS)

    Mkoko, Z.; Abou-El-Hossein, K.

    2015-08-01

    Optical aluminium alloys such as 6061-T6 are traditionally used in ultra-high precision manufacturing for making optical mirrors for aerospace and other applications. However, the optics industry has recently witnessed the development of more advanced optical aluminium grades that are capable of addressing some of the issues encountered when turning with single-point natural monocrystalline diamond cutters. The advent of rapidly solidified aluminium (RSA) grades has generally opened up new possibilities for ultra-high precision manufacturing of optical components. In this study, experiments were conducted with single-point diamond cutters on rapidly solidified aluminium RSA 443 material. The objective of this study is to observe the effects of depth of cut and feed rate at a fixed rotational speed on the tool wear rate and resulting surface roughness of diamond turned specimens. This is done to gain further understanding of the rate of wear on the diamond cutters versus the surface texture generated on the RSA 443 material. The diamond machining experiments yielded machined surfaces which are less reflective but with consistent surface roughness values. Cutting tools were observed for wear through scanning microscopy; relatively low wear pattern was evident on the diamond tool edge. The highest tool wear were obtained at higher depth of cut and increased feed rate.

  14. CHEOPS: a space telescope for ultra-high precision photometry of exoplanet transits

    NASA Astrophysics Data System (ADS)

    Cessa, V.; Beck, T.; Benz, W.; Broeg, C.; Ehrenreich, D.; Fortier, A.; Peter, G.; Magrin, D.; Pagano, I.; Plesseria, J.-Y.; Steller, M.; Szoke, J.; Thomas, N.; Ragazzoni, R.; Wildi, F.

    2017-11-01

    The CHaracterising ExOPlanet Satellite (CHEOPS) is a joint ESA-Switzerland space mission dedicated to search for exoplanet transits by means of ultra-high precision photometry whose launch readiness is expected end 2017. The CHEOPS instrument will be the first space telescope dedicated to search for transits on bright stars already known to host planets. By being able to point at nearly any location on the sky, it will provide the unique capability of determining accurate radii for a subset of those planets for which the mass has already been estimated from ground-based spectroscopic surveys. CHEOPS will also provide precision radii for new planets discovered by the next generation ground-based transits surveys (Neptune-size and smaller). The main science goals of the CHEOPS mission will be to study the structure of exoplanets with radii typically ranging from 1 to 6 Earth radii orbiting bright stars. With an accurate knowledge of masses and radii for an unprecedented sample of planets, CHEOPS will set new constraints on the structure and hence on the formation and evolution of planets in this mass range. To reach its goals CHEOPS will measure photometric signals with a precision of 20 ppm in 6 hours of integration time for a 9th magnitude star. This corresponds to a signal to noise of 5 for a transit of an Earth-sized planet orbiting a solar-sized star (0.9 solar radii). This precision will be achieved by using a single frame-transfer backside illuminated CCD detector cool down at 233K and stabilized within {10 mK . The CHEOPS optical design is based on a Ritchey-Chretien style telescope with 300 mm effective aperture diameter, which provides a defocussed image of the target star while minimizing straylight using a dedicated field stop and baffle system. As CHEOPS will be in a LEO orbit, straylight suppression is a key point to allow the observation of faint stars. The telescope will be the only payload on a spacecraft platform providing pointing stability of < 8

  15. Precise CCD positions of Phoebe in 2011-2014

    NASA Astrophysics Data System (ADS)

    Peng, Q. Y.; Wang, N.; Vienne, A.; Zhang, Q. F.; Li, Z.; Meng, X. H.

    2015-05-01

    346 new CCD observations during the years 2011-2014 have been reduced to derive the precise positions of Phoebe, the ninth satellite of Saturn. The observations were made by the 2.4 m telescope at Yunnan Observatory over nine nights. Due to the use of a focal-reducer on the telescope, its significant geometric distortion is solved for and removed for each CCD field of view. The positions of Phoebe are measured with respect to the stars in UCAC2 catalogue. The theoretical position of Phoebe was retrieved from the Institute de Méchanique Céleste et de Calcul des Éphémérides ephemeris which includes the latest theory PH12 by Desmars et al., while the position of Saturn was obtained from the Jet Propulsion Laboratory ephemeris DE431. Our results show that the mean O-Cs (observed minus computed) are -0.02 and -0.07 arcsec in right ascension and declination, respectively. The dispersions of our observations are estimated at about 0.04 arcsec in each direction.

  16. Air Bearings Machined On Ultra Precision, Hydrostatic CNC-Lathe

    NASA Astrophysics Data System (ADS)

    Knol, Pierre H.; Szepesi, Denis; Deurwaarder, Jan M.

    1987-01-01

    Micromachining of precision elements requires an adequate machine concept to meet the high demand of surface finish, dimensional and shape accuracy. The Hembrug ultra precision lathes have been exclusively designed with hydrostatic principles for main spindle and guideways. This concept is to be explained with some major advantages of hydrostatics compared with aerostatics at universal micromachining applications. Hembrug has originally developed the conventional Mikroturn ultra precision facing lathes, for diamond turning of computer memory discs. This first generation of machines was followed by the advanced computer numerically controlled types for machining of complex precision workpieces. One of these parts, an aerostatic bearing component has been succesfully machined on the Super-Mikroturn CNC. A case study of airbearing machining confirms the statement that a good result of the micromachining does not depend on machine performance alone, but also on the technology applied.

  17. Mechanism and experimental research on ultra-precision grinding of ferrite

    NASA Astrophysics Data System (ADS)

    Ban, Xinxing; Zhao, Huiying; Dong, Longchao; Zhu, Xueliang; Zhang, Chupeng; Gu, Yawen

    2017-02-01

    Ultra-precision grinding of ferrite is conducted to investigate the removal mechanism. Effect of the accuracy of machine tool key components on grinding surface quality is analyzed. The surface generation model of ferrite ultra-precision grinding machining is established. In order to reveal the surface formation mechanism of ferrite in the process of ultraprecision grinding, furthermore, the scientific and accurate of the calculation model are taken into account to verify the grinding surface roughness, which is proposed. Orthogonal experiment is designed using the high precision aerostatic turntable and aerostatic spindle for ferrite which is a typical hard brittle materials. Based on the experimental results, the influence factors and laws of ultra-precision grinding surface of ferrite are discussed through the analysis of the surface roughness. The results show that the quality of ferrite grinding surface is the optimal parameters, when the wheel speed of 20000r/mm, feed rate of 10mm/min, grinding depth of 0.005mm, and turntable rotary speed of 5r/min, the surface roughness Ra can up to 75nm.

  18. High-resolution CCD imaging alternatives

    NASA Astrophysics Data System (ADS)

    Brown, D. L.; Acker, D. E.

    1992-08-01

    High resolution CCD color cameras have recently stimulated the interest of a large number of potential end-users for a wide range of practical applications. Real-time High Definition Television (HDTV) systems are now being used or considered for use in applications ranging from entertainment program origination through digital image storage to medical and scientific research. HDTV generation of electronic images offers significant cost and time-saving advantages over the use of film in such applications. Further in still image systems electronic image capture is faster and more efficient than conventional image scanners. The CCD still camera can capture 3-dimensional objects into the computing environment directly without having to shoot a picture on film develop it and then scan the image into a computer. 2. EXTENDING CCD TECHNOLOGY BEYOND BROADCAST Most standard production CCD sensor chips are made for broadcast-compatible systems. One popular CCD and the basis for this discussion offers arrays of roughly 750 x 580 picture elements (pixels) or a total array of approximately 435 pixels (see Fig. 1). FOR. A has developed a technique to increase the number of available pixels for a given image compared to that produced by the standard CCD itself. Using an inter-lined CCD with an overall spatial structure several times larger than the photo-sensitive sensor areas each of the CCD sensors is shifted in two dimensions in order to fill in spatial gaps between adjacent sensors.

  19. Linear CCD attitude measurement system based on the identification of the auxiliary array CCD

    NASA Astrophysics Data System (ADS)

    Hu, Yinghui; Yuan, Feng; Li, Kai; Wang, Yan

    2015-10-01

    Object to the high precision flying target attitude measurement issues of a large space and large field of view, comparing existing measurement methods, the idea is proposed of using two array CCD to assist in identifying the three linear CCD with multi-cooperative target attitude measurement system, and to address the existing nonlinear system errors and calibration parameters and more problems with nine linear CCD spectroscopic test system of too complicated constraints among camera position caused by excessive. The mathematical model of binocular vision and three linear CCD test system are established, co-spot composition triangle utilize three red LED position light, three points' coordinates are given in advance by Cooperate Measuring Machine, the red LED in the composition of the three sides of a triangle adds three blue LED light points as an auxiliary, so that array CCD is easier to identify three red LED light points, and linear CCD camera is installed of a red filter to filter out the blue LED light points while reducing stray light. Using array CCD to measure the spot, identifying and calculating the spatial coordinates solutions of red LED light points, while utilizing linear CCD to measure three red LED spot for solving linear CCD test system, which can be drawn from 27 solution. Measured with array CCD coordinates auxiliary linear CCD has achieved spot identification, and has solved the difficult problems of multi-objective linear CCD identification. Unique combination of linear CCD imaging features, linear CCD special cylindrical lens system is developed using telecentric optical design, the energy center of the spot position in the depth range of convergence in the direction is perpendicular to the optical axis of the small changes ensuring highprecision image quality, and the entire test system improves spatial object attitude measurement speed and precision.

  20. A high-speed pnCCD detector system for optical applications

    NASA Astrophysics Data System (ADS)

    Hartmann, R.; Buttler, W.; Gorke, H.; Herrmann, S.; Holl, P.; Meidinger, N.; Soltau, H.; Strüder, L.

    2006-11-01

    Measurements of a frame-store pnCCD detector system, optimized for high-speed applications in the optical and near infrared (NIR) region, will be presented. The device with an image area of 13.5 mm by 13.5 mm and a pixelsize of 51 μm by 51 μm exhibits a readout time faster than 1100 frames per second with an overall electronic noise contribution of less than three electrons. Variable operation modes of the detector system allow for even higher readout speeds by a pixel binning in transfer direction or, at slightly slower readout speeds, a further improvement in noise performance. We will also present the concept of a data acquisition system being able to handle pixel rates of more than 75 megapixel per second. The application of an anti-reflective coating on the ultra-thin entrance window of the back illuminated detector together with the large sensitive volume ensures a high and uniform detection efficiency from the ultra violet to the NIR.

  1. Ultra-High Precision Half-Life Measurement for the Superallowed &+circ; Emitter ^26Al^m

    NASA Astrophysics Data System (ADS)

    Finlay, P.; Demand, G.; Garrett, P. E.; Leach, K. G.; Phillips, A. A.; Sumithrarachchi, C. S.; Svensson, C. E.; Triambak, S.; Grinyer, G. F.; Leslie, J. R.; Andreoiu, C.; Cross, D.; Austin, R. A. E.; Ball, G. C.; Bandyopadhyay, D.; Djongolov, M.; Ettenauer, S.; Hackman, G.; Pearson, C. J.; Williams, S. J.

    2009-10-01

    The calculated nuclear structure dependent correction for ^26Al^m (δC-δNS= 0.305(27)% [1]) is smaller by nearly a factor of two than the other twelve precision superallowed cases, making it an ideal case to pursue a reduction in the experimental errors contributing to the Ft value. An ultra-high precision half-life measurement for the superallowed &+circ; emitter ^26Al^m has been made at the Isotope Separator and Accelerator (ISAC) facility at TRIUMF in Vancouver, Canada. A beam of ˜10^5 ^26Al^m/s was delivered in October 2007 and its decay was observed using a 4π continuous gas flow proportional counter as part of an ongoing experimental program in superallowed Fermi β decay studies. With a statistical precision of ˜0.008%, the present work represents the single most precise measurement of any superallowed half-life to date. [4pt] [1] I.S. Towner and J.C. Hardy, Phys. Rev. C 79, 055502 (2009).

  2. Ultra-High Precision Half-Life Measurement for the Superallowed &+circ; Emitter ^26Al^m

    NASA Astrophysics Data System (ADS)

    Finlay, P.; Demand, G.; Garrett, P. E.; Leach, K. G.; Phillips, A. A.; Sumithrarachchi, C. S.; Svensson, C. E.; Triambak, S.; Ball, G. C.; Bandyopadhyay, D.; Djongolov, M.; Ettenauer, S.; Hackman, G.; Pearson, C. J.; Williams, S. J.; Andreoiu, C.; Cross, D.; Austin, R. A. E.; Grinyer, G. F.; Leslie, J. R.

    2008-10-01

    The calculated nuclear structure dependent correction for ^26Al^m (δC-δNS= 0.305(27)% [1]) is smaller by nearly a factor of two than the other twelve precision superallowed cases, making it an ideal case to pursue a reduction in the experimental errors contributing to the Ft value. An ultra-high precision half-life measurement for the superallowed &+circ; emitter ^26Al^m has been made using a 4π continuous gas flow proportional counter as part of an ongoing experimental program in superallowed Fermi β decay studies at the Isotope Separator and Accelerator (ISAC) facility at TRIUMF in Vancouver, Canada, which delivered a beam of ˜10^5 ^26Al^m/s in October 2007. With a statistical precision of ˜0.008%, the present work represents the single most precise measurement of any superallowed half-life to date. [1] I.S. Towner and J.C. Hardy, Phys. Rev. C 77, 025501 (2008).

  3. Development of ultra-precision micro-cavity measurement technique in HIT-UOI

    NASA Astrophysics Data System (ADS)

    Cui, Jiwen; Li, Lei; Tan, Jiubin

    2010-08-01

    Micro cavities with high aspect ratio are widely used in different fields including aerospace and defense industries with the development of manufacturing technology. So how to measure the dimension of these cavities has become one of the major research subjects in the field of measurement and instrument. This paper describes some activities of the precision micro cavity measurement technique in Center of Ultra-precision Optoelectronic Instrument (UOI), Harbin Institute of Technology (HIT). The key issue of micro cavity measurement in UOI is called touch-trigger measurement method. The first scheme is double optical fiber coupling, in which light coming from the incident optical fiber is transmitted in the reversal direction via the optical fiber coupling into the effluent optical fiber, the lateral displacement of the touch-trigger sensor is transformed into the deflexion of light coming out from the effluent optical fiber, and the deflexion is transformed into an image signal by the object lens and CCD capturing system. And the second scheme is micro focal-length collimation, in which a fiber stem with a ball mounted on its end is used as a probe and a small segment of it is used as a cylindrical lens to collimate a point light source and image it to a camera, the deflection of the fiber stem can be inferred from the change in image acquired by the camera with ultrahigh displacement sensitivity. Experiments for these activities will be given with a focus on the measurement results and repeatability uncertainty.

  4. Manufacture of ultra high precision aerostatic bearings based on glass guide

    NASA Astrophysics Data System (ADS)

    Guo, Meng; Dai, Yifan; Peng, Xiaoqiang; Tie, Guipeng; Lai, Tao

    2017-10-01

    The aerostatic guide in the traditional three-coordinate measuring machine and profilometer generally use metal or ceramics material. Limited by the guide processing precision, the measurement accuracy of these traditional instruments is around micro-meter level. By selection of optical materials as guide material, optical processing method and laser interference measurement can be introduced to the traditional aerostatic bearings manufacturing field. By using the large aperture wave-front interference measuring equipment , the shape and position error of the glass guide can be obtained in high accuracy and then it can be processed to 0.1μm or even better with the aid of Magnetorheological Finishing(MRF) and Computer Controlled Optical Surfacing (CCOS) process and other modern optical processing method, so the accuracy of aerostatic bearings can be fundamentally improved and ultra high precision coordinate measuring can be achieved. This paper introduces the fabrication and measurement process of the glass guide by K9 with 300mm measuring range, and its working surface accuracy is up to 0.1μm PV, the verticality and parallelism error between the two guide rail face is better than 2μm, and the straightness of the aerostatic bearings by this K9 glass guide is up to 40nm after error compensation.

  5. Ultra-precision process of CaF2 single crystal

    NASA Astrophysics Data System (ADS)

    Yin, Guoju; Li, Shengyi; Xie, Xuhui; Zhou, Lin

    2014-08-01

    This paper proposes a new chemical mechanical polishing (CMP) process method for CaF2 single crystal to get ultraprecision surface. The CMP processes are improving polishing pad and using alkaline SiO2 polishing slurry with PH=8, PH=11 two phases to polish, respectively, and the roughness can be 0.181nm Rq (10μm×10μm). The CMP process can't get high surface figure, so we use ion beam figuring (IBF) technology to obtain high surface figure. However, IBF is difficult to improve the CaF2 surface roughness. We optimize IBF process to improve surface figure and keep good surface roughness too. Different IBF incident ion energy from 400ev to 800ev does not affect on the surface roughness obviously but the depth of material removal is reverse. CaF2 single crystal can get high precision surface figure (RMS=2.251nm) and still keep ultra-smooth surface (Rq=0.207nm) by IBF when removal depth is less than 200nm. The researches above provide important information for CaF2 single crystal to realize ultra-precision manufacture.

  6. Ultra-Light Precision Membrane Optics

    NASA Technical Reports Server (NTRS)

    Moore, Jim; Gunter, Kent; Patrick, Brian; Marty, Dave; Bates, Kevin; Gatlin, Romona; Clayton, Bill; Rood, Bob; Brantley, Whitt (Technical Monitor)

    2001-01-01

    SRS Technologies and NASA Marshall Space Flight Center have conducted a research effort to explore the possibility of developing ultra-lightweight membrane optics for future imaging applications. High precision optical flats and spherical mirrors were produced under this research effort. The thin film mirrors were manufactured using surface replication casting of CPI(Trademark), a polyimide material developed specifically for UV hardness and thermal stability. In the course of this program, numerous polyimide films were cast with surface finishes better than 1.5 nanometers rms and thickness variation of less than 63 nanometers. Precision membrane optical flats were manufactured demonstrating better than 1/13 wave figure error when measured at 633 nanometers. The aerial density of these films is 0.037 kilograms per square meter. Several 0.5-meter spherical mirrors were also manufactured. These mirrors had excellent surface finish (1.5 nanometers rms) and figure error on the order of tens of microns. This places their figure error within the demonstrated correctability of advanced wavefront correction technologies such as real time holography.

  7. French Meteor Network for High Precision Orbits of Meteoroids

    NASA Technical Reports Server (NTRS)

    Atreya, P.; Vaubaillon, J.; Colas, F.; Bouley, S.; Gaillard, B.; Sauli, I.; Kwon, M. K.

    2011-01-01

    There is a lack of precise meteoroids orbit from video observations as most of the meteor stations use off-the-shelf CCD cameras. Few meteoroids orbit with precise semi-major axis are available using film photographic method. Precise orbits are necessary to compute the dust flux in the Earth s vicinity, and to estimate the ejection time of the meteoroids accurately by comparing them with the theoretical evolution model. We investigate the use of large CCD sensors to observe multi-station meteors and to compute precise orbit of these meteoroids. An ideal spatial and temporal resolution to get an accuracy to those similar of photographic plates are discussed. Various problems faced due to the use of large CCD, such as increasing the spatial and the temporal resolution at the same time and computational problems in finding the meteor position are illustrated.

  8. CCD centroiding analysis for Nano-JASMINE observation data

    NASA Astrophysics Data System (ADS)

    Niwa, Yoshito; Yano, Taihei; Araki, Hiroshi; Gouda, Naoteru; Kobayashi, Yukiyasu; Yamada, Yoshiyuki; Tazawa, Seiichi; Hanada, Hideo

    2010-07-01

    Nano-JASMINE is a very small satellite mission for global space astrometry with milli-arcsecond accuracy, which will be launched in 2011. In this mission, centroids of stars in CCD image frames are estimated with sub-pixel accuracy. In order to realize such a high precision centroiding an algorithm utilizing a least square method is employed. One of the advantages is that centroids can be calculated without explicit assumption of the point spread functions of stars. CCD centroiding experiment has been performed to investigate whether this data analysis is available, and centroids of artificial star images on a CCD are determined with a precision of less than 0.001 pixel. This result indicates parallaxes of stars within 300 pc from Sun can be observed in Nano-JASMINE.

  9. Curved CCD detector devices and arrays for multispectral astrophysical applications and terrestrial stereo panoramic cameras

    NASA Astrophysics Data System (ADS)

    Swain, Pradyumna; Mark, David

    2004-09-01

    The emergence of curved CCD detectors as individual devices or as contoured mosaics assembled to match the curved focal planes of astronomical telescopes and terrestrial stereo panoramic cameras represents a major optical design advancement that greatly enhances the scientific potential of such instruments. In altering the primary detection surface within the telescope"s optical instrumentation system from flat to curved, and conforming the applied CCD"s shape precisely to the contour of the telescope"s curved focal plane, a major increase in the amount of transmittable light at various wavelengths through the system is achieved. This in turn enables multi-spectral ultra-sensitive imaging with much greater spatial resolution necessary for large and very large telescope applications, including those involving infrared image acquisition and spectroscopy, conducted over very wide fields of view. For earth-based and space-borne optical telescopes, the advent of curved CCD"s as the principle detectors provides a simplification of the telescope"s adjoining optics, reducing the number of optical elements and the occurrence of optical aberrations associated with large corrective optics used to conform to flat detectors. New astronomical experiments may be devised in the presence of curved CCD applications, in conjunction with large format cameras and curved mosaics, including three dimensional imaging spectroscopy conducted over multiple wavelengths simultaneously, wide field real-time stereoscopic tracking of remote objects within the solar system at high resolution, and deep field survey mapping of distant objects such as galaxies with much greater multi-band spatial precision over larger sky regions. Terrestrial stereo panoramic cameras equipped with arrays of curved CCD"s joined with associative wide field optics will require less optical glass and no mechanically moving parts to maintain continuous proper stereo convergence over wider perspective viewing fields than

  10. Jig Aligns Shadow Mask On CCD

    NASA Technical Reports Server (NTRS)

    Matus, Carlos V.

    1989-01-01

    Alignment viewed through microscope. Alignment jig positions shadow mask on charge-coupled device (CCD) so metal film deposited on it precisely. Allows CCD package to be inserted and removed without disturbing alignment of mask. Holds CCD packages securely and isolates it electrostatically while providing electrical contact to each of its pins. When alignment jig assembled with CCD, used to move mask under micrometer control.

  11. High-frame rate multiport CCD imager and camera

    NASA Astrophysics Data System (ADS)

    Levine, Peter A.; Patterson, David R.; Esposito, Benjamin J.; Tower, John R.; Lawler, William B.

    1993-01-01

    A high frame rate visible CCD camera capable of operation up to 200 frames per second is described. The camera produces a 256 X 256 pixel image by using one quadrant of a 512 X 512 16-port, back illuminated CCD imager. Four contiguous outputs are digitally reformatted into a correct, 256 X 256 image. This paper details the architecture and timing used for the CCD drive circuits, analog processing, and the digital reformatter.

  12. Ultra-narrow pulse generator with precision-adjustable pulse width

    NASA Astrophysics Data System (ADS)

    Fu, Zaiming; Liu, Hanglin

    2018-05-01

    In this paper, a novel ultra-narrow pulse generation approach is proposed. It is based on the decomposition and synthesis of pulse edges. Through controlling their relative delay, an ultra-narrow pulse could be generated. By employing field programmable gate array digital synthesis technology, the implemented pulse generator is with programmable ability. The amplitude of pulse signals is controlled by the radio frequency amplifiers and bias tees, and high precision can be achieved. More importantly, the proposed approach can break through the limitation of device's propagation delay and optimize the resolution and the accuracy of the pulse width significantly. The implemented pulse generator has two channels, whose minimum pulse width, frequency range, and amplitude range are 100 ps, 15 MHz-1.5 GHz, and 0.1 Vpp-1.8 Vpp, respectively. Both resolution of pulse width and channel delay are 1 ps, and amplitude resolution is 10 mVpp.

  13. An ultra-stable voltage source for precision Penning-trap experiments

    NASA Astrophysics Data System (ADS)

    Böhm, Ch.; Sturm, S.; Rischka, A.; Dörr, A.; Eliseev, S.; Goncharov, M.; Höcker, M.; Ketter, J.; Köhler, F.; Marschall, D.; Martin, J.; Obieglo, D.; Repp, J.; Roux, C.; Schüssler, R. X.; Steigleder, M.; Streubel, S.; Wagner, Th.; Westermann, J.; Wieder, V.; Zirpel, R.; Melcher, J.; Blaum, K.

    2016-08-01

    An ultra-stable and low-noise 25-channel voltage source providing 0 to -100 V has been developed. It will supply stable bias potentials for Penning-trap electrodes used in high-precision experiments. The voltage source generates all its supply voltages via a specially designed transformer. Each channel can be operated either in a precision mode or can be dynamically ramped. A reference module provides reference voltages for all the channels, each of which includes a low-noise amplifier to gain a factor of 10 in the output stage. A relative voltage stability of δV / V ≈ 2 ×10-8 has been demonstrated at -89 V within about 10 min.

  14. High-precision Non-Contact Measurement of Creep of Ultra-High Temperature Materials for Aerospace

    NASA Technical Reports Server (NTRS)

    Rogers, Jan R.; Hyers, Robert

    2008-01-01

    For high-temperature applications (greater than 2,000 C) such as solid rocket motors, hypersonic aircraft, nuclear electric/thermal propulsion for spacecraft, and more efficient jet engines, creep becomes one of the most important design factors to be considered. Conventional creep-testing methods, where the specimen and test apparatus are in contact with each other, are limited to temperatures approximately 1,700 C. Development of alloys for higher-temperature applications is limited by the availability of testing methods at temperatures above 2000 C. Development of alloys for applications requiring a long service life at temperatures as low as 1500 C, such as the next generation of jet turbine superalloys, is limited by the difficulty of accelerated testing at temperatures above 1700 C. For these reasons, a new, non-contact creep-measurement technique is needed for higher temperature applications. A new non-contact method for creep measurements of ultra-high-temperature metals and ceramics has been developed and validated. Using the electrostatic levitation (ESL) facility at NASA Marshall Space Flight Center, a spherical sample is rotated quickly enough to cause creep deformation due to centrifugal acceleration. Very accurate measurement of the deformed shape through digital image analysis allows the stress exponent n to be determined very precisely from a single test, rather than from numerous conventional tests. Validation tests on single-crystal niobium spheres showed excellent agreement with conventional tests at 1985 C; however the non-contact method provides much greater precision while using only about 40 milligrams of material. This method is being applied to materials including metals and ceramics for non-eroding throats in solid rockets and next-generation superalloys for turbine engines. Recent advances in the method and the current state of these new measurements will be presented.

  15. Note: High precision measurements using high frequency gigahertz signals

    NASA Astrophysics Data System (ADS)

    Jin, Aohan; Fu, Siyuan; Sakurai, Atsunori; Liu, Liang; Edman, Fredrik; Pullerits, Tõnu; Öwall, Viktor; Karki, Khadga Jung

    2014-12-01

    Generalized lock-in amplifiers use digital cavities with Q-factors as high as 5 × 108 to measure signals with very high precision. In this Note, we show that generalized lock-in amplifiers can be used to analyze microwave (giga-hertz) signals with a precision of few tens of hertz. We propose that the physical changes in the medium of propagation can be measured precisely by the ultra-high precision measurement of the signal. We provide evidence to our proposition by verifying the Newton's law of cooling by measuring the effect of change in temperature on the phase and amplitude of the signals propagating through two calibrated cables. The technique could be used to precisely measure different physical properties of the propagation medium, for example, the change in length, resistance, etc. Real time implementation of the technique can open up new methodologies of in situ virtual metrology in material design.

  16. Research on precision grinding technology of large scale and ultra thin optics

    NASA Astrophysics Data System (ADS)

    Zhou, Lian; Wei, Qiancai; Li, Jie; Chen, Xianhua; Zhang, Qinghua

    2018-03-01

    The flatness and parallelism error of large scale and ultra thin optics have an important influence on the subsequent polishing efficiency and accuracy. In order to realize the high precision grinding of those ductile elements, the low deformation vacuum chuck was designed first, which was used for clamping the optics with high supporting rigidity in the full aperture. Then the optics was planar grinded under vacuum adsorption. After machining, the vacuum system was turned off. The form error of optics was on-machine measured using displacement sensor after elastic restitution. The flatness would be convergenced with high accuracy by compensation machining, whose trajectories were integrated with the measurement result. For purpose of getting high parallelism, the optics was turned over and compensation grinded using the form error of vacuum chuck. Finally, the grinding experiment of large scale and ultra thin fused silica optics with aperture of 430mm×430mm×10mm was performed. The best P-V flatness of optics was below 3 μm, and parallelism was below 3 ″. This machining technique has applied in batch grinding of large scale and ultra thin optics.

  17. Deep-UV-sensitive high-frame-rate backside-illuminated CCD camera developments

    NASA Astrophysics Data System (ADS)

    Dawson, Robin M.; Andreas, Robert; Andrews, James T.; Bhaskaran, Mahalingham; Farkas, Robert; Furst, David; Gershstein, Sergey; Grygon, Mark S.; Levine, Peter A.; Meray, Grazyna M.; O'Neal, Michael; Perna, Steve N.; Proefrock, Donald; Reale, Michael; Soydan, Ramazan; Sudol, Thomas M.; Swain, Pradyumna K.; Tower, John R.; Zanzucchi, Pete

    2002-04-01

    New applications for ultra-violet imaging are emerging in the fields of drug discovery and industrial inspection. High throughput is critical for these applications where millions of drug combinations are analyzed in secondary screenings or high rate inspection of small feature sizes over large areas is required. Sarnoff demonstrated in1990 a back illuminated, 1024 X 1024, 18 um pixel, split-frame-transfer device running at > 150 frames per second with high sensitivity in the visible spectrum. Sarnoff designed, fabricated and delivered cameras based on these CCDs and is now extending this technology to devices with higher pixel counts and higher frame rates through CCD architectural enhancements. The high sensitivities obtained in the visible spectrum are being pushed into the deep UV to support these new medical and industrial inspection applications. Sarnoff has achieved measured quantum efficiencies > 55% at 193 nm, rising to 65% at 300 nm, and remaining almost constant out to 750 nm. Optimization of the sensitivity is being pursued to tailor the quantum efficiency for particular wavelengths. Characteristics of these high frame rate CCDs and cameras will be described and results will be presented demonstrating high UV sensitivity down to 150 nm.

  18. High precision detector robot arm system

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

    Shu, Deming; Chu, Yong

    A method and high precision robot arm system are provided, for example, for X-ray nanodiffraction with an X-ray nanoprobe. The robot arm system includes duo-vertical-stages and a kinematic linkage system. A two-dimensional (2D) vertical plane ultra-precision robot arm supporting an X-ray detector provides positioning and manipulating of the X-ray detector. A vertical support for the 2D vertical plane robot arm includes spaced apart rails respectively engaging a first bearing structure and a second bearing structure carried by the 2D vertical plane robot arm.

  19. Driving techniques for high frame rate CCD camera

    NASA Astrophysics Data System (ADS)

    Guo, Weiqiang; Jin, Longxu; Xiong, Jingwu

    2008-03-01

    This paper describes a high-frame rate CCD camera capable of operating at 100 frames/s. This camera utilizes Kodak KAI-0340, an interline transfer CCD with 640(vertical)×480(horizontal) pixels. Two output ports are used to read out CCD data and pixel rates approaching 30 MHz. Because of its reduced effective opacity of vertical charge transfer registers, interline transfer CCD can cause undesired image artifacts, such as random white spots and smear generated in the registers. To increase frame rate, a kind of speed-up structure has been incorporated inside KAI-0340, then it is vulnerable to a vertical stripe effect. The phenomena which mentioned above may severely impair the image quality. To solve these problems, some electronic methods of eliminating these artifacts are adopted. Special clocking mode can dump the unwanted charge quickly, then the fast readout of the images, cleared of smear, follows immediately. Amplifier is used to sense and correct delay mismatch between the dual phase vertical clock pulses, the transition edges become close to coincident, so vertical stripes disappear. Results obtained with the CCD camera are shown.

  20. Full-band error control and crack-free surface fabrication techniques for ultra-precision fly cutting of large-aperture KDP crystals

    NASA Astrophysics Data System (ADS)

    Zhang, F. H.; Wang, S. F.; An, C. H.; Wang, J.; Xu, Q.

    2017-06-01

    Large-aperture potassium dihydrogen phosphate (KDP) crystals are widely used in the laser path of inertial confinement fusion (ICF) systems. The most common method of manufacturing half-meter KDP crystals is ultra-precision fly cutting. When processing KDP crystals by ultra-precision fly cutting, the dynamic characteristics of the fly cutting machine and fluctuations in the fly cutting environment are translated into surface errors at different spatial frequency bands. These machining errors should be suppressed effectively to guarantee that KDP crystals meet the full-band machining accuracy specified in the evaluation index. In this study, the anisotropic machinability of KDP crystals and the causes of typical surface errors in ultra-precision fly cutting of the material are investigated. The structures of the fly cutting machine and existing processing parameters are optimized to improve the machined surface quality. The findings are theoretically and practically important in the development of high-energy laser systems in China.

  1. Quantum efficiency measurement of the Transiting Exoplanet Survey Satellite (TESS) CCD detectors

    NASA Astrophysics Data System (ADS)

    Krishnamurthy, A.; Villasenor, J.; Thayer, C.; Kissel, S.; Ricker, G.; Seager, S.; Lyle, R.; Deline, A.; Morgan, E.; Sauerwein, T.; Vanderspek, R.

    2016-07-01

    Very precise on-ground characterization and calibration of TESS CCD detectors will significantly assist in the analysis of the science data from the mission. An accurate optical test bench with very high photometric stability has been developed to perform precise measurements of the absolute quantum efficiency. The setup consists of a vacuum dewar with a single MIT Lincoln Lab CCID-80 device mounted on a cold plate with the calibrated reference photodiode mounted next to the CCD. A very stable laser-driven light source is integrated with a closed-loop intensity stabilization unit to control variations of the light source down to a few parts-per-million when averaged over 60 s. Light from the stabilization unit enters a 20 inch integrating sphere. The output light from the sphere produces near-uniform illumination on the cold CCD and on the calibrated reference photodiode inside the dewar. The ratio of the CCD and photodiode signals provides the absolute quantum efficiency measurement. The design, key features, error analysis, and results from the test campaign are presented.

  2. Application of CCD drift-scan photoelectric technique on monitoring GEO satellites

    NASA Astrophysics Data System (ADS)

    Yu, Yong; Zhao, Xiao-Fen; Luo, Hao; Mao, Yin-Dun; Tang, Zheng-Hong

    2018-05-01

    Geosynchronous Earth Orbit (GEO) satellites are widely used because of their unique characteristics of high-orbit and remaining permanently in the same area of the sky. Precise monitoring of GEO satellites can provide a key reference for the judgment of satellite operation status, the capture and identification of targets, and the analysis of collision warning. The observation using ground-based optical telescopes plays an important role in the field of monitoring GEO targets. Different from distant celestial bodies, there is a relative movement between the GEO target and the background reference stars, which makes the conventional observation method limited for long focal length telescopes. CCD drift-scan photoelectric technique is applied on monitoring GEO targets. In the case of parking the telescope, the good round images of the background reference stars and the GEO target at the same sky region can be obtained through the alternating observation of CCD drift-scan mode and CCD stare mode, so as to improve the precision of celestial positioning for the GEO target. Observation experiments of GEO targets were carried out with 1.56-meter telescope of Shanghai Astronomical Observatory. The results show that the application of CCD drift-scan photoelectric technique makes the precision of observing the GEO target reach the level of 0.2″, which gives full play to the advantage of the long focal length of the telescope. The effect of orbit improvement based on multi-pass of observations is obvious and the prediction precision of extrapolating to 72-h is in the order of several arc seconds in azimuth and elevation.

  3. Measuring the effective pixel positions for the HARPS3 CCD

    NASA Astrophysics Data System (ADS)

    Hall, Richard D.; Thompson, Samantha; Queloz, Didier

    2016-07-01

    We present preliminary results from an experiment designed to measure the effective pixel positions of a CCD to sub-pixel precision. This technique will be used to characterise the 4k x 4k CCD destined for the HARPS-3 spectrograph. The principle of coherent beam interference is used to create intensity fringes along one axis of the CCD. By sweeping the physical parameters of the experiment, the geometry of the fringes can be altered which is used to probe the pixel structure. We also present the limitations of the current experimental set-up and suggest what will be implemented in the future to vastly improve the precision of the measurements.

  4. UltraForm Finishing (UFF) a 5-axis computer controlled precision optical component grinding and polishing system

    NASA Astrophysics Data System (ADS)

    Bechtold, Michael; Mohring, David; Fess, Edward

    2007-05-01

    OptiPro Systems has developed a new finishing process for the manufacturing of precision optical components. UltraForm Finishing (UFF) has evolved from a tire shaped tool with polishing material on its periphery, to its newest design, which incorporates a precision rubber wheel wrapped with a band of polishing material passing over it. Through our research we have developed a user friendly graphical interface giving the optician a deterministic path for finishing precision optical components. Complex UFF Algorithms combine the removal function and desired depth of removal into a motion controlled tool path which minimizes surface roughness and form errors. The UFF process includes 5 axes of computer controlled motion, (3 linear and 2 rotary) which provide the flexibility for finishing a variety of shapes including spheres, aspheres, and freeform optics. The long arm extension, along with a range of diameters for the "UltraWheel" provides a unique solution for the finishing of steep concave shapes such as ogives and domes. The UltraForm process utilizes, fixed and loose abrasives, in combination with our proprietary "UltraBelts" made of a range of materials such as polyurethane, felt, resin, diamond and others.

  5. pnCCD for photon detection from near-infrared to X-rays

    NASA Astrophysics Data System (ADS)

    Meidinger, Norbert; Andritschke, Robert; Hartmann, Robert; Herrmann, Sven; Holl, Peter; Lutz, Gerhard; Strüder, Lothar

    2006-09-01

    A pnCCD is a special type of charge-coupled device developed for spectroscopy and imaging of X-rays with high time resolution and quantum efficiency. Its most famous application is the operation on the XMM-Newton satellite, an X-ray astronomy mission that was launched by the European space agency in 1999. The excellent performance of the focal plane camera has been maintained for more than 6 years in orbit. The energy resolution in particular has shown hardly any degradation since launch. In order to satisfy the requirements of future X-ray astronomy missions as well as those of ground-based experiments, a new type of pnCCD has been developed. This ‘frame-store pnCCD’ shows an enhanced performance compared to the XMM-Newton type of pnCCD. Now, more options in device design and operation are available to tailor the detector to its respective application. Part of this concept is a programmable analog signal processor, which has been developed for the readout of the CCD signals. The electronic noise of the new detector has a value of only 2 electrons equivalent noise charge (ENC), which is less than half of the figure achieved for the XMM-Newton-type pnCCD. The energy resolution for the Mn-Kα line at 5.9 keV is approximately 130 eV FWHM. We have close to 100% quantum efficiency for both low- and high-energy photon detection (e.g. the C-K line at 277 eV, and the Ge-Kα line at 10 keV, respectively). Very high frame rates of 1000 images/s have been achieved due to the ultra-fast readout accomplished by the parallel architecture of the pnCCD and the analog signal processor. Excellent spectroscopic performance is shown even at the relatively high operating temperature of -25 °C that can be achieved by a Peltier cooler. The applications of the low-noise and fast pnCCD detector are not limited to the detection of X-rays. With an anti-reflective coating deposited on the photon entrance window, we achieve high quantum efficiency also for near-infrared and optical

  6. Ultra-precision turning of complex spiral optical delay line

    NASA Astrophysics Data System (ADS)

    Zhang, Xiaodong; Li, Po; Fang, Fengzhou; Wang, Qichang

    2011-11-01

    Optical delay line (ODL) implements the vertical or depth scanning of optical coherence tomography, which is the most important factor affecting the scanning resolution and speed. The spinning spiral mirror is found as an excellent optical delay device because of the high-speed and high-repetition-rate. However, it is one difficult task to machine the mirror due to the special shape and precision requirement. In this paper, the spiral mirror with titled parabolic generatrix is proposed, and the ultra-precision turning method is studied for its machining using the spiral mathematic model. Another type of ODL with the segmental shape is also introduced and machined to make rotation balance for the mass equalization when scanning. The efficiency improvement is considered in details, including the rough cutting with the 5- axis milling machine, the machining coordinates unification, and the selection of layer direction in turning. The onmachine measuring method based on stylus gauge is designed to analyze the shape deviation. The air bearing is used as the measuring staff and the laser interferometer sensor as the position sensor, whose repeatability accuracy is proved up to 10nm and the stable feature keeps well. With this method developed, the complex mirror with nanometric finish of 10.7nm in Ra and the form error within 1um are achieved.

  7. Precise CCD positions of Triton in 2014-2016 from the Gaia DR1

    NASA Astrophysics Data System (ADS)

    Wang, N.; Peng, Q. Y.; Peng, H. W.; Zhang, Q. F.

    2018-04-01

    755 CCD observations during the years 2014-2016 have been reduced to derive the precise positions of Triton, the first satellite of Neptune. The observations were made by the 1 m telescope at Yunnan Observatory over 15 nights during the years 2014-2016. The theoretical position of Triton was retrieved from the Jet Propulsion Laboratory Horizons system. Our results show that when the newest Gaia catalogue (Gaia DR1) is referred to the mean O-Cs (observed minus computed) residuals are about 0.042 and -0.006 arcsec, the dispersions are 0.012 and 0.012 arcsec in right ascension and declination, respectively. The dispersions are improved very significantly when the Gaia DR1 is referred to. However, the agreement in right ascension is not so good as that in declination, the reason might come from the uncertainty of planet ephemeris. More observations are needed to confirm this.

  8. A new Ultra Precision Interferometer for absolute length measurements down to cryogenic temperatures

    NASA Astrophysics Data System (ADS)

    Schödel, R.; Walkov, A.; Zenker, M.; Bartl, G.; Meeß, R.; Hagedorn, D.; Gaiser, C.; Thummes, G.; Heltzel, S.

    2012-09-01

    A new Ultra Precision Interferometer (UPI) was built at Physikalisch-Technische Bundesanstalt. As its precursor, the precision interferometer, it was designed for highly precise absolute length measurements of prismatic bodies, e.g. gauge blocks, under well-defined temperature conditions and pressure, making use of phase stepping imaging interferometry. The UPI enables a number of enhanced features, e.g. it is designed for a much better lateral resolution and better temperature stability. In addition to the original concept, the UPI is equipped with an external measurement pathway (EMP) in which a prismatic body can be placed alternatively. The temperature of the EMP can be controlled in a much wider range compared to the temperature of the interferometer's main chamber. An appropriate cryostat system, a precision temperature measurement system and improved imaging interferometry were established to permit absolute length measurements down to cryogenic temperature, demonstrated for the first time ever. Results of such measurements are important for studying thermal expansion of materials from room temperature towards less than 10 K.

  9. Advances in molecular dynamics simulation of ultra-precision machining of hard and brittle materials

    NASA Astrophysics Data System (ADS)

    Guo, Xiaoguang; Li, Qiang; Liu, Tao; Kang, Renke; Jin, Zhuji; Guo, Dongming

    2017-03-01

    Hard and brittle materials, such as silicon, SiC, and optical glasses, are widely used in aerospace, military, integrated circuit, and other fields because of their excellent physical and chemical properties. However, these materials display poor machinability because of their hard and brittle properties. Damages such as surface micro-crack and subsurface damage often occur during machining of hard and brittle materials. Ultra-precision machining is widely used in processing hard and brittle materials to obtain nanoscale machining quality. However, the theoretical mechanism underlying this method remains unclear. This paper provides a review of present research on the molecular dynamics simulation of ultra-precision machining of hard and brittle materials. The future trends in this field are also discussed.

  10. Occultation Predictions Using CCD Strip-Scanning Astrometry

    NASA Technical Reports Server (NTRS)

    Dunham, Edward W.; Ford, C. H.; Stone, R. P. S.; McDonald, S. W.; Olkin, C. B.; Elliot, J. L.; Witteborn, Fred C. (Technical Monitor)

    1994-01-01

    We are developing the method of CCD strip-scanning astrometry for the purpose of deriving reliable advance predictions for occultations involving small objects in the outer solar system. We are using a camera system based on a Ford/Loral 2Kx2K CCD with the Crossley telescope at Lick Observatory for this work. The columns of die CCD are aligned East-West, the telescope drive is stopped, and the CCD is clocked at the same rate that the stars drift across it. In this way we obtain arbitrary length strip images 20 arcmin wide with 0.58" pixels. Since planets move mainly in RA, it is possible to obtain images of the planet and star to be occulted on the same strip well before the occultation occurs. The strip-to-strip precision (i.e. reproducibility) of positions is limited by atmospheric image motion to about 0.1" rms per strip. However, for objects that are nearby in R.A., the image motion is highly correlated and their relative positions are good to 0.02" rms per strip. We will show that the effects of atmospheric image motion on a given strip can be removed if a sufficient number of strips of a given area have been obtained. Thus, it is possible to reach an rms precision of 0.02" per strip, corresponding to about 0.3 of Pluto or Triton's angular radius. The ultimate accuracy of a prediction based on strip-scanning astrometry is currently limited by the accuracy of the positions of the stars in the astrometric network used and by systematic errors most likely due to the optical system. We will show the results of . the prediction of some recent occultations as examples of the current capabilities and limitations of this technique.

  11. A High Resolution TDI CCD Camera forMicrosatellite (HRCM)

    NASA Astrophysics Data System (ADS)

    Hao, Yuncai; Zheng, You; Dong, Ying; Li, Tao; Yu, Shijie

    In resent years it is a important development direction in the commercial remote sensing field to obtain (1-5)m high ground resolution from space using microsatellite. Thanks to progress of new technologies, new materials and new detectors it is possible to develop 1m ground resolution space imaging system with weight less than 20kg. Based on many years works on optical system design a project of very high resolution TDI CCD camera using in space was proposed by the authors of this paper. The performance parameters and optical lay-out of the HRCM was presented. A compact optical design and results analysis for the system was given in the paper also. and small fold mirror to take a line field of view usable for TDI CCD and short outer size. The length along the largest size direction is about 1/4 of the focal length. And two 4096X96(grades) line TDI CCD will be used as the focal plane detector. The special optical parts are fixed near before the final image for getting the ground pixel resolution higher than the Nyquist resolution of the detector using the sub-pixel technique which will be explained in the paper. In the system optical SiC will be used as the mirror material, the C-C composite material will be used as the material of the mechanical structure framework. The circle frame of the primary and secondary mirrors will use one time turning on a machine tool in order to assuring concentric request for alignment of the system. In general the HRCM have the performance parameters with 2.5m focal length, 20 FOV, 1/11relative aperture, (0.4-0.8) micrometer spectral range, 10 micron pixel size of TDI CCD, weight less than 20kg, 1m ground pixel resolution at flying orbit 500km high. Design and analysis of the HRCM put up in the paper indicate that HRCM have many advantages to use it in space. Keywords High resolution TDI CCD Sub-pixel imaging Light-weighted optical system SiC mirror

  12. Quantum preservation of the measurements precision using ultra-short strong pulses in exact analytical solution

    NASA Astrophysics Data System (ADS)

    Berrada, K.; Eleuch, H.

    2017-09-01

    Various schemes have been proposed to improve the parameter-estimation precision. In the present work, we suggest an alternative method to preserve the estimation precision by considering a model that closely describes a realistic experimental scenario. We explore this active way to control and enhance the measurements precision for a two-level quantum system interacting with classical electromagnetic field using ultra-short strong pulses with an exact analytical solution, i.e. beyond the rotating wave approximation. In particular, we investigate the variation of the precision with a few cycles pulse and a smooth phase jump over a finite time interval. We show that by acting on the shape of the phase transient and other parameters of the considered system, the amount of information may be increased and has smaller decay rate in the long time. These features make two-level systems incorporated in ultra-short, of-resonant and gradually changing phase good candidates for implementation of schemes for the quantum computation and the coherent information processing.

  13. Thinning and mounting a Texas Instruments 3-phase CCD

    NASA Technical Reports Server (NTRS)

    Lesser, M. P.; Leach, R. W.; Angel, J. R. P.

    1986-01-01

    Thin CCDs with precise control of thickness and surface quality allow astronomers to optimize chips for specific applications. A means of mechanically thinning a TI 800 x 800 CCD with an abrasive slurry of aluminum oxide is presented. Using the same techniques, the abrasives can be replaced with a chemical solution to eliminate subsurface damage. A technique of mounting the CCD which retains the high quality surface generated during thinning is also demonstrated. This requires the backside of the chip to be bonded to a glass window which closely matches silicon's thermal expansion properties. Thinned CCDs require backside treatment to enhance blue and UV quantum efficiency. Two methods are discussed which may be effective with this mounting system.

  14. Fast and sensitive analysis of beta blockers by ultra-high-performance liquid chromatography coupled with ultra-high-resolution TOF mass spectrometry.

    PubMed

    Tomková, Jana; Ondra, Peter; Kocianová, Eva; Václavík, Jan

    2017-07-01

    This paper presents a method for the determination of acebutolol, betaxolol, bisoprolol, metoprolol, nebivolol and sotalol in human serum by liquid-liquid extraction and ultra-high-performance liquid chromatography coupled with ultra-high-resolution TOF mass spectrometry. After liquid-liquid extraction, beta blockers were separated on a reverse-phase analytical column (Acclaim RS 120; 100 × 2.1 mm, 2.2 μm). The total run time was 6 min for each sample. Linearity, limit of detection, limit of quantification, matrix effects, specificity, precision, accuracy, recovery and sample stability were evaluated. The method was successfully applied to the therapeutic drug monitoring of 108 patients with hypertension. This method was also used for determination of beta blockers in 33 intoxicated patients. Copyright © 2016 John Wiley & Sons, Ltd.

  15. CCD Camera Detection of HIV Infection.

    PubMed

    Day, John R

    2017-01-01

    Rapid and precise quantification of the infectivity of HIV is important for molecular virologic studies, as well as for measuring the activities of antiviral drugs and neutralizing antibodies. An indicator cell line, a CCD camera, and image-analysis software are used to quantify HIV infectivity. The cells of the P4R5 line, which express the receptors for HIV infection as well as β-galactosidase under the control of the HIV-1 long terminal repeat, are infected with HIV and then incubated 2 days later with X-gal to stain the infected cells blue. Digital images of monolayers of the infected cells are captured using a high resolution CCD video camera and a macro video zoom lens. A software program is developed to process the images and to count the blue-stained foci of infection. The described method allows for the rapid quantification of the infected cells over a wide range of viral inocula with reproducibility, accuracy and at relatively low cost.

  16. Challenges in mold manufacturing for high precision molded diffractive optical elements

    NASA Astrophysics Data System (ADS)

    Pongs, Guido; Bresseler, Bernd; Schweizer, Klaus; Bergs, Thomas

    2016-09-01

    Isothermal precision glass molding of imaging optics is the key technology for mass production of precise optical elements. Especially for numerous consumer applications (e.g. digital cameras, smart phones, …), high precision glass molding is applied for the manufacturing of aspherical lenses. The usage of diffractive optical elements (DOEs) can help to further reduce the number of lenses in the optical systems which will lead to a reduced weight of hand-held optical devices. But today the application of molded glass DOEs is limited due to the technological challenges in structuring the mold surfaces. Depending on the application submicrometer structures are required on the mold surface. Furthermore these structures have to be replicated very precisely to the glass lens surface. Especially the micro structuring of hard and brittle mold materials such as Tungsten Carbide is very difficult and not established. Thus a multitude of innovative approaches using diffractive optical elements cannot be realized. Aixtooling has investigated in different mold materials and different suitable machining technologies for the micro- and sub-micrometer structuring of mold surfaces. The focus of the work lays on ultra-precision grinding to generate the diffractive pattern on the mold surfaces. This paper presents the latest achievements in diffractive structuring of Tungsten Carbide mold surfaces by ultra-precision grinding.

  17. Ultra-precision positioning assembly

    DOEpatents

    Montesanti, Richard C.; Locke, Stanley F.; Thompson, Samuel L.

    2002-01-01

    An apparatus and method is disclosed for ultra-precision positioning. A slide base provides a foundational support. A slide plate moves with respect to the slide base along a first geometric axis. Either a ball-screw or a piezoelectric actuator working separate or in conjunction displaces the slide plate with respect to the slide base along the first geometric axis. A linking device directs a primary force vector into a center-line of the ball-screw. The linking device consists of a first link which directs a first portion of the primary force vector to an apex point, located along the center-line of the ball-screw, and a second link for directing a second portion of the primary force vector to the apex point. A set of rails, oriented substantially parallel to the center-line of the ball-screw, direct movement of the slide plate with respect to the slide base along the first geometric axis and are positioned such that the apex point falls within a geometric plane formed by the rails. The slide base, the slide plate, the ball-screw, and the linking device together form a slide assembly. Multiple slide assemblies can be distributed about a platform. In such a configuration, the platform may be raised and lowered, or tipped and tilted by jointly or independently displacing the slide plates.

  18. An Ultra-Precise Method for the Nano Thin-Film Removal

    NASA Astrophysics Data System (ADS)

    Pa, P. S.

    In this research an electrode-set is used to investigate via an ultra-precise method for the removal of Indium Tin Oxide (ITO) thin-film microstructure from defective display panels to conquer the low yield rate in display panel production as to from imperfect Indium Tin Oxide layer deposition is well known. This process, which involves the removal of ITO layer substructure by means of an electrochemical removal (ECMR), is of major interest to the optoelectronics semiconductor industry. In this electro machining process a high current flow and high feed rate of the display (color filter) achieves complete and efficient removal of the ITO layer. The ITO thin-film can be removed completely by a proper combination of feed rate and electric power. A small gap between the diameter cathode virtual rotation circle and the diameter virtual rotation circle also corresponds to a higher removal rate. A small anode edge radius with a small cathode edge radius effectively improves dregs discharge and is an advantage when associated with a high workpiece feed rate. This precision method for the recycling of defective display screen color filters is presented as an effective tool for use in the screen manufacturing process. The defective Indium Tin Oxide thin-film can be removed easily and cleanly in a short time. The complete removal of the ITO layer makes it possible to put these panels back into the production line for reuse with a considerable reduction of both waste and production cost.

  19. Combining HJ CCD, GF-1 WFV and MODIS Data to Generate Daily High Spatial Resolution Synthetic Data for Environmental Process Monitoring.

    PubMed

    Wu, Mingquan; Huang, Wenjiang; Niu, Zheng; Wang, Changyao

    2015-08-20

    The limitations of satellite data acquisition mean that there is a lack of satellite data with high spatial and temporal resolutions for environmental process monitoring. In this study, we address this problem by applying the Enhanced Spatial and Temporal Adaptive Reflectance Fusion Model (ESTARFM) and the Spatial and Temporal Data Fusion Approach (STDFA) to combine Huanjing satellite charge coupled device (HJ CCD), Gaofen satellite no. 1 wide field of view camera (GF-1 WFV) and Moderate Resolution Imaging Spectroradiometer (MODIS) data to generate daily high spatial resolution synthetic data for land surface process monitoring. Actual HJ CCD and GF-1 WFV data were used to evaluate the precision of the synthetic images using the correlation analysis method. Our method was tested and validated for two study areas in Xinjiang Province, China. The results show that both the ESTARFM and STDFA can be applied to combine HJ CCD and MODIS reflectance data, and GF-1 WFV and MODIS reflectance data, to generate synthetic HJ CCD data and synthetic GF-1 WFV data that closely match actual data with correlation coefficients (r) greater than 0.8989 and 0.8643, respectively. Synthetic red- and near infrared (NIR)-band data generated by ESTARFM are more suitable for the calculation of Normalized Different Vegetation Index (NDVI) than the data generated by STDFA.

  20. Combining HJ CCD, GF-1 WFV and MODIS Data to Generate Daily High Spatial Resolution Synthetic Data for Environmental Process Monitoring

    PubMed Central

    Wu, Mingquan; Huang, Wenjiang; Niu, Zheng; Wang, Changyao

    2015-01-01

    The limitations of satellite data acquisition mean that there is a lack of satellite data with high spatial and temporal resolutions for environmental process monitoring. In this study, we address this problem by applying the Enhanced Spatial and Temporal Adaptive Reflectance Fusion Model (ESTARFM) and the Spatial and Temporal Data Fusion Approach (STDFA) to combine Huanjing satellite charge coupled device (HJ CCD), Gaofen satellite no. 1 wide field of view camera (GF-1 WFV) and Moderate Resolution Imaging Spectroradiometer (MODIS) data to generate daily high spatial resolution synthetic data for land surface process monitoring. Actual HJ CCD and GF-1 WFV data were used to evaluate the precision of the synthetic images using the correlation analysis method. Our method was tested and validated for two study areas in Xinjiang Province, China. The results show that both the ESTARFM and STDFA can be applied to combine HJ CCD and MODIS reflectance data, and GF-1 WFV and MODIS reflectance data, to generate synthetic HJ CCD data and synthetic GF-1 WFV data that closely match actual data with correlation coefficients (r) greater than 0.8989 and 0.8643, respectively. Synthetic red- and near infrared (NIR)-band data generated by ESTARFM are more suitable for the calculation of Normalized Different Vegetation Index (NDVI) than the data generated by STDFA. PMID:26308017

  1. Fundamental performance differences of CMOS and CCD imagers: part V

    NASA Astrophysics Data System (ADS)

    Janesick, James R.; Elliott, Tom; Andrews, James; Tower, John; Pinter, Jeff

    2013-02-01

    Previous papers delivered over the last decade have documented developmental progress made on large pixel scientific CMOS imagers that match or surpass CCD performance. New data and discussions presented in this paper include: 1) a new buried channel CCD fabricated on a CMOS process line, 2) new data products generated by high performance custom scientific CMOS 4T/5T/6T PPD pixel imagers, 3) ultimate CTE and speed limits for large pixel CMOS imagers, 4) fabrication and test results of a flight 4k x 4k CMOS imager for NRL's SoloHi Solar Orbiter Mission, 5) a progress report on ultra large stitched Mk x Nk CMOS imager, 6) data generated by on-chip sub-electron CDS signal chain circuitry used in our imagers, 7) CMOS and CMOSCCD proton and electron radiation damage data for dose levels up to 10 Mrd, 8) discussions and data for a new class of PMOS pixel CMOS imagers and 9) future CMOS development work planned.

  2. Single-Electron and Single-Photon Sensitivity with a Silicon Skipper CCD

    NASA Astrophysics Data System (ADS)

    Tiffenberg, Javier; Sofo-Haro, Miguel; Drlica-Wagner, Alex; Essig, Rouven; Guardincerri, Yann; Holland, Steve; Volansky, Tomer; Yu, Tien-Tien

    2017-09-01

    We have developed ultralow-noise electronics in combination with repetitive, nondestructive readout of a thick, fully depleted charge-coupled device (CCD) to achieve an unprecedented noise level of 0.068 e- rms /pixel . This is the first time that discrete subelectron readout noise has been achieved reproducible over millions of pixels on a stable, large-area detector. This enables the contemporaneous, discrete, and quantized measurement of charge in pixels, irrespective of whether they contain zero electrons or thousands of electrons. Thus, the resulting CCD detector is an ultra-sensitive calorimeter. It is also capable of counting single photons in the optical and near-infrared regime. Implementing this innovative non-destructive readout system has a negligible impact on CCD design and fabrication, and there are nearly immediate scientific applications. As a particle detector, this CCD will have unprecedented sensitivity to low-mass dark matter particles and coherent neutrino-nucleus scattering, while future astronomical applications may include direct imaging and spectroscopy of exoplanets.

  3. Single-Electron and Single-Photon Sensitivity with a Silicon Skipper CCD.

    PubMed

    Tiffenberg, Javier; Sofo-Haro, Miguel; Drlica-Wagner, Alex; Essig, Rouven; Guardincerri, Yann; Holland, Steve; Volansky, Tomer; Yu, Tien-Tien

    2017-09-29

    We have developed ultralow-noise electronics in combination with repetitive, nondestructive readout of a thick, fully depleted charge-coupled device (CCD) to achieve an unprecedented noise level of 0.068  e^{-} rms/pixel. This is the first time that discrete subelectron readout noise has been achieved reproducible over millions of pixels on a stable, large-area detector. This enables the contemporaneous, discrete, and quantized measurement of charge in pixels, irrespective of whether they contain zero electrons or thousands of electrons. Thus, the resulting CCD detector is an ultra-sensitive calorimeter. It is also capable of counting single photons in the optical and near-infrared regime. Implementing this innovative non-destructive readout system has a negligible impact on CCD design and fabrication, and there are nearly immediate scientific applications. As a particle detector, this CCD will have unprecedented sensitivity to low-mass dark matter particles and coherent neutrino-nucleus scattering, while future astronomical applications may include direct imaging and spectroscopy of exoplanets.

  4. The research and realization of digital management platform for ultra-precision optical elements within life-cycle

    NASA Astrophysics Data System (ADS)

    Wang, Juan; Wang, Jian; Li, Lijuan; Zhou, Kun

    2014-08-01

    In order to solve the information fusion, process integration, collaborative design and manufacturing for ultra-precision optical elements within life-cycle management, this paper presents a digital management platform which is based on product data and business processes by adopting the modern manufacturing technique, information technique and modern management technique. The architecture and system integration of the digital management platform are discussed in this paper. The digital management platform can realize information sharing and interaction for information-flow, control-flow and value-stream from user's needs to offline in life-cycle, and it can also enhance process control, collaborative research and service ability of ultra-precision optical elements.

  5. Night Sky Weather Monitoring System Using Fish-Eye CCD

    NASA Astrophysics Data System (ADS)

    Tomida, Takayuki; Saito, Yasunori; Nakamura, Ryo; Yamazaki, Katsuya

    Telescope Array (TA) is international joint experiment observing ultra-high energy cosmic rays. TA employs fluorescence detection technique to observe cosmic rays. In this technique, tho existence of cloud significantly affects quality of data. Therefore, cloud monitoring provides important information. We are developing two new methods for evaluating night sky weather with pictures taken by charge-coupled device (CCD) camera. One is evaluating the amount of cloud with pixels brightness. The other is counting the number of stars with contour detection technique. The results of these methods show clear correlation, and we concluded both the analyses are reasonable methods for weather monitoring. We discuss reliability of the star counting method.

  6. An Astronomical Test of CCD Photometric Precision

    NASA Technical Reports Server (NTRS)

    Koch, David G.; Dunham, Edward W.; Borucki, William J.; Jenkins, Jon M.

    2001-01-01

    Ground-based differential photometry is limited to a precision of order 10(exp -3) because of atmospheric effects. A space-based photometer should be limited only by the inherent instrument precision and shot noise. Laboratory tests have shown that a precision of order 10-5 is achievable with commercially available charged coupled devices (CCDs). We have proposed to take this one step further by performing measurements at a telescope using a Wollaston prism as a beam splitter First-order atmospheric effects (e.g., extinction) will appear to be identical in the two images of each star formed by the prism and will be removed in the data analysis. This arrangement can determine the precision that is achievable under the influence of second-order atmospheric effects (e.g., variable point-spread function (PSF) from seeing). These telescopic observations will thus provide a lower limit to the precision that can be realized by a space-based differential photometer.

  7. Mesoplasticity approach to studies of the cutting mechanism in ultra-precision machining

    NASA Astrophysics Data System (ADS)

    Lee, Rongbin W. B.; Wang, Hao; To, Suet; Cheung, Chi Fai; Chan, Chang Yuen

    2014-03-01

    There have been various theoretical attempts by researchers worldwide to link up different scales of plasticity studies from the nano-, micro- and macro-scale of observation, based on molecular dynamics, crystal plasticity and continuum mechanics. Very few attempts, however, have been reported in ultra-precision machining studies. A mesoplasticity approach advocated by Lee and Yang is adopted by the authors and is successfully applied to studies of the micro-cutting mechanisms in ultra-precision machining. Traditionally, the shear angle in metal cutting, as well as the cutting force variation, can only be determined from cutting tests. In the pioneering work of the authors, the use of mesoplasticity theory enables prediction of the fluctuation of the shear angle and micro-cutting force, shear band formation, chip morphology in diamond turning and size effect in nano-indentation. These findings are verified by experiments. The mesoplasticity formulation opens up a new direction of studies to enable how the plastic behaviour of materials and their constitutive representations in deformation processing, such as machining can be predicted, assessed and deduced from the basic properties of the materials measurable at the microscale.

  8. Single-Electron and Single-Photon Sensitivity with a Silicon Skipper CCD

    DOE PAGES

    Tiffenberg, Javier; Sofo-Haro, Miguel; Drlica-Wagner, Alex; ...

    2017-09-26

    Here, we have developed ultralow-noise electronics in combination with repetitive, nondestructive readout of a thick, fully depleted charge-coupled device (CCD) to achieve an unprecedented noise level of 0.068 e - rms/pixel. This is the first time that discrete subelectron readout noise has been achieved reproducible over millions of pixels on a stable, large-area detector. This enables the contemporaneous, discrete, and quantized measurement of charge in pixels, irrespective of whether they contain zero electrons or thousands of electrons. Thus, the resulting CCD detector is an ultra-sensitive calorimeter. It is also capable of counting single photons in the optical and near-infrared regime.more » Implementing this innovative non-destructive readout system has a negligible impact on CCD design and fabrication, and there are nearly immediate scientific applications. As a particle detector, this CCD will have unprecedented sensitivity to low-mass dark matter particles and coherent neutrino-nucleus scattering, while future astronomical applications may include direct imaging and spectroscopy of exoplanets.« less

  9. Characterization of a fully depleted CCD on high-resistivity silicon

    NASA Astrophysics Data System (ADS)

    Stover, Richard J.; Wei, Mingzhi; Lee, Y.; Gilmore, David K.; Holland, S. E.; Groom, D. E.; Moses, William W.; Perlmutter, Saul; Goldhaber, G.; Pennypacker, C.; Wang, N. W.; Palaio, N.

    1997-04-01

    Most scientific CCD imagers are fabricated on 30-50 (Omega) - cm epitaxial silicon. When illuminated form the front side of the device they generally have low quantum efficiency in the blue region of the visible spectrum because of strong absorption in the polycrystalline silicon gates as well as poor quantum efficiency in the far red and near infrared region of the spectrum because of the shallow depletion depth of the low-resistivity silicon. To enhance the blue response of scientific CCDs they are often thinned and illuminated from the back side. While blue response is greatly enhanced by this process, it is expensive and it introduces additional problems for the red end of the spectrum. A typical thinned CCD is 15 to 25 micrometers thick, and at wavelengths beyond about 800 nm the absorption depth becomes comparable to the thickness of the device, leading to interference fringes from reflected light. Because these interference fringes are of high order, the spatial pattern of the fringes is extremely sensitive to small changes in the optical illumination of the detector. Calibration and removal of the effects of the fringes is one of the primary limitations on the performance of astronomical images taken at wavelengths of 800 nm or more. In this paper we present results from the characterization of a CCD which promises to address many of the problems of typical thinned CCDs. The CCD reported on here was fabricated at Lawrence Berkeley National Laboratory (LBNL) on a 10-12 K$OMega-cm n-type silicon substrate.THe CCD is a 200 by 200 15-micrometers square pixel array, and due to the very high resistivity of the starting material, the entire 300 micrometers substrate is depleted. Full depletion works because of the gettering technology developed at LBNL which keeps leakage current down. Both front-side illuminated and backside illuminated devices have been tested. We have measured quantum efficiency, read-noise, full-well, charge-transfer efficiency, and leakage

  10. The design and development of low- and high-voltage ASICs for space-borne CCD cameras

    NASA Astrophysics Data System (ADS)

    Waltham, N.; Morrissey, Q.; Clapp, M.; Bell, S.; Jones, L.; Torbet, M.

    2017-12-01

    The CCD remains the pre-eminent visible and UV wavelength image sensor in space science, Earth and planetary remote sensing. However, the design of space-qualified CCD readout electronics is a significant challenge with requirements for low-volume, low-mass, low-power, high-reliability and tolerance to space radiation. Space-qualified components are frequently unavailable and up-screened commercial components seldom meet project or international space agency requirements. In this paper, we describe an alternative approach of designing and space-qualifying a series of low- and high-voltage mixed-signal application-specific integrated circuits (ASICs), the ongoing development of two low-voltage ASICs with successful flight heritage, and two new high-voltage designs. A challenging sub-system of any CCD camera is the video processing and digitisation electronics. We describe recent developments to improve performance and tolerance to radiation-induced single event latchup of a CCD video processing ASIC originally developed for NASA's Solar Terrestrial Relations Observatory and Solar Dynamics Observatory. We also describe a programme to develop two high-voltage ASICs to address the challenges presented with generating a CCD's bias voltages and drive clocks. A 0.35 μm, 50 V tolerant, CMOS process has been used to combine standard low-voltage 3.3 V transistors with high-voltage 50 V diffused MOSFET transistors that enable output buffers to drive CCD bias drains, gates and clock electrodes directly. We describe a CCD bias voltage generator ASIC that provides 24 independent and programmable 0-32 V outputs. Each channel incorporates a 10-bit digital-to-analogue converter, provides current drive of up to 20 mA into loads of 10 μF, and includes current-limiting and short-circuit protection. An on-chip telemetry system with a 12-bit analogue-to-digital converter enables the outputs and multiple off-chip camera voltages to be monitored. The ASIC can drive one or more CCDs and

  11. High-performance visible/UV CCD focal plane technology for spacebased applications

    NASA Technical Reports Server (NTRS)

    Burke, B. E.; Mountain, R. W.; Gregory, J. A.; Huang, J. C. M.; Cooper, M. J.; Savoye, E. D.; Kosicki, B. B.

    1993-01-01

    We describe recent technology developments aimed at large CCD imagers for space based applications in the visible and UV. Some of the principal areas of effort include work on reducing device degradation in the natural space-radiation environment, improvements in quantum efficiency in the visible and UV, and larger-device formats. One of the most serious hazards for space based CCD's operating at low signal levels is the displacement damage resulting from bombardment by energetic protons. Such damage degrades charge-transfer efficiency and increases dark current. We have achieved improved hardness to proton-induced displacement damage by selective ion implants into the CCD channel and by reduced temperature of operation. To attain high quantum efficiency across the visible and UV we have developed a technology for back-illuminated CCD's. With suitable antireflection (AR) coatings such devices have quantum efficiencies near 90 percent in the 500-700-nm band. In the UV band from 200 to 400 nm, where it is difficult to find coatings that are sufficiently transparent and can provide good matching to the high refractive index of silicon, we have been able to substantially increase the quantum efficiency using a thin film of HfO2 as an AR coating. These technology efforts were applied to a 420 x 420-pixel frame-transfer imager, and future work will be extended to a 1024 x 1024-pixel device now under development.

  12. Fully depleted back illuminated CCD

    DOEpatents

    Holland, Stephen Edward

    2001-01-01

    A backside illuminated charge coupled device (CCD) is formed of a relatively thick high resistivity photon sensitive silicon substrate, with frontside electronic circuitry, and an optically transparent backside ohmic contact for applying a backside voltage which is at least sufficient to substantially fully deplete the substrate. A greater bias voltage which overdepletes the substrate may also be applied. One way of applying the bias voltage to the substrate is by physically connecting the voltage source to the ohmic contact. An alternate way of applying the bias voltage to the substrate is to physically connect the voltage source to the frontside of the substrate, at a point outside the depletion region. Thus both frontside and backside contacts can be used for backside biasing to fully deplete the substrate. Also, high resistivity gaps around the CCD channels and electrically floating channel stop regions can be provided in the CCD array around the CCD channels. The CCD array forms an imaging sensor useful in astronomy.

  13. Software design of control system of CCD side-scatter lidar

    NASA Astrophysics Data System (ADS)

    Kuang, Zhiqiang; Liu, Dong; Deng, Qian; Zhang, Zhanye; Wang, Zhenzhu; Yu, Siqi; Tao, Zongming; Xie, Chenbo; Wang, Yingjian

    2018-03-01

    Because of the existence of blind zone and transition zone, the application of backscattering lidar in near-ground is limited. The side-scatter lidar equipped with the Charge Coupled Devices (CCD) can separate the transmitting and receiving devices to avoid the impact of the geometric factors which is exited in the backscattering lidar and, detect the more precise near-ground aerosol signals continuously. Theories of CCD side-scatter lidar and the design of control system are introduced. The visible control of laser and CCD and automatic data processing method of the side-scatter lidar are developed by using the software of Visual C #. The results which are compared with the calibration of the atmospheric aerosol lidar data show that signals from the CCD side- scatter lidar are convincible.

  14. Development of a 300,000-pixel ultrahigh-speed high-sensitivity CCD

    NASA Astrophysics Data System (ADS)

    Ohtake, H.; Hayashida, T.; Kitamura, K.; Arai, T.; Yonai, J.; Tanioka, K.; Maruyama, H.; Etoh, T. Goji; Poggemann, D.; Ruckelshausen, A.; van Kuijk, H.; Bosiers, Jan T.

    2006-02-01

    We are developing an ultrahigh-speed, high-sensitivity broadcast camera that is capable of capturing clear, smooth slow-motion videos even where lighting is limited, such as at professional baseball games played at night. In earlier work, we developed an ultrahigh-speed broadcast color camera1) using three 80,000-pixel ultrahigh-speed, highsensitivity CCDs2). This camera had about ten times the sensitivity of standard high-speed cameras, and enabled an entirely new style of presentation for sports broadcasts and science programs. Most notably, increasing the pixel count is crucially important for applying ultrahigh-speed, high-sensitivity CCDs to HDTV broadcasting. This paper provides a summary of our experimental development aimed at improving the resolution of CCD even further: a new ultrahigh-speed high-sensitivity CCD that increases the pixel count four-fold to 300,000 pixels.

  15. Event-Driven X-Ray CCD Detectors for High Energy Astrophysics

    NASA Technical Reports Server (NTRS)

    Ricker, George R.

    2004-01-01

    A viewgraph presentation describing the Event-Driven X- Ray CCD (EDCCD) detector system for high energy astrophysics is presented. The topics include: 1) EDCCD: Description and Advantages; 2) Summary of Grant Activity Carried Out; and 3) EDCCD Test System.

  16. Interferometric apparatus for ultra-high precision displacement measurement

    NASA Technical Reports Server (NTRS)

    Zhao, Feng (Inventor)

    2004-01-01

    A high-precision heterodyne interferometer measures relative displacement by creating a thermally-insensitive system generally not subject to polarization leakage. By using first and second light beams separated by a small frequency difference (.DELTA.f), beams of light at the first frequency (f.sub.0) are reflected by co-axial mirrors, the first mirror of which has a central aperture through which the light is transmitted to and reflected by the second mirror. Prior to detection, the light beams from the two mirrors are combined with light of the second and slightly different frequency. The combined light beams are separated according to the light from the mirrors. The change in phase (.DELTA..phi.) with respect to the two signals is proportional to the change in distance of Fiducial B by a factor of wavelength (.lambda.) divided by 4.pi. (.DELTA.L=.lambda..DELTA..phi.1/(4.pi.)). In a second embodiment, a polarizing beam splitting system can be used.

  17. Design and Fabrication of High-Efficiency CMOS/CCD Imagers

    NASA Technical Reports Server (NTRS)

    Pain, Bedabrata

    2007-01-01

    An architecture for back-illuminated complementary metal oxide/semiconductor (CMOS) and charge-coupled-device (CCD) ultraviolet/visible/near infrared- light image sensors, and a method of fabrication to implement the architecture, are undergoing development. The architecture and method are expected to enable realization of the full potential of back-illuminated CMOS/CCD imagers to perform with high efficiency, high sensitivity, excellent angular response, and in-pixel signal processing. The architecture and method are compatible with next-generation CMOS dielectric-forming and metallization techniques, and the process flow of the method is compatible with process flows typical of the manufacture of very-large-scale integrated (VLSI) circuits. The architecture and method overcome all obstacles that have hitherto prevented high-yield, low-cost fabrication of back-illuminated CMOS/CCD imagers by use of standard VLSI fabrication tools and techniques. It is not possible to discuss the obstacles in detail within the space available for this article. Briefly, the obstacles are posed by the problems of generating light-absorbing layers having desired uniform and accurate thicknesses, passivation of surfaces, forming structures for efficient collection of charge carriers, and wafer-scale thinning (in contradistinction to diescale thinning). A basic element of the present architecture and method - the element that, more than any other, makes it possible to overcome the obstacles - is the use of an alternative starting material: Instead of starting with a conventional bulk-CMOS wafer that consists of a p-doped epitaxial silicon layer grown on a heavily-p-doped silicon substrate, one starts with a special silicon-on-insulator (SOI) wafer that consists of a thermal oxide buried between a lightly p- or n-doped, thick silicon layer and a device silicon layer of appropriate thickness and doping. The thick silicon layer is used as a handle: that is, as a mechanical support for the

  18. Experimental research on thermal conductive fillers for CCD module in space borne optical remote sensor

    NASA Astrophysics Data System (ADS)

    Zeng, Yi; Han, Xue-bing; Yang, Dong-shang; Gui, Li-jia; Zhao, Xiao-xiang; Si, Fu-qi

    2016-03-01

    A space-borne differential optical absorption spectrometer is a high precision aerospace optical remote sensor. It obtains the hyper-spectral,high spatial resolution radiation information by using the spectrometer with CCD(Charge Coupled Device)array detectors. Since a few CCDs are used as the key detector, the performance of the entire instrument is greatly affected by working condition of CCDs. The temperature of CCD modules has a great impact on the instrument measurement accuracy. It requires strict temperature control. The selection of the thermal conductive filler sticking CCD to the radiator is important in the CCD thermal design. Besides,due tothe complex and compact structure, it needs to take into account the anti-pollution of the optical system. Therefore, it puts forward high requirements on the selection of the conductive filler. In this paper, according to the structure characteristics of the CCD modules and the distribution of heat consumption, the thermal analysis tool I-DEAS/TMG is utilized to compute and simulate the temperature level of the CCD modules, while filling in thermal grease and thermal pad respectively. The temperature distribution of CCD heat dissipation in typical operating conditions is obtained. In addition, the heat balance test was carried out under the condition of two kinds of thermal conductive fillers. The thermal control of CCD was tested under various conditions, and the results were compared with the results of thermal analysis. The results show that there are some differences in thermal performance between the two kinds of thermal conductive fillers. Although they both can meet the thermal performance requirements of the instrument, either would be chosen taking account of other conditions and requirements such as anti-pollution and insulation. The content and results of this paper will be a good reference for the thermal design of the CCD in the aerospace optical payload.

  19. Extreme ultra-violet movie camera for imaging microsecond time scale magnetic reconnection

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

    Chai, Kil-Byoung; Bellan, Paul M.

    2013-12-15

    An ultra-fast extreme ultra-violet (EUV) movie camera has been developed for imaging magnetic reconnection in the Caltech spheromak/astrophysical jet experiment. The camera consists of a broadband Mo:Si multilayer mirror, a fast decaying YAG:Ce scintillator, a visible light block, and a high-speed visible light CCD camera. The camera can capture EUV images as fast as 3.3 × 10{sup 6} frames per second with 0.5 cm spatial resolution. The spectral range is from 20 eV to 60 eV. EUV images reveal strong, transient, highly localized bursts of EUV radiation when magnetic reconnection occurs.

  20. Applications of a pnCCD detector coupled to columnar structure CsI(Tl) scintillator system in ultra high energy X-ray Laue diffraction

    NASA Astrophysics Data System (ADS)

    Shokr, M.; Schlosser, D.; Abboud, A.; Algashi, A.; Tosson, A.; Conka, T.; Hartmann, R.; Klaus, M.; Genzel, C.; Strüder, L.; Pietsch, U.

    2017-12-01

    Most charge coupled devices (CCDs) are made of silicon (Si) with typical active layer thicknesses of several microns. In case of a pnCCD detector the sensitive Si thickness is 450 μm. However, for silicon based detectors the quantum efficiency for hard X-rays drops significantly for photon energies above 10 keV . This drawback can be overcome by combining a pixelated silicon-based detector system with a columnar scintillator. Here we report on the characterization of a low noise, fully depleted 128×128 pixels pnCCD detector with 75×75 μm2 pixel size coupled to a 700 μm thick columnar CsI(Tl) scintillator in the photon range between 1 keV to 130 keV . The excellent performance of the detection system in the hard X-ray range is demonstrated in a Laue type X-ray diffraction experiment performed at EDDI beamline of the BESSY II synchrotron taken at a set of several GaAs single crystals irradiated by white synchrotron radiation. With the columnar structure of the scintillator, the position resolution of the whole system reaches a value of less than one pixel. Using the presented detector system and considering the functional relation between indirect and direct photon events Laue diffraction peaks with X-ray energies up to 120 keV were efficiently detected. As one of possible applications of the combined CsI-pnCCD system we demonstrate that the accuracy of X-ray structure factors extracted from Laue diffraction peaks can be significantly improved in hard X-ray range using the combined CsI(Tl)-pnCCD system compared to a bare pnCCD.

  1. High-resolution chronology of sediment below CCD based on Holocene paleomagnetic secular variations in the Tohoku-oki earthquake rupture zone

    NASA Astrophysics Data System (ADS)

    Kanamatsu, Toshiya; Usami, Kazuko; McHugh, Cecilia M. G.; Ikehara, Ken

    2017-08-01

    Using high-resolution paleomagnetic data, we examined the potential for obtaining precise ages from sediment core samples recovered from deep-sea basins close to rupture zones of the 2011 and earlier earthquakes off Tohoku, Japan. Obtaining detailed stratigraphic ages from deep-sea sediments below the calcium compensation depth (CCD) is difficult, but we found that the samples contain excellent paleomagnetic secular variation records to constrain age models. Variations in paleomagnetic directions obtained from the sediments reveal systematic changes in the cores. A stacked paleomagnetic profile closely matches the Lake Biwa data sets in southwest Japan for the past 7000 years, one can establish age models based on secular variations of the geomagnetic field on sediments recovered uniquely below the CCD. Comparison of paleomagnetic directions near a tephra and a paleomagnetic direction of contemporaneous pyroclastic flow deposits acquired by different magnetization processes shows precise depositional ages reflecting the magnetization delay of the marine sediment record.Plain Language SummaryGenerally obtaining detailed ages from deep-sea sediments is difficult, because available dating method is very limited. We found that the deep-see sediment off North Japan recorded past sequential geomagnetic directions. If those records correlate well with the reference record in past 7000 years, then we could estimate age of sediment by pattern matching. Additionally a volcanic ash emitted in 915 A.D., which was intercalated in our samples, indicates a time lag in our age model. This observation makes our age model more <span class="hlt">precise</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22340219-ccd-photometry-bright-stars-using-objective-wire-mesh','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22340219-ccd-photometry-bright-stars-using-objective-wire-mesh"><span><span class="hlt">CCD</span> Photometry of bright stars using objective wire mesh</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>Kamiński, Krzysztof; Zgórz, Marika; Schwarzenberg-Czerny, Aleksander, E-mail: chrisk@amu.edu.pl</p> <p>2014-06-01</p> <p>Obtaining accurate photometry of bright stars from the ground remains problematic due to the danger of overexposing the target and/or the lack of suitable nearby comparison stars. The century-old method of using objective wire mesh to produce multiple stellar images seems promising for the <span class="hlt">precise</span> <span class="hlt">CCD</span> photometry of such stars. Furthermore, our tests on β Cep and its comparison star, differing by 5 mag, are very encouraging. Using a <span class="hlt">CCD</span> camera and a 20 cm telescope with the objective covered by a plastic wire mesh, in poor weather conditions, we obtained differential photometry with a <span class="hlt">precision</span> of 4.5 mmag permore » two minute exposure. Our technique is flexible and may be tuned to cover a range as big as 6-8 mag. We discuss the possibility of installing a wire mesh directly in the filter wheel.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/872737','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/872737"><span>Transmission electron microscope <span class="hlt">CCD</span> camera</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Downing, Kenneth H.</p> <p>1999-01-01</p> <p>In order to improve the performance of a <span class="hlt">CCD</span> camera on a <span class="hlt">high</span> voltage electron microscope, an electron decelerator is inserted between the microscope column and the <span class="hlt">CCD</span>. This arrangement optimizes the interaction of the electron beam with the scintillator of the <span class="hlt">CCD</span> camera while retaining optimization of the microscope optics and of the interaction of the beam with the specimen. Changing the electron beam energy between the specimen and camera allows both to be optimized.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/864811','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/864811"><span><span class="hlt">High</span> <span class="hlt">precision</span> triangular waveform generator</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Mueller, Theodore R.</p> <p>1983-01-01</p> <p>An <span class="hlt">ultra</span>-linear ramp generator having separately programmable ascending and descending ramp rates and voltages is provided. Two constant current sources provide the ramp through an integrator. Switching of the current at current source inputs rather than at the integrator input eliminates switching transients and contributes to the waveform <span class="hlt">precision</span>. The triangular waveforms produced by the waveform generator are characterized by accurate reproduction and low drift over periods of several hours. The ascending and descending slopes are independently selectable.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5039406','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/5039406"><span><span class="hlt">High-precision</span> triangular-waveform generator</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Mueller, T.R.</p> <p>1981-11-14</p> <p>An <span class="hlt">ultra</span>-linear ramp generator having separately programmable ascending and decending ramp rates and voltages is provided. Two constant current sources provide the ramp through an integrator. Switching of the current at current source inputs rather than at the integrator input eliminates switching transients and contributes to the waveform <span class="hlt">precision</span>. The triangular waveforms produced by the waveform generator are characterized by accurate reproduction and low drift over periods of several hours. The ascending and descending slopes are independently selectable.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MeScT..29e4004C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MeScT..29e4004C"><span>An <span class="hlt">ultra-precision</span> tool nanoindentation instrument for replication of single point diamond tool cutting edges</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cai, Yindi; Chen, Yuan-Liu; Xu, Malu; Shimizu, Yuki; Ito, So; Matsukuma, Hiraku; Gao, Wei</p> <p>2018-05-01</p> <p><span class="hlt">Precision</span> replication of the diamond tool cutting edge is required for non-destructive tool metrology. This paper presents an <span class="hlt">ultra-precision</span> tool nanoindentation instrument designed and constructed for replication of the cutting edge of a single point diamond tool onto a selected soft metal workpiece by <span class="hlt">precisely</span> indenting the tool cutting edge into the workpiece surface. The instrument has the ability to control the indentation depth with a nanometric resolution, enabling the replication of tool cutting edges with <span class="hlt">high</span> <span class="hlt">precision</span>. The motion of the diamond tool along the indentation direction is controlled by the piezoelectric actuator of a fast tool servo (FTS). An integrated capacitive sensor of the FTS is employed to detect the displacement of the diamond tool. The soft metal workpiece is attached to an aluminum cantilever whose deflection is monitored by another capacitive sensor, referred to as an outside capacitive sensor. The indentation force and depth can be accurately evaluated from the diamond tool displacement, the cantilever deflection and the cantilever spring constant. Experiments were carried out by replicating the cutting edge of a single point diamond tool with a nose radius of 2.0 mm on a copper workpiece surface. The profile of the replicated tool cutting edge was measured using an atomic force microscope (AFM). The effectiveness of the instrument in <span class="hlt">precision</span> replication of diamond tool cutting edges is well-verified by the experimental results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23478758','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23478758"><span>Measuring <span class="hlt">high</span>-resolution sky luminance distributions with a <span class="hlt">CCD</span> camera.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tohsing, Korntip; Schrempf, Michael; Riechelmann, Stefan; Schilke, Holger; Seckmeyer, Gunther</p> <p>2013-03-10</p> <p>We describe how sky luminance can be derived from a newly developed hemispherical sky imager (HSI) system. The system contains a commercial compact charge coupled device (<span class="hlt">CCD</span>) camera equipped with a fish-eye lens. The projection of the camera system has been found to be nearly equidistant. The luminance from the <span class="hlt">high</span> dynamic range images has been calculated and then validated with luminance data measured by a <span class="hlt">CCD</span> array spectroradiometer. The deviation between both datasets is less than 10% for cloudless and completely overcast skies, and differs by no more than 20% for all sky conditions. The global illuminance derived from the HSI pictures deviates by less than 5% and 20% under cloudless and cloudy skies for solar zenith angles less than 80°, respectively. This system is therefore capable of measuring sky luminance with the <span class="hlt">high</span> spatial and temporal resolution of more than a million pixels and every 20 s respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhDT.......175S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhDT.......175S"><span>Observing exoplanet populations with <span class="hlt">high-precision</span> astrometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sahlmann, Johannes</p> <p>2012-06-01</p> <p>This thesis deals with the application of the astrometry technique, consisting in measuring the position of a star in the plane of the sky, for the discovery and characterisation of extra-solar planets. It is feasible only with a very <span class="hlt">high</span> measurement <span class="hlt">precision</span>, which motivates the use of space observatories, the development of new ground-based astronomical instrumentation and of innovative data analysis methods: The study of Sun-like stars with substellar companions using CORALIE radial velocities and HIPPARCOS astrometry leads to the determination of the frequency of close brown dwarf companions and to the discovery of a dividing line between massive planets and brown dwarf companions; An observation campaign employing optical imaging with a very large telescope demonstrates sufficient astrometric <span class="hlt">precision</span> to detect planets around <span class="hlt">ultra</span>-cool dwarf stars and the first results of the survey are presented; Finally, the design and initial astrometric performance of PRIMA, ! a new dual-feed near-infrared interferometric observing facility for relative astrometry is presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10377E..0KZ','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10377E..0KZ"><span><span class="hlt">High-precision</span> laser microcutting and laser microdrilling using diffractive beam-splitting and <span class="hlt">high-precision</span> flexible beam alignment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zibner, F.; Fornaroli, C.; Holtkamp, J.; Shachaf, Lior; Kaplan, Natan; Gillner, A.</p> <p>2017-08-01</p> <p><span class="hlt">High-precision</span> laser micro machining gains more importance in industrial applications every month. Optical systems like the helical optics offer highest quality together with controllable and adjustable drilling geometry, thus as taper angle, aspect ratio and heat effected zone. The helical optics is based on a rotating Dove-prism which is mounted in a hollow shaft engine together with other optical elements like wedge prisms and plane plates. Although the achieved quality can be interpreted as extremely <span class="hlt">high</span> the low process efficiency is a main reason that this manufacturing technology has only limited demand within the industrial market. The objective of the research studies presented in this paper is to dramatically increase process efficiency as well as process flexibility. During the last years, the average power of commercial <span class="hlt">ultra</span>-short pulsed laser sources has increased significantly. The efficient utilization of the <span class="hlt">high</span> average laser power in the field of material processing requires an effective distribution of the laser power onto the work piece. One approach to increase the efficiency is the application of beam splitting devices to enable parallel processing. Multi beam processing is used to parallelize the fabrication of periodic structures as most application only require a partial amount of the emitted <span class="hlt">ultra</span>-short pulsed laser power. In order to achieve highest flexibility while using multi beam processing the single beams are diverted and re-guided in a way that enables the opportunity to process with each partial beam on locally apart probes or semimanufactures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ITNS...63.2617W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ITNS...63.2617W"><span>A 3.9 ps Time-Interval RMS <span class="hlt">Precision</span> Time-to-Digital Converter Using a Dual-Sampling Method in an <span class="hlt">Ultra</span>Scale FPGA</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Yonggang; Liu, Chong</p> <p>2016-10-01</p> <p>Field programmable gate arrays (FPGAs) manufactured with more advanced processing technology have faster carry chains and smaller delay elements, which are favorable for the design of tapped delay line (TDL)-style time-to-digital converters (TDCs) in FPGA. However, new challenges are posed in using them to implement TDCs with a <span class="hlt">high</span> time <span class="hlt">precision</span>. In this paper, we propose a bin realignment method and a dual-sampling method for TDC implementation in a Xilinx <span class="hlt">Ultra</span>Scale FPGA. The former realigns the disordered time delay taps so that the TDC <span class="hlt">precision</span> can approach the limit of its delay granularity, while the latter doubles the number of taps in the delay line so that the TDC <span class="hlt">precision</span> beyond the cell delay limitation can be expected. Two TDC channels were implemented in a Kintex <span class="hlt">Ultra</span>Scale FPGA, and the effectiveness of the new methods was evaluated. For fixed time intervals in the range from 0 to 440 ns, the average RMS <span class="hlt">precision</span> measured by the two TDC channels reaches 5.8 ps using the bin realignment, and it further improves to 3.9 ps by using the dual-sampling method. The time <span class="hlt">precision</span> has a 5.6% variation in the measured temperature range. Every part of the TDC, including dual-sampling, encoding, and on-line calibration, could run at a 500 MHz clock frequency. The system measurement dead time is only 4 ns.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AIPC..984..162S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AIPC..984..162S"><span>Development and use of an L3<span class="hlt">CCD</span> <span class="hlt">high</span>-cadence imaging system for Optical Astronomy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sheehan, Brendan J.; Butler, Raymond F.</p> <p>2008-02-01</p> <p>A <span class="hlt">high</span> cadence imaging system, based on a Low Light Level <span class="hlt">CCD</span> (L3<span class="hlt">CCD</span>) camera, has been developed for photometric and polarimetric applications. The camera system is an iXon DV-887 from Andor Technology, which uses a <span class="hlt">CCD</span>97 L3<span class="hlt">CCD</span> detector from E2V technologies. This is a back illuminated device, giving it an extended blue response, and has an active area of 512×512 pixels. The camera system allows frame-rates ranging from 30 fps (full frame) to 425 fps (windowed & binned frame). We outline the system design, concentrating on the calibration and control of the L3<span class="hlt">CCD</span> camera. The L3<span class="hlt">CCD</span> detector can be either triggered directly by a GPS timeserver/frequency generator or be internally triggered. A central PC remotely controls the camera computer system and timeserver. The data is saved as standard `FITS' files. The large data loads associated with <span class="hlt">high</span> frame rates, leads to issues with gathering and storing the data effectively. To overcome such problems, a specific data management approach is used, and a Python/PYRAF data reduction pipeline was written for the Linux environment. This uses calibration data collected either on-site, or from lab based measurements, and enables a fast and reliable method for reducing images. To date, the system has been used twice on the 1.5 m Cassini Telescope in Loiano (Italy) we present the reduction methods and observations made.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JDSO...12...39M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JDSO...12...39M"><span><span class="hlt">CCD</span> Astrometry of the Four Components of STF 1088</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Martin, Stuart; Daclison, Linsey; Ramos, Cathrina; Castaneda, Diana; Genet, Russell; Mohanan, Kakkala; Carro, Joseph M.</p> <p>2016-01-01</p> <p>Fifty <span class="hlt">CCD</span> astrometric measurements were made of the separations and position angles of the AB, AC, AD, and AE components of STF 1088. Longer integration times provided more stars in the astrometric solution which may have significantly improved the <span class="hlt">precision</span> of the measurements. The <span class="hlt">precision</span> of the measurements did not appear to be a function of component separation, although the smallest separation (that of STF 1088 AB) was only 11".</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SPIE.7654E..0KR','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SPIE.7654E..0KR"><span>Design and control of the <span class="hlt">precise</span> tracking bed based on complex electromechanical design theory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ren, Changzhi; Liu, Zhao; Wu, Liao; Chen, Ken</p> <p>2010-05-01</p> <p>The <span class="hlt">precise</span> tracking technology is wide used in astronomical instruments, satellite tracking and aeronautic test bed. However, the <span class="hlt">precise</span> <span class="hlt">ultra</span> low speed tracking drive system is one <span class="hlt">high</span> integrated electromechanical system, which one complexly electromechanical design method is adopted to improve the efficiency, reliability and quality of the system during the design and manufacture circle. The <span class="hlt">precise</span> Tracking Bed is one <span class="hlt">ultra</span>-exact, <span class="hlt">ultra</span>-low speed, <span class="hlt">high</span> <span class="hlt">precision</span> and huge inertial instrument, which some kind of mechanism and environment of the <span class="hlt">ultra</span> low speed is different from general technology. This paper explores the design process based on complex electromechanical optimizing design theory, one non-PID with a CMAC forward feedback control method is used in the servo system of the <span class="hlt">precise</span> tracking bed and some simulation results are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013SPIE.8884E..0QB','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013SPIE.8884E..0QB"><span>Efficient machining of <span class="hlt">ultra</span> <span class="hlt">precise</span> steel moulds with freeform surfaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bulla, B.; Robertson, D. J.; Dambon, O.; Klocke, F.</p> <p>2013-09-01</p> <p><span class="hlt">Ultra</span> <span class="hlt">precision</span> diamond turning of hardened steel to produce optical quality surfaces can be realized by applying an ultrasonic assisted process. With this technology optical moulds used typically for injection moulding can be machined directly from steel without the requirement to overcoat the mould with a diamond machinable material such as Nickel Phosphor. This has both the advantage of increasing the mould tool lifetime and also reducing manufacture costs by dispensing with the relatively expensive plating process. This publication will present results we have obtained for generating free form moulds in hardened steel by means of ultrasonic assisted diamond turning with a vibration frequency of 80 kHz. To provide a baseline with which to characterize the system performance we perform plane cutting experiments on different steel alloys with different compositions. The baseline machining results provides us information on the surface roughness and on tool wear caused during machining and we relate these to material composition. Moving on to freeform surfaces, we will present a theoretical background to define the machine program parameters for generating free forms by applying slow slide servo machining techniques. A solution for optimal part generation is introduced which forms the basis for the freeform machining experiments. The entire process chain, from the raw material through to <span class="hlt">ultra</span> <span class="hlt">precision</span> machining is presented, with emphasis on maintaining surface alignment when moving a component from CNC pre-machining to final machining using ultrasonic assisted diamond turning. The free form moulds are qualified on the basis of the surface roughness measurements and a form error map comparing the machined surface with the originally defined surface. These experiments demonstrate the feasibility of efficient free form machining applying ultrasonic assisted diamond turning of hardened steel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22938339','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22938339"><span><span class="hlt">Ultra-precise</span> tracking control of piezoelectric actuators via a fuzzy hysteresis model.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Pengzhi; Yan, Feng; Ge, Chuan; Zhang, Mingchao</p> <p>2012-08-01</p> <p>In this paper, a novel Takagi-Sugeno (T-S) fuzzy system based model is proposed for hysteresis in piezoelectric actuators. The antecedent and consequent structures of the fuzzy hysteresis model (FHM) can be, respectively, identified on-line through uniform partition approach and recursive least squares (RLS) algorithm. With respect to controller design, the inverse of FHM is used to develop a feedforward controller to cancel out the hysteresis effect. Then a hybrid controller is designed for <span class="hlt">high</span>-performance tracking. It combines the feedforward controller with a proportional integral differential (PID) controller favourable for stabilization and disturbance compensation. To achieve nanometer-scale tracking <span class="hlt">precision</span>, the enhanced adaptive hybrid controller is further developed. It uses real-time input and output data to update FHM, thus changing the feedforward controller to suit the on-site hysteresis character of the piezoelectric actuator. Finally, as to 3 cases of 50 Hz sinusoidal, multiple frequency sinusoidal and 50 Hz triangular trajectories tracking, experimental results demonstrate the efficiency of the proposed controllers. Especially, being only 0.35% of the maximum desired displacement, the maximum error of 50 Hz sinusoidal tracking is greatly reduced to 5.8 nm, which clearly shows the <span class="hlt">ultra-precise</span> nanometer-scale tracking performance of the developed adaptive hybrid controller.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/984640','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/984640"><span>Measuring the Flatness of Focal Plane for Very Large Mosaic <span class="hlt">CCD</span> Camera</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>Hao, Jiangang; Estrada, Juan; Cease, Herman</p> <p>2010-06-08</p> <p>Large mosaic multi<span class="hlt">CCD</span> camera is the key instrument for modern digital sky survey. DECam is an extremely red sensitive 520 Megapixel camera designed for the incoming Dark Energy Survey (DES). It is consist of sixty two 4k x 2k and twelve 2k x 2k 250-micron thick fully-depleted CCDs, with a focal plane of 44 cm in diameter and a field of view of 2.2 square degree. It will be attached to the Blanco 4-meter telescope at CTIO. The DES will cover 5000 square-degrees of the southern galactic cap in 5 color bands (g, r, i, z, Y) in 5 yearsmore » starting from 2011. To achieve the science goal of constraining the Dark Energy evolution, stringent requirements are laid down for the design of DECam. Among them, the flatness of the focal plane needs to be controlled within a 60-micron envelope in order to achieve the specified PSF variation limit. It is very challenging to measure the flatness of the focal plane to such <span class="hlt">precision</span> when it is placed in a <span class="hlt">high</span> vacuum dewar at 173 K. We developed two image based techniques to measure the flatness of the focal plane. By imaging a regular grid of dots on the focal plane, the <span class="hlt">CCD</span> offset along the optical axis is converted to the variation the grid spacings at different positions on the focal plane. After extracting the patterns and comparing the change in spacings, we can measure the flatness to <span class="hlt">high</span> <span class="hlt">precision</span>. In method 1, the regular dots are kept in <span class="hlt">high</span> sub micron <span class="hlt">precision</span> and cover the whole focal plane. In method 2, no <span class="hlt">high</span> <span class="hlt">precision</span> for the grid is required. Instead, we use a <span class="hlt">precise</span> XY stage moves the pattern across the whole focal plane and comparing the variations of the spacing when it is imaged by different CCDs. Simulation and real measurements show that the two methods work very well for our purpose, and are in good agreement with the direct optical measurements.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001SPIE.4183..978T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001SPIE.4183..978T"><span><span class="hlt">High</span>-speed <span class="hlt">high</span>-resolution epifluorescence imaging system using <span class="hlt">CCD</span> sensor and digital storage for neurobiological research</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Takashima, Ichiro; Kajiwara, Riichi; Murano, Kiyo; Iijima, Toshio; Morinaka, Yasuhiro; Komobuchi, Hiroyoshi</p> <p>2001-04-01</p> <p>We have designed and built a <span class="hlt">high</span>-speed <span class="hlt">CCD</span> imaging system for monitoring neural activity in an exposed animal cortex stained with a voltage-sensitive dye. Two types of custom-made <span class="hlt">CCD</span> sensors were developed for this system. The type I chip has a resolution of 2664 (H) X 1200 (V) pixels and a wide imaging area of 28.1 X 13.8 mm, while the type II chip has 1776 X 1626 pixels and an active imaging area of 20.4 X 18.7 mm. The <span class="hlt">CCD</span> arrays were constructed with multiple output amplifiers in order to accelerate the readout rate. The two chips were divided into either 24 (I) or 16 (II) distinct areas that were driven in parallel. The parallel <span class="hlt">CCD</span> outputs were digitized by 12-bit A/D converters and then stored in the frame memory. The frame memory was constructed with synchronous DRAM modules, which provided a capacity of 128 MB per channel. On-chip and on-memory binning methods were incorporated into the system, e.g., this enabled us to capture 444 X 200 pixel-images for periods of 36 seconds at a rate of 500 frames/second. This system was successfully used to visualize neural activity in the cortices of rats, guinea pigs, and monkeys.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22356226-crystallization-terminal-domain-addiction-antidote-ccda-complex-its-toxin-ccdb','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22356226-crystallization-terminal-domain-addiction-antidote-ccda-complex-its-toxin-ccdb"><span>Crystallization of the C-terminal domain of the addiction antidote <span class="hlt">Ccd</span>A in complex with its toxin <span class="hlt">Ccd</span>B</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>Buts, Lieven; De Jonge, Natalie; Loris, Remy, E-mail: reloris@vub.ac.be</p> <p>2005-10-01</p> <p>The <span class="hlt">Ccd</span>A C-terminal domain was crystallized in complex with <span class="hlt">Ccd</span>B in two crystal forms that diffract to beyond 2.0 Å resolution. <span class="hlt">Ccd</span>A and <span class="hlt">Ccd</span>B are the antidote and toxin of the <span class="hlt">ccd</span> addiction module of Escherichia coli plasmid F. The <span class="hlt">Ccd</span>A C-terminal domain (<span class="hlt">Ccd</span>A{sub C36}; 36 amino acids) was crystallized in complex with <span class="hlt">Ccd</span>B (dimer of 2 × 101 amino acids) in three different crystal forms, two of which diffract to <span class="hlt">high</span> resolution. Form II belongs to space group P2{sub 1}2{sub 1}2{sub 1}, with unit-cell parameters a = 37.6, b = 60.5, c = 83.8 Å and diffracts to 1.8more » Å resolution. Form III belongs to space group P2{sub 1}, with unit-cell parameters a = 41.0, b = 37.9, c = 69.6 Å, β = 96.9°, and diffracts to 1.9 Å resolution.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001StarC...6.....P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001StarC...6.....P"><span>The <span class="hlt">CCD</span> Photometric Calibration Cookbook</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Palmer, J.; Davenhall, A. C.</p> <p></p> <p>This cookbook presents simple recipes for the photometric calibration of <span class="hlt">CCD</span> frames. Using these recipes you can calibrate the brightness of objects measured in <span class="hlt">CCD</span> frames into magnitudes in standard photometric systems, such as the Johnson-Morgan UBV, system. The recipes use standard software available at all Starlink sites. The topics covered include: selecting standard stars, measuring instrumental magnitudes and calibrating instrumental magnitudes into a standard system. The recipes are appropriate for use with data acquired with optical CCDs and filters, operated in standard ways, and describe the usual calibration technique of observing standard stars. The software is robust and reliable, but the techniques are usually not suitable where very <span class="hlt">high</span> accuracy is required. In addition to the recipes and scripts, sufficient background material is presented to explain the procedures and techniques used. The treatment is deliberately practical rather than theoretical, in keeping with the aim of providing advice on the actual calibration of observations. This cookbook is aimed firmly at people who are new to astronomical photometry. Typical readers might have a set of photometric observations to reduce (perhaps observed by a colleague) or be planning a programme of photometric observations, perhaps for the first time. No prior knowledge of astronomical photometry is assumed. The cookbook is not aimed at experts in astronomical photometry. Many finer points are omitted for clarity and brevity. Also, in order to make the most accurate possible calibration of <span class="hlt">high-precision</span> photometry, it is usually necessary to use bespoke software tailored to the observing programme and photometric system you are using.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006NIMPA.565..157S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006NIMPA.565..157S"><span><span class="hlt">CCD</span> developments for particle colliders</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stefanov, Konstantin D.</p> <p>2006-09-01</p> <p>Charge Coupled Devices (CCDs) have been successfully used in several <span class="hlt">high</span>-energy physics experiments over the last 20 years. Their small pixel size and excellent <span class="hlt">precision</span> provide superb tool for studying of short-lived particles and understanding the nature at fundamental level. Over the last years the Linear Collider Flavour Identification (LCFI) collaboration has developed Column-Parallel CCDs (CPCCD) and CMOS readout chips to be used for the vertex detector at the International Linear Collider (ILC). The CPCCDs are very fast devices capable of satisfying the challenging requirements imposed by the beam structure of the superconducting accelerator. First set of prototype devices have been designed, manufactured and successfully tested, with second-generation chips on the way. Another idea for <span class="hlt">CCD</span>-based device, the In-situ Storage Image Sensor (ISIS) is also under development and the first prototype is in production.</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_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li class="active"><span>5</span></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_5 --> <div id="page_6" 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_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</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="101"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGeod.tmp..461L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGeod.tmp..461L"><span>Improving multi-GNSS <span class="hlt">ultra</span>-rapid orbit determination for real-time <span class="hlt">precise</span> point positioning</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Xingxing; Chen, Xinghan; Ge, Maorong; Schuh, Harald</p> <p>2018-03-01</p> <p>Currently, with the rapid development of multi-constellation Global Navigation Satellite Systems (GNSS), the real-time positioning and navigation are undergoing dramatic changes with potential for a better performance. To provide more <span class="hlt">precise</span> and reliable <span class="hlt">ultra</span>-rapid orbits is critical for multi-GNSS real-time positioning, especially for the three merging constellations Beidou, Galileo and QZSS which are still under construction. In this contribution, we present a five-system <span class="hlt">precise</span> orbit determination (POD) strategy to fully exploit the GPS + GLONASS + BDS + Galileo + QZSS observations from CDDIS + IGN + BKG archives for the realization of hourly five-constellation <span class="hlt">ultra</span>-rapid orbit update. After adopting the optimized 2-day POD solution (updated every hour), the predicted orbit accuracy can be obviously improved for all the five satellite systems in comparison to the conventional 1-day POD solution (updated every 3 h). The orbit accuracy for the BDS IGSO satellites can be improved by about 80, 45 and 50% in the radial, cross and along directions, respectively, while the corresponding accuracy improvement for the BDS MEO satellites reaches about 50, 20 and 50% in the three directions, respectively. Furthermore, the multi-GNSS real-time <span class="hlt">precise</span> point positioning (PPP) ambiguity resolution has been performed by using the improved <span class="hlt">precise</span> satellite orbits. Numerous results indicate that combined GPS + BDS + GLONASS + Galileo (GCRE) kinematic PPP ambiguity resolution (AR) solutions can achieve the shortest time to first fix (TTFF) and highest positioning accuracy in all coordinate components. With the addition of the BDS, GLONASS and Galileo observations to the GPS-only processing, the GCRE PPP AR solution achieves the shortest average TTFF of 11 min with 7{°} cutoff elevation, while the TTFF of GPS-only, GR, GE and GC PPP AR solution is 28, 15, 20 and 17 min, respectively. As the cutoff elevation increases, the reliability and accuracy of GPS-only PPP AR solutions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008SPIE.6890E..0MH','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008SPIE.6890E..0MH"><span>Improvement in the light sensitivity of the ultrahigh-speed <span class="hlt">high</span>-sensitivity <span class="hlt">CCD</span> with a microlens array</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hayashida, T.,; Yonai, J.; Kitamura, K.; Arai, T.; Kurita, T.; Tanioka, K.; Maruyama, H.; Etoh, T. Goji; Kitagawa, S.; Hatade, K.; Yamaguchi, T.; Takeuchi, H.; Iida, K.</p> <p>2008-02-01</p> <p>We are advancing the development of ultrahigh-speed, <span class="hlt">high</span>-sensitivity CCDs for broadcast use that are capable of capturing smooth slow-motion videos in vivid colors even where lighting is limited, such as at professional baseball games played at night. We have already developed a 300,000 pixel, ultrahigh-speed <span class="hlt">CCD</span>, and a single <span class="hlt">CCD</span> color camera that has been used for sports broadcasts and science programs using this <span class="hlt">CCD</span>. However, there are cases where even higher sensitivity is required, such as when using a telephoto lens during a baseball broadcast or a <span class="hlt">high</span>-magnification microscope during science programs. This paper provides a summary of our experimental development aimed at further increasing the sensitivity of CCDs using the light-collecting effects of a microlens array.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9912E..25K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9912E..25K"><span>Fabrication of a wide-field NIR integral field unit for SWIMS using <span class="hlt">ultra-precision</span> cutting</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kitagawa, Yutaro; Yamagata, Yutaka; Morita, Shin-ya; Motohara, Kentaro; Ozaki, Shinobu; Takahashi, Hidenori; Konishi, Masahiro; Kato, Natsuko M.; Kobayakawa, Yutaka; Terao, Yasunori; Ohashi, Hirofumi</p> <p>2016-07-01</p> <p>We describe overview of fabrication methods and measurement results of test fabrications of optical surfaces for an integral field unit (IFU) for Simultaneous color Wide-field Infrared Multi-object Spectrograph, SWIMS, which is a first-generation instrument for the University of Tokyo Atacama Observatory 6.5-m telescope. SWIMS-IFU provides entire near-infrared spectrum from 0.9 to 2.5 μm simultaneously covering wider field of view of 17" × 13" compared with current near-infrared IFUs. We investigate an <span class="hlt">ultra-precision</span> cutting technique to monolithically fabricate optical surfaces of IFU optics such as an image slicer. Using 4- or 5-axis <span class="hlt">ultra</span> <span class="hlt">precision</span> machine we compare the milling process and shaper cutting process to find the best way of fabrication of image slicers. The measurement results show that the surface roughness almost satisfies our requirement in both of two methods. Moreover, we also obtain ideal surface form in the shaper cutting process. This method will be adopted to other mirror arrays (i.e. pupil mirror and slit mirror, and such monolithic fabrications will also help us to considerably reduce alignment procedure of each optical elements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SPIE.7850E..07X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SPIE.7850E..07X"><span>A configurable distributed <span class="hlt">high</span>-performance computing framework for satellite's TDI-<span class="hlt">CCD</span> imaging simulation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xue, Bo; Mao, Bingjing; Chen, Xiaomei; Ni, Guoqiang</p> <p>2010-11-01</p> <p>This paper renders a configurable distributed <span class="hlt">high</span> performance computing(HPC) framework for TDI-<span class="hlt">CCD</span> imaging simulation. It uses strategy pattern to adapt multi-algorithms. Thus, this framework help to decrease the simulation time with low expense. Imaging simulation for TDI-<span class="hlt">CCD</span> mounted on satellite contains four processes: 1) atmosphere leads degradation, 2) optical system leads degradation, 3) electronic system of TDI-<span class="hlt">CCD</span> leads degradation and re-sampling process, 4) data integration. Process 1) to 3) utilize diversity data-intensity algorithms such as FFT, convolution and LaGrange Interpol etc., which requires powerful CPU. Even uses Intel Xeon X5550 processor, regular series process method takes more than 30 hours for a simulation whose result image size is 1500 * 1462. With literature study, there isn't any mature distributing HPC framework in this field. Here we developed a distribute computing framework for TDI-<span class="hlt">CCD</span> imaging simulation, which is based on WCF[1], uses Client/Server (C/S) layer and invokes the free CPU resources in LAN. The server pushes the process 1) to 3) tasks to those free computing capacity. Ultimately we rendered the HPC in low cost. In the computing experiment with 4 symmetric nodes and 1 server , this framework reduced about 74% simulation time. Adding more asymmetric nodes to the computing network, the time decreased namely. In conclusion, this framework could provide unlimited computation capacity in condition that the network and task management server are affordable. And this is the brand new HPC solution for TDI-<span class="hlt">CCD</span> imaging simulation and similar applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..210a2056T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..210a2056T"><span>Practical controller design for <span class="hlt">ultra-precision</span> positioning of stages with a pneumatic artificial muscle actuator</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tang, T. F.; Chong, S. H.</p> <p>2017-06-01</p> <p>This paper presents a practical controller design method for <span class="hlt">ultra-precision</span> positioning of pneumatic artificial muscle actuator stages. Pneumatic artificial muscle (PAM) actuators are safe to use and have numerous advantages which have brought these actuators to wide applications. However, PAM exhibits strong non-linear characteristics, and these limitations lead to low controllability and limit its application. In practice, the non-linear characteristics of PAM mechanism are difficult to be <span class="hlt">precisely</span> modeled, and time consuming to model them accurately. The purpose of the present study is to clarify a practical controller design method that emphasizes a simple design procedure that does not acquire plants parameters modeling, and yet is able to demonstrate <span class="hlt">ultra-precision</span> positioning performance for a PAM driven stage. The practical control approach adopts continuous motion nominal characteristic trajectory following (CM NCTF) control as the feedback controller. The constructed PAM driven stage is in low damping characteristic and causes severe residual vibration that deteriorates motion accuracy of the system. Therefore, the idea to increase the damping characteristic by having an acceleration feedback compensation to the plant has been proposed. The effectiveness of the proposed controller was verified experimentally and compared with a classical PI controller in point-to-point motion. The experiment results proved that the CM NCTF controller demonstrates better positioning performance in smaller motion error than the PI controller. Overall, the CM NCTF controller has successfully to reduce motion error to 3µm, which is 88.7% smaller than the PI controller.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10565E..03W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10565E..03W"><span>Systems approach to the design of the <span class="hlt">CCD</span> sensors and camera electronics for the AIA and HMI instruments on solar dynamics observatory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Waltham, N.; Beardsley, S.; Clapp, M.; Lang, J.; Jerram, P.; Pool, P.; Auker, G.; Morris, D.; Duncan, D.</p> <p>2017-11-01</p> <p>Solar Dynamics Observatory (SDO) is imaging the Sun in many wavelengths near simultaneously and with a resolution ten times higher than the average <span class="hlt">high</span>-definition television. In this paper we describe our innovative systems approach to the design of the <span class="hlt">CCD</span> cameras for two of SDO's remote sensing instruments, the Atmospheric Imaging Assembly (AIA) and the Helioseismic and Magnetic Imager (HMI). Both instruments share use of a custom-designed 16 million pixel science-grade <span class="hlt">CCD</span> and common camera readout electronics. A prime requirement was for the <span class="hlt">CCD</span> to operate with significantly lower drive voltages than before, motivated by our wish to simplify the design of the camera readout electronics. Here, the challenge lies in the design of circuitry to drive the <span class="hlt">CCD</span>'s <span class="hlt">highly</span> capacitive electrodes and to digitize its analogue video output signal with low noise and to <span class="hlt">high</span> <span class="hlt">precision</span>. The challenge is greatly exacerbated when forced to work with only fully space-qualified, radiation-tolerant components. We describe our systems approach to the design of the AIA and HMI <span class="hlt">CCD</span> and camera electronics, and the engineering solutions that enabled us to comply with both mission and instrument science requirements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9281E..05Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9281E..05Z"><span>Diamond tool wear detection method using cutting force and its power spectrum analysis in <span class="hlt">ultra-precision</span> fly cutting</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, G. Q.; To, S.</p> <p>2014-08-01</p> <p>Cutting force and its power spectrum analysis was thought to be an effective method monitoring tool wear in many cutting processes and a significant body of research has been conducted on this research area. However, relative little similar research was found in <span class="hlt">ultra-precision</span> fly cutting. In this paper, a group of experiments were carried out to investigate the cutting forces and its power spectrum characteristics under different tool wear stages. Result reveals that the cutting force increases with the progress of tool wear. The cutting force signals under different tool wear stages were analyzed using power spectrum analysis. The analysis indicates that a characteristic frequency does exist in the power spectrum of the cutting force, whose power spectral density increases with the increasing of tool wear level, this characteristic frequency could be adopted to monitor diamond tool wear in <span class="hlt">ultra-precision</span> fly cutting.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005jsrs.meet..242Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005jsrs.meet..242Y"><span>A FORTRAN version implementation of block adjustment of <span class="hlt">CCD</span> frames and its preliminary application</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yu, Y.; Tang, Z.-H.; Li, J.-L.; Zhao, M.</p> <p>2005-09-01</p> <p>A FORTRAN version implementation of the block adjustment (BA) of overlapping <span class="hlt">CCD</span> frames is developed and its flowchart is shown. The program is preliminarily applied to obtain the optical positions of four extragalactic radio sources. The results show that because of the increase in the number and sky coverage of reference stars the <span class="hlt">precision</span> of optical positions with BA is improved compared with the single <span class="hlt">CCD</span> frame adjustment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19770010346&hterms=inverse+multiplication&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dinverse%2Bmultiplication','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19770010346&hterms=inverse+multiplication&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dinverse%2Bmultiplication"><span><span class="hlt">CCD</span> correlation techniques</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hewes, C. R.; Bosshart, P. W.; Eversole, W. L.; Dewit, M.; Buss, D. D.</p> <p>1976-01-01</p> <p>Two <span class="hlt">CCD</span> techniques were discussed for performing an N-point sampled data correlation between an input signal and an electronically programmable reference function. The design and experimental performance of an implementation of the direct time correlator utilizing two analog CCDs and MOS multipliers on a single IC were evaluated. The performance of a <span class="hlt">CCD</span> implementation of the chirp z transform was described, and the design of a new <span class="hlt">CCD</span> integrated circuit for performing correlation by multiplication in the frequency domain was presented. This chip provides a discrete Fourier transform (DFT) or inverse DFT, multipliers, and complete support circuitry for the <span class="hlt">CCD</span> CZT. The two correlation techniques are compared.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006SPIE.6159E..0JU','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006SPIE.6159E..0JU"><span>Toolkit for testing scientific <span class="hlt">CCD</span> cameras</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Uzycki, Janusz; Mankiewicz, Lech; Molak, Marcin; Wrochna, Grzegorz</p> <p>2006-03-01</p> <p>The <span class="hlt">CCD</span> Toolkit (1) is a software tool for testing <span class="hlt">CCD</span> cameras which allows to measure important characteristics of a camera like readout noise, total gain, dark current, 'hot' pixels, useful area, etc. The application makes a statistical analysis of images saved in files with FITS format, commonly used in astronomy. A graphical interface is based on the ROOT package, which offers <span class="hlt">high</span> functionality and flexibility. The program was developed in a way to ensure future compatibility with different operating systems: Windows and Linux. The <span class="hlt">CCD</span> Toolkit was created for the "Pie of the Sky" project collaboration (2).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006NIMPA.569...48S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006NIMPA.569...48S"><span><span class="hlt">CCD</span>-based vertex detector for ILC</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stefanov, Konstantin D.</p> <p>2006-12-01</p> <p>Charge Coupled Devices (CCDs) have been successfully used in several <span class="hlt">high</span>-energy physics experiments over the last 20 years. Their small pixel size and excellent <span class="hlt">precision</span> provide a superb tool for studying of short-lived particles and understanding the nature at fundamental level. Over the last few years the Linear Collider Flavour Identification (LCFI) collaboration has developed Column-Parallel CCDs (CPCCD) and CMOS readout chips, to be used for the vertex detector at the International Linear Collider (ILC). The CPCCDs are very fast devices capable of satisfying the challenging requirements imposed by the beam structure of the superconducting accelerator. The first set of prototype devices have been successfully designed, manufactured and tested, with second generation chips on the way. Another idea for <span class="hlt">CCD</span>-based device, the In-situ Storage Image Sensor (ISIS) is also under development and the first prototype has been manufactured.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996SPIE.2654..259S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996SPIE.2654..259S"><span><span class="hlt">High</span>-performance dual-speed <span class="hlt">CCD</span> camera system for scientific imaging</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Simpson, Raymond W.</p> <p>1996-03-01</p> <p>Traditionally, scientific camera systems were partitioned with a `camera head' containing the <span class="hlt">CCD</span> and its support circuitry and a camera controller, which provided analog to digital conversion, timing, control, computer interfacing, and power. A new, unitized <span class="hlt">high</span> performance scientific <span class="hlt">CCD</span> camera with dual speed readout at 1 X 106 or 5 X 106 pixels per second, 12 bit digital gray scale, <span class="hlt">high</span> performance thermoelectric cooling, and built in composite video output is described. This camera provides all digital, analog, and cooling functions in a single compact unit. The new system incorporates the A/C converter, timing, control and computer interfacing in the camera, with the power supply remaining a separate remote unit. A 100 Mbyte/second serial link transfers data over copper or fiber media to a variety of host computers, including Sun, SGI, SCSI, PCI, EISA, and Apple Macintosh. Having all the digital and analog functions in the camera made it possible to modify this system for the Woods Hole Oceanographic Institution for use on a remote controlled submersible vehicle. The oceanographic version achieves 16 bit dynamic range at 1.5 X 105 pixels/second, can be operated at depths of 3 kilometers, and transfers data to the surface via a real time fiber optic link.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29500386','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29500386"><span>Ductile and brittle transition behavior of titanium alloys in <span class="hlt">ultra-precision</span> machining.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yip, W S; To, S</p> <p>2018-03-02</p> <p>Titanium alloys are extensively applied in biomedical industries due to their excellent material properties. However, they are recognized as difficult to cut materials due to their low thermal conductivity, which induces a complexity to their deformation mechanisms and restricts <span class="hlt">precise</span> productions. This paper presents a new observation about the removal regime of titanium alloys. The experimental results, including the chip formation, thrust force signal and surface profile, showed that there was a critical cutting distance to achieve better surface integrity of machined surface. The machined areas with better surface roughness were located before the clear transition point, defining as the ductile to brittle transition. The machined area at the brittle region displayed the fracture deformation which showed cracks on the surface edge. The relationship between depth of cut and the ductile to brittle transaction behavior of titanium alloys in <span class="hlt">ultra-precision</span> machining(UPM) was also revealed in this study, it showed that the ductile to brittle transaction behavior of titanium alloys occurred mainly at relatively small depth of cut. The study firstly defines the ductile to brittle transition behavior of titanium alloys in UPM, contributing the information of ductile machining as an optimal machining condition for <span class="hlt">precise</span> productions of titanium alloys.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9158E..0BW','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9158E..0BW"><span>Comparative analysis of data quality and applications in vegetation of HJ-1A <span class="hlt">CCD</span> images</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wei, Hongwei; Tian, Qingjiu; Huang, Yan; Wang, Yan</p> <p>2014-05-01</p> <p>To study the data quality and to find the differences in vegetation monitoring applications, the same region at Chuzhou Lai 'an, the data of HJ-1A <span class="hlt">CCD</span>1 on the April 1st, 2012 and the data of HJ-1A <span class="hlt">CCD</span>2 on the March 31, 2012 have being comparative analysis by the method of objective quality (image)assessment which selecting over five spectral image evaluation parameters: radiation <span class="hlt">precision</span> (mean, variance, inclination, steepness), information entropy, signal-to-noise ratio, sharpness, contrast, and normalized differential vegetation index. The results show that there is little differences between the HJ-1A <span class="hlt">CCD</span>1 and <span class="hlt">CCD</span>2 by objective evaluation of data quality except radiation <span class="hlt">precision</span> conform to their design theory, so the conclusion is that the difference of them without considering on the usual unless continuation;and Combination of field observation data Lai'an spectral data and GPS data (each point),selecting the normalized difference vegetation index as <span class="hlt">CCD</span>1, <span class="hlt">CCD</span>2 in vegetation monitoring application on the evaluation of the differences, and the specific process is based on GPS data is divided into nine small plots of spectral data ,and image data of nine one-to-one correspondence plots, and their normalized difference vegetation index values were calculated ,and measured spectra data resampling HJ-1A <span class="hlt">CCD</span>1, <span class="hlt">CCD</span>2 spectral response function calculated NDVI, and the results show that there is little differences between the HJ-1A <span class="hlt">CCD</span>1 and <span class="hlt">CCD</span>2 by objective evaluation of data quality, and, the differences of wheat `s reflection and normalized vegetation index is mainly due to calibration coefficients of <span class="hlt">CCD</span>1 and <span class="hlt">CCD</span>2, the differences of the solar elevation angle when obtaining the image and atmospheric conditions, so it has to consider the performance indicators as well as access conditions of <span class="hlt">CCD</span>1 and <span class="hlt">CCD</span>2, and to be take the normalization techniques for processing for the comparison analysis in the use of HJ-1A <span class="hlt">CCD</span> Data to surface dynamic changes; Finally, in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997SPIE.2869.1094Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997SPIE.2869.1094Z"><span><span class="hlt">CCD</span> <span class="hlt">high</span>-speed videography system with new concepts and techniques</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zheng, Zengrong; Zhao, Wenyi; Wu, Zhiqiang</p> <p>1997-05-01</p> <p>A novel <span class="hlt">CCD</span> <span class="hlt">high</span> speed videography system with brand-new concepts and techniques is developed by Zhejiang University recently. The system can send a series of short flash pulses to the moving object. All of the parameters, such as flash numbers, flash durations, flash intervals, flash intensities and flash colors, can be controlled according to needs by the computer. A series of moving object images frozen by flash pulses, carried information of moving object, are recorded by a <span class="hlt">CCD</span> video camera, and result images are sent to a computer to be frozen, recognized and processed with special hardware and software. Obtained parameters can be displayed, output as remote controlling signals or written into CD. The highest videography frequency is 30,000 images per second. The shortest image freezing time is several microseconds. The system has been applied to wide fields of energy, chemistry, medicine, biological engineering, aero- dynamics, explosion, multi-phase flow, mechanics, vibration, athletic training, weapon development and national defense engineering. It can also be used in production streamline to carry out the online, real-time monitoring and controlling.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997ESASP.402..121Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997ESASP.402..121Z"><span>Comparing the TYCHO Catalogue with <span class="hlt">CCD</span> Astrograph Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zacharias, N.; Hoeg, E.; Urban, S. E.; Corbin, T. E.</p> <p>1997-08-01</p> <p>Selected fields around radio-optical reference frame sources have been observed with the U.S. Naval Observatory <span class="hlt">CCD</span> astrograph (UCA). This telescope is equipped with a red-corrected 206mm 5-element lens and a 4k by 4k <span class="hlt">CCD</span> camera which provides a 1 square degree field of view. Positions with internal <span class="hlt">precisions</span> of 20 mas for stars in the 7 to 12 magnitude range have been obtained with 30 second exposures. A comparison is made with the Tycho Catalogue, which is accurate to about 5 to 50 mas at mean epoch of J1991.25, depending on the magnitude of the star. Preliminary proper motions are obtained using the Astrographic Catalogue (AC) to update the Tycho positions to the epoch of the UCA observations, which adds an error contribution of about 15 to 20 mas. Individual <span class="hlt">CCD</span> frames have been reduced with an average of 30 Tycho reference stars per frame. A linear plate model gives an average adjustment standard error of 46 mas, consistent with the internal errors. The UCA is capable of significantly improving the positions of Tycho stars fainter than about visual magnitude 9.5.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1175196','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1175196"><span>Method and system for <span class="hlt">ultra-precision</span> positioning</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Montesanti, Richard C.; Locke, Stanley F.; Thompson, Samuel L.</p> <p>2005-01-11</p> <p>An apparatus and method is disclosed for <span class="hlt">ultra-precision</span> positioning. A slide base provides a foundational support. A slide plate moves with respect to the slide base along a first geometric axis. Either a ball-screw or a piezoelectric actuator working separate or in conjunction displaces the slide plate with respect to the slide base along the first geometric axis. A linking device directs a primary force vector into a center-line of the ball-screw. The linking device consists of a first link which directs a first portion of the primary force vector to an apex point, located along the center-line of the ball-screw, and a second link for directing a second portion of the primary force vector to the apex point. A set of rails, oriented substantially parallel to the center-line of the ball-screw, direct movement of the slide plate with respect to the slide base along the first geometric axis and are positioned such that the apex point falls within a geometric plane formed by the rails. The slide base, the slide plate, the ball-screw, and the linking device together form a slide assembly. Multiple slide assemblies can be distributed about a platform. In such a configuration, the platform may be raised and lowered, or tipped and tilted by jointly or independently displacing the slide plates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1348215','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1348215"><span><span class="hlt">Precision</span> mechanical structure of an <span class="hlt">ultra-high</span>-resolution spectrometer for inelastic X-ray scattering instrument</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Shu, Deming; Shvydko, Yuri; Stoupin, Stanislav A.; Khachatryan, Ruben; Goetze, Kurt A.; Roberts, Timothy</p> <p>2015-04-14</p> <p>A method and an ultrahigh-resolution spectrometer including a <span class="hlt">precision</span> mechanical structure for positioning inelastic X-ray scattering optics are provided. The spectrometer includes an X-ray monochromator and an X-ray analyzer, each including X-ray optics of a collimating (C) crystal, a pair of dispersing (D) element crystals, anomalous transmission filter (F) and a wavelength (W) selector crystal. A respective <span class="hlt">precision</span> mechanical structure is provided with the X-ray monochromator and the X-ray analyzer. The <span class="hlt">precision</span> mechanical structure includes a base plate, such as an aluminum base plate; positioning stages for D-crystal alignment; positioning stages with an incline sensor for C/F/W-crystal alignment, and the positioning stages including flexure-based <span class="hlt">high</span>-stiffness structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-GRC-2015-C-04208.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-GRC-2015-C-04208.html"><span><span class="hlt">Ultra</span> <span class="hlt">High</span> Bypass Integrated System Test</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2015-09-14</p> <p>NASA’s Environmentally Responsible Aviation Project, in collaboration with the Federal Aviation Administration (FAA) and Pratt & Whitney, completed testing of an <span class="hlt">Ultra</span> <span class="hlt">High</span> Bypass Ratio Turbofan Model in the 9’ x 15’ Low Speed Wind Tunnel at NASA Glenn Research Center. The fan model is representative of the next generation of efficient and quiet <span class="hlt">Ultra</span> <span class="hlt">High</span> Bypass Ratio Turbofan Engine designs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005SPIE.5879..117N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005SPIE.5879..117N"><span>Low-cost <span class="hlt">precision</span> rotary index calibration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ng, T. W.; Lim, T. S.</p> <p>2005-08-01</p> <p>The traditional method for calibrating angular indexing repeatability of rotary axes on machine tools and measuring equipment is with a <span class="hlt">precision</span> polygon (usually 12 sided) and an autocollimator or angular interferometer. Such a setup is typically expensive. Here, we propose a far more cost-effective approach that uses just a laser, diffractive optical element, and <span class="hlt">CCD</span> camera. We show that significantly <span class="hlt">high</span> accuracies can be achieved for angular index calibration.</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_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_6 --> <div id="page_7" 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_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="121"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000AAS...196.5303G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000AAS...196.5303G"><span>The first US Naval Observatory <span class="hlt">CCD</span> Astrograph Catalog</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Germain, M. E.; Zacharias, N.; Urban, S. E.; Rafferty, T. J.; Holdenried, E. R.; Zacharias, M. I.; Hall, D. M.; Wycoff, G. L.; Monet, D. G.</p> <p>2000-05-01</p> <p>The USNO <span class="hlt">CCD</span> Astrograph Catalog (UCAC) project is a <span class="hlt">high</span> <span class="hlt">precision</span>, astrometric survey of stars having R magnitudes between 7th and 16th. The positional accuracy is 20 mas for stars between 9th and 14th, and 70 mas for fainter stars. This gives a density (stars per square degree) higher than that of the Guide Star Catalog (GSC), with an improvement in positional accuracy of about a factor of ten. Observations began in January 1998 at Cerro Tololo Inter--American Observatory (CTIO) using a five-element 0.2 meter astrograph equipped with a 4k by 4k <span class="hlt">CCD</span>. The instrument will be moved north in early 2001, and full sky coverage is expected by early 2003. A preliminary catalog (UCAC1) of positions and proper motions of 27 million stars has been constructed which is available on CD-ROM from USNO. Observations between 13 Feb 1998 and 07 Nov 1999 are included with a total of over 79,000 <span class="hlt">CCD</span> frames covering 80% of the Southern Hemisphere. The catalog is on the International Celestial Reference System (ICRS), which is consistent with J2000. Proper motions of bright stars (V <= 12.5) were derived using a combination of ground-based astrometric catalogs, Hipparcos, and Tycho-2 positions, giving a typical error of 3 mas/yr. For the fainter stars the USNO A2.0 (Monet, 1998) was used as first epoch, with typical proper motion errors of 10 to 15 mas/yr. External comparisons with Tycho-2 and the Yale Southern Proper Motion (SPM) 2.0 data reveal systematic errors to be only on the 10 mas level.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890048371&hterms=Programmable+Logic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DProgrammable%2BLogic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890048371&hterms=Programmable+Logic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DProgrammable%2BLogic"><span>A programmable <span class="hlt">CCD</span> driver circuit for multiphase <span class="hlt">CCD</span> operation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ewin, Audrey J.; Reed, Kenneth V.</p> <p>1989-01-01</p> <p>A programmable <span class="hlt">CCD</span> (charge-coupled device) driver circuit was designed to drive CCDs in multiphased modes. The purpose of the drive electronics is to operate developmental <span class="hlt">CCD</span> imaging arrays for NASA's tiltable moderate resolution imaging spectrometer (MODIS-T). Five objectives for the driver were considered during its design: (1) the circuit drives <span class="hlt">CCD</span> electrode voltages between 0 V and +30 V to produce reasonable potential wells, (2) the driving sequence is started with one input signal, (3) the driving sequence is started with one input signal, (4) the circuit allows programming of frame sequences required by arrays of any size, (5) it produces interfacing signals for the <span class="hlt">CCD</span> and the DTF (detector test facility). Simulation of the driver verified its function with the master clock running up to 10 MHz. This suggests a maximum rate of 400,000 pixels/s. Timing and packaging parameters were verified. The design uses 54 TTL (transistor-transistor logic) chips. Two versions of hardware were fabricated: wirewrap and printed circuit board. Both were verified functionally with a logic analyzer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29519053','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29519053"><span>Machining approach of freeform optics on infrared materials via <span class="hlt">ultra-precision</span> turning.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Zexiao; Fang, Fengzhou; Chen, Jinjin; Zhang, Xiaodong</p> <p>2017-02-06</p> <p>Optical freeform surfaces are of great advantage in excellent optical performance and integrated alignment features. It has wide applications in illumination, imaging and non-imaging, etc. Machining freeform surfaces on infrared (IR) materials with <span class="hlt">ultra-precision</span> finish is difficult due to its brittle nature. Fast tool servo (FTS) assisted diamond turning is a powerful technique for the realization of freeform optics on brittle materials due to its features of <span class="hlt">high</span> spindle speed and <span class="hlt">high</span> cutting speed. However it has difficulties with large slope angles and large rise-and-falls in the sagittal direction. In order to overcome this defect, the balance of the machining quality on the freeform surface and the brittle nature in IR materials should be realized. This paper presents the design of a near-rotational freeform surface (NRFS) with a low non-rotational degree (NRD) to constraint the variation of traditional freeform optics to solve this issue. In NRFS, the separation of the surface results in a rotational part and a residual part denoted as a non-rotational surface (NRS). Machining NRFS on germanium is operated by FTS diamond turning. Characteristics of the surface indicate that the optical finish of the freeform surface has been achieved. The modulation transfer function (MTF) of the freeform optics shows a good agreement to the design expectation. Images of the final optical system confirm that the fabricating strategy is of <span class="hlt">high</span> efficiency and <span class="hlt">high</span> quality. Challenges and prospects are discussed to provide guidance of future work.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25916793','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25916793"><span>Simultaneous determination of mushroom toxins α-amanitin, β-amanitin and muscarine in human urine by solid-phase extraction and <span class="hlt">ultra-high</span>-performance liquid chromatography coupled with <span class="hlt">ultra-high</span>-resolution TOF mass spectrometry.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tomková, Jana; Ondra, Peter; Válka, Ivo</p> <p>2015-06-01</p> <p>This paper presents a method for the simultaneous determination of α-amanitin, β-amanitin and muscarine in human urine by solid-phase extraction (SPE) and <span class="hlt">ultra-high</span>-performance liquid chromatography coupled with <span class="hlt">ultra-high</span>-resolution TOF mass spectrometry. The method can be used for a diagnostics of mushroom poisonings. Different SPE cartridges were tested for sample preparation, namely hydrophilic modified reversed-phase (Oasis HLB) and polymeric weak cation phase (Strata X-CW). The latter gave better results and therefore it was chosen for the subsequent method optimization and partial validation. In the course of validation, limits of detection, linearity, intraday and interday <span class="hlt">precisions</span> and recoveries were evaluated. The obtained LOD values of α-amanitin and β-amanitin were 1ng/mL and of muscarine 0.09ng/mL. The intraday and interday <span class="hlt">precisions</span> of human urine spiked with α-amanitin (10ng/mL), β-amanitin (10ng/mL) and muscarine (1ng/mL) ranged from 6% to 10% and from 7% to 13%, respectively. The developed method was proved to be a relevant tool for the simultaneous determination of the studied mushroom toxins in human urine after mushroom poisoning. Copyright © 2015 Elsevier Ireland Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080004993','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080004993"><span>Delta-doped <span class="hlt">CCD</span>'s as low-energy particle detectors and imagers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nikzad, Shouleh (Inventor); Hoenk, Michael E. (Inventor); Hecht, Michael H. (Inventor)</p> <p>2002-01-01</p> <p>The back surface of a thinned charged-coupled device (<span class="hlt">CCD</span>) is treated to eliminate the backside potential well that appears in a conventional thinned <span class="hlt">CCD</span> during backside illumination. The backside of the <span class="hlt">CCD</span> includes a delta layer of <span class="hlt">high</span>-concentration dopant confined to less than one monolayer of the crystal semiconductor. The thinned, delta-doped <span class="hlt">CCD</span> is used to detect very low-energy particles that penetrate less than 1.0 nm into the <span class="hlt">CCD</span>, including electrons having energies less than 1000 eV and protons having energies less than 10 keV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28683184','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28683184"><span>Comparison of <span class="hlt">ultra</span> <span class="hlt">high</span> performance supercritical fluid chromatography, <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography, and gas chromatography for the separation of synthetic cathinones.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Carnes, Stephanie; O'Brien, Stacey; Szewczak, Angelica; Tremeau-Cayel, Lauriane; Rowe, Walter F; McCord, Bruce; Lurie, Ira S</p> <p>2017-09-01</p> <p>A comparison of <span class="hlt">ultra</span> <span class="hlt">high</span> performance supercritical fluid chromatography, <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography, and gas chromatography for the separation of synthetic cathinones has been conducted. Nine different mixtures of bath salts were analyzed in this study. The three different chromatographic techniques were examined using a general set of controlled synthetic cathinones as well as a variety of other synthetic cathinones that exist as positional isomers. Overall 35 different synthetic cathinones were analyzed. A variety of column types and chromatographic modes were examined for developing each separation. For the <span class="hlt">ultra</span> <span class="hlt">high</span> performance supercritical fluid chromatography separations, analyses were performed using a series of Torus and Trefoil columns with either ammonium formate or ammonium hydroxide as additives, and methanol, ethanol or isopropanol organic solvents as modifiers. <span class="hlt">Ultra</span> <span class="hlt">high</span> performance liquid chromatographic separations were performed in both reversed phase and hydrophilic interaction chromatographic modes using SPP C18 and SPP HILIC columns. Gas chromatography separations were performed using an Elite-5MS capillary column. The orthogonality of <span class="hlt">ultra</span> <span class="hlt">high</span> performance supercritical fluid chromatography, <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography, and gas chromatography was examined using principal component analysis. For the best overall separation of synthetic cathinones, the use of <span class="hlt">ultra</span> <span class="hlt">high</span> performance supercritical fluid chromatography in combination with gas chromatography is recommended. © 2017 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150020510','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150020510"><span>Atomically <span class="hlt">Precise</span> Surface Engineering for Producing Imagers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nikzad, Shouleh (Inventor); Hoenk, Michael E. (Inventor); Greer, Frank (Inventor); Jones, Todd J. (Inventor)</p> <p>2015-01-01</p> <p><span class="hlt">High</span>-quality surface coatings, and techniques combining the atomic <span class="hlt">precision</span> of molecular beam epitaxy and atomic layer deposition, to fabricate such <span class="hlt">high</span>-quality surface coatings are provided. The coatings made in accordance with the techniques set forth by the invention are shown to be capable of forming silicon <span class="hlt">CCD</span> detectors that demonstrate world record detector quantum efficiency (>50%) in the near and far ultraviolet (155 nm-300 nm). The surface engineering approaches used demonstrate the robustness of detector performance that is obtained by achieving atomic level <span class="hlt">precision</span> at all steps in the coating fabrication process. As proof of concept, the characterization, materials, and exemplary devices produced are presented along with a comparison to other approaches.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004SPIE.5198..163T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004SPIE.5198..163T"><span>Advances in <span class="hlt">CCD</span> detector technology for x-ray diffraction applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thorson, Timothy A.; Durst, Roger D.; Frankel, Dan; Bordwell, Rex L.; Camara, Jose R.; Leon-Guerrero, Edward; Onishi, Steven K.; Pang, Francis; Vu, Paul; Westbrook, Edwin M.</p> <p>2004-01-01</p> <p>Phosphor-coupled CCDs are established as one of the most successful technologies for x-ray diffraction. This application demands that the <span class="hlt">CCD</span> simultaneously achieve both the highest possible sensitivity and <span class="hlt">high</span> readout speeds. Recently, wafer-scale, back illuminated devices have become available which offer significantly higher quantum efficiency than conventional devices (the Fairchild Imaging <span class="hlt">CCD</span> 486 BI). However, since back thinning significantly changes the electrical properties of the <span class="hlt">CCD</span> the <span class="hlt">high</span> speed operation of wafer-scale, back-illuminated devices is not well understood. Here we describe the operating characteristics (including noise, linearity, full well capacity and CTE) of the back-illuminated <span class="hlt">CCD</span> 486 at readout speeds up to 4 MHz.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27250371','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27250371"><span><span class="hlt">Ultra-precision</span> fabrication of 500 mm long and laterally graded Ru/C multilayer mirrors for X-ray light sources.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Störmer, M; Gabrisch, H; Horstmann, C; Heidorn, U; Hertlein, F; Wiesmann, J; Siewert, F; Rack, A</p> <p>2016-05-01</p> <p>X-ray mirrors are needed for beam shaping and monochromatization at advanced research light sources, for instance, free-electron lasers and synchrotron sources. Such mirrors consist of a substrate and a coating. The shape accuracy of the substrate and the layer <span class="hlt">precision</span> of the coating are the crucial parameters that determine the beam properties required for various applications. In principal, the selection of the layer materials determines the mirror reflectivity. A single layer mirror offers <span class="hlt">high</span> reflectivity in the range of total external reflection, whereas the reflectivity is reduced considerably above the critical angle. A periodic multilayer can enhance the reflectivity at higher angles due to Bragg reflection. Here, the selection of a suitable combination of layer materials is essential to achieve a <span class="hlt">high</span> flux at distinct photon energies, which is often required for applications such as microtomography, diffraction, or protein crystallography. This contribution presents the current development of a Ru/C multilayer mirror prepared by magnetron sputtering with a sputtering facility that was designed in-house at the Helmholtz-Zentrum Geesthacht. The deposition conditions were optimized in order to achieve <span class="hlt">ultra-high</span> <span class="hlt">precision</span> and <span class="hlt">high</span> flux in future mirrors. Input for the improved deposition parameters came from investigations by transmission electron microscopy. The X-ray optical properties were investigated by means of X-ray reflectometry using Cu- and Mo-radiation. The change of the multilayer d-spacing over the mirror dimensions and the variation of the Bragg angles were determined. The results demonstrate the ability to <span class="hlt">precisely</span> control the variation in thickness over the whole mirror length of 500 mm thus achieving picometer-<span class="hlt">precision</span> in the meter-range.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22597924-ultra-precision-fabrication-mm-long-laterally-graded-ru-multilayer-mirrors-ray-light-sources','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22597924-ultra-precision-fabrication-mm-long-laterally-graded-ru-multilayer-mirrors-ray-light-sources"><span><span class="hlt">Ultra-precision</span> fabrication of 500 mm long and laterally graded Ru/C multilayer mirrors for X-ray light sources</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>Störmer, M., E-mail: michael.stoermer@hzg.de; Gabrisch, H.; Horstmann, C.</p> <p>2016-05-15</p> <p>X-ray mirrors are needed for beam shaping and monochromatization at advanced research light sources, for instance, free-electron lasers and synchrotron sources. Such mirrors consist of a substrate and a coating. The shape accuracy of the substrate and the layer <span class="hlt">precision</span> of the coating are the crucial parameters that determine the beam properties required for various applications. In principal, the selection of the layer materials determines the mirror reflectivity. A single layer mirror offers <span class="hlt">high</span> reflectivity in the range of total external reflection, whereas the reflectivity is reduced considerably above the critical angle. A periodic multilayer can enhance the reflectivity atmore » higher angles due to Bragg reflection. Here, the selection of a suitable combination of layer materials is essential to achieve a <span class="hlt">high</span> flux at distinct photon energies, which is often required for applications such as microtomography, diffraction, or protein crystallography. This contribution presents the current development of a Ru/C multilayer mirror prepared by magnetron sputtering with a sputtering facility that was designed in-house at the Helmholtz-Zentrum Geesthacht. The deposition conditions were optimized in order to achieve <span class="hlt">ultra-high</span> <span class="hlt">precision</span> and <span class="hlt">high</span> flux in future mirrors. Input for the improved deposition parameters came from investigations by transmission electron microscopy. The X-ray optical properties were investigated by means of X-ray reflectometry using Cu- and Mo-radiation. The change of the multilayer d-spacing over the mirror dimensions and the variation of the Bragg angles were determined. The results demonstrate the ability to <span class="hlt">precisely</span> control the variation in thickness over the whole mirror length of 500 mm thus achieving picometer-<span class="hlt">precision</span> in the meter-range.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/873049','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/873049"><span>Vacuum compatible miniature <span class="hlt">CCD</span> camera head</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Conder, Alan D.</p> <p>2000-01-01</p> <p>A charge-coupled device (<span class="hlt">CCD</span>) camera head which can replace film for digital imaging of visible light, ultraviolet radiation, and soft to penetrating x-rays, such as within a target chamber where laser produced plasmas are studied. The camera head is small, capable of operating both in and out of a vacuum environment, and is versatile. The <span class="hlt">CCD</span> camera head uses PC boards with an internal heat sink connected to the chassis for heat dissipation, which allows for close(0.04" for example) stacking of the PC boards. Integration of this <span class="hlt">CCD</span> camera head into existing instrumentation provides a substantial enhancement of diagnostic capabilities for studying <span class="hlt">high</span> energy density plasmas, for a variety of military industrial, and medical imaging applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4037707','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4037707"><span><span class="hlt">High-Precision</span> Distribution of <span class="hlt">Highly</span> Stable Optical Pulse Trains with 8.8 × 10−19 instability</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ning, B.; Zhang, S. Y.; Hou, D.; Wu, J. T.; Li, Z. B.; Zhao, J. Y.</p> <p>2014-01-01</p> <p>The <span class="hlt">high-precision</span> distribution of optical pulse trains via fibre links has had a considerable impact in many fields. In most published work, the accuracy is still fundamentally limited by unavoidable noise sources, such as thermal and shot noise from conventional photodiodes and thermal noise from mixers. Here, we demonstrate a new <span class="hlt">high-precision</span> timing distribution system that uses a <span class="hlt">highly</span> <span class="hlt">precise</span> phase detector to obviously reduce the effect of these limitations. Instead of using photodiodes and microwave mixers, we use several fibre Sagnac-loop-based optical-microwave phase detectors (OM-PDs) to achieve optical-electrical conversion and phase measurements, thereby suppressing the sources of noise and achieving <span class="hlt">ultra-high</span> accuracy. The results of a distribution experiment using a 10-km fibre link indicate that our system exhibits a residual instability of 2.0 × 10−15 at1 s and8.8 × 10−19 at 40,000 s and an integrated timing jitter as low as 3.8 fs in a bandwidth of 1 Hz to 100 kHz. This low instability and timing jitter make it possible for our system to be used in the distribution of optical-clock signals or in applications that require extremely accurate frequency/time synchronisation. PMID:24870442</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JDSO...13...13H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JDSO...13...13H"><span>Quasi-Speckle Measurements of Close Double Stars With a <span class="hlt">CCD</span> Camera</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harshaw, Richard</p> <p>2017-01-01</p> <p><span class="hlt">CCD</span> measurements of visual double stars have been an active area of amateur observing for several years now. However, most <span class="hlt">CCD</span> measurements rely on “lucky imaging” (selecting a very small percentage of the best frames of a larger frame set so as to get the best “frozen” atmosphere for the image), a technique that has limitations with regards to how close the stars can be and still be cleanly resolved in the lucky image. In this paper, the author reports how using deconvolution stars in the analysis of close double stars can greatly enhance the quality of the autocorellogram, leading to a more <span class="hlt">precise</span> solution using speckle reduction software rather than lucky imaging.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhDT.........2O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhDT.........2O"><span><span class="hlt">High</span> Efficient <span class="hlt">Ultra</span>-Thin Flat Optics Based on Dielectric Metasurfaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ozdemir, Aytekin</p> <p></p> <p>Metasurfaces which emerged as two-dimensional counterparts of metamaterials, facilitate the realization of arbitrary phase distributions using large arrays with subwavelength and <span class="hlt">ultra</span>-thin features. Even if metasurfaces are <span class="hlt">ultra</span>-thin, they still effectively manipulate the phase, amplitude, and polarization of light in transmission or reflection mode. In contrast, conventional optical components are bulky, and they lose their functionality at sub-wavelength scales, which requires conceptually new types of nanoscale optical devices. On the other hand, as the optical systems shrink in size day by day, conventional bulky optical components will have tighter alignment and fabrication tolerances. Since metasurfaces can be fabricated lithographically, alignment can be done during lithographic fabrication, thus eliminating the need for post-fabrication alignments. In this work, various types of metasurface applications are thoroughly investigated for robust wavefront engineering with enhanced characteristics in terms of broad bandwidth, <span class="hlt">high</span> efficiency and active tunability, while beneficial for application. Plasmonic metasurfaces are not compatible with the CMOS process flow, and, additionally their <span class="hlt">high</span> absorption and ohmic loss is problematic in transmission based applications. Dielectric metasurfaces, however, offer a strong magnetic response at optical frequencies, and thus they can offer great opportunities for interacting not only with the electric component of a light field, but also with its magnetic component. They show great potential to enable practical device functionalities at optical frequencies, which motivates us to explore them one step further on wavefront engineering and imaging sensor platforms. Therefore, we proposed an efficient <span class="hlt">ultra</span>-thin flat metalens at near-infrared regime constituted by silicon nanodisks which can support both electric and magnetic dipolar Mie-type resonances. These two dipole resonances can be overlapped at the same frequency</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5362893','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5362893"><span>Plasmonic metamaterial for electromagnetically induced transparency analogue and <span class="hlt">ultra-high</span> figure of merit sensor</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Wu, Dong; Liu, Yumin; Yu, Li; Yu, Zhongyuan; Chen, Lei; Li, Ruifang; Ma, Rui; Liu, Chang; Zhang, Jinqiannan; Ye, Han</p> <p>2017-01-01</p> <p>In this work, using finite-difference time-domain method, we propose and numerically demonstrate a novel way to achieve electromagnetically induced transparency (EIT) phenomenon in the reflection spectrum by stacking two different types of coupling effect among different elements of the designed metamaterial. Compared with the conventional EIT-like analogues coming from only one type of coupling effect between bright and dark meta-atoms on the same plane, to our knowledge the novel approach is the first to realize the optically active and <span class="hlt">precise</span> control of the wavelength position of EIT-like phenomenon using optical metamaterials. An on-to-off dynamic control of the EIT-like phenomenon also can be achieved by changing the refractive index of the dielectric substrate via adjusting an optical pump pulse. Furthermore, in near infrared region, the metamaterial structure can be operated as an <span class="hlt">ultra-high</span> resolution refractive index sensor with an <span class="hlt">ultra-high</span> figure of merit (FOM) reaching 3200, which remarkably improve the FOM value of plasmonic refractive index sensors. The novel approach realizing EIT-like spectral shape with easy adjustment to the working wavelengths will open up new avenues for future research and practical application of active plasmonic switch, <span class="hlt">ultra-high</span> resolution sensors and active slow-light devices. PMID:28332629</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010IAUS..266..361B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010IAUS..266..361B"><span>Multicolor <span class="hlt">CCD</span> photometry of the open cluster NGC 752</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bartašiūtė, Stanislava; Janusz, Robert; Boyle, Richard P.; Philip, A. G. Davis; Deveikis, Viktoras</p> <p>2010-01-01</p> <p>We obtained <span class="hlt">CCD</span> observations of the open cluster NGC 752 with the 1.8m Vatican Advanced Technology Telescope (Mt. Graham, Arizona) with a 4K <span class="hlt">CCD</span> camera and eight intermediate-band filters of the Stromvil (Strömgren + Vilnius) system. Four 12‧ × 12‧ fields were observed, covering the central part of the cluster. The good-quality multicolor data made it possible to obtain <span class="hlt">precise</span> estimates of distance moduli, metallicity and foreground reddening for individual stars down to the limiting magnitude, V = 17.5, enabling photometric identification of faint cluster members. The new observations provide an extension of the lower main sequence to three magnitudes beyond the previous (photographic) limit. A relatively small number of photometric members identified at fainter magnitudes seems to be indicative of actual dissolution of the cluster from the low-mass end.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23405276','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23405276"><span><span class="hlt">Ultra</span> <span class="hlt">high</span> energy electrons powered by pulsar rotation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mahajan, Swadesh; Machabeli, George; Osmanov, Zaza; Chkheidze, Nino</p> <p>2013-01-01</p> <p>A new mechanism of particle acceleration, driven by the rotational slow down of the Crab pulsar, is explored. The rotation, through the time dependent centrifugal force, can efficiently excite unstable Langmuir waves in the electron-positron (hereafter e(±)) plasma of the star magnetosphere. These waves, then, Landau damp on electrons accelerating them in the process. The net transfer of energy is optimal when the wave growth and the Landau damping times are comparable and are both very short compared to the star rotation time. We show, by detailed calculations, that these are <span class="hlt">precisely</span> the conditions for the parameters of the Crab pulsar. This <span class="hlt">highly</span> efficient route for energy transfer allows the electrons in the primary beam to be catapulted to multiple TeV (~ 100 TeV) and even PeV energy domain. It is expected that the proposed mechanism may, unravel the puzzle of the origin of <span class="hlt">ultra</span> <span class="hlt">high</span> energy cosmic ray electrons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22632177-su-sparing-normal-tissue-ultra-high-dose-rate-radiation-therapy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22632177-su-sparing-normal-tissue-ultra-high-dose-rate-radiation-therapy"><span>SU-F-J-45: Sparing Normal Tissue with <span class="hlt">Ultra-High</span> Dose Rate in Radiation Therapy</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>Feng, Y</p> <p></p> <p>Purpose: To spare normal tissue by reducing the location uncertainty of a moving target, we proposed an <span class="hlt">ultra-high</span> dose rate system and evaluated. Methods: <span class="hlt">High</span> energy electrons generated with a linear accelerator were injected into a storage ring to be accumulated. The number of the electrons in the ring was determined based on the prescribed radiation dose. The dose was delivered within a millisecond, when an online imaging system found that the target was in the position that was consistent with that in a treatment plan. In such a short time period, the displacement of the target was negligible. Themore » margin added to the clinical target volume (CTV) could be reduced that was evaluated by comparing of volumes between CTV and ITV in 14 cases of lung stereotactic body radiation therapy (SBRT) treatments. A design of the <span class="hlt">ultra-high</span> dose rate system was evaluated based clinical needs and the recent developments of low energy (a few MeV) electron storage ring. Results: This design of <span class="hlt">ultra-high</span> dose rate system was feasible based on the techniques currently available. The reduction of a target volume was significant by reducing the margin that accounted the motion of the target. ∼50% volume reduction of the internal target volume (ITV) could be achieved in lung SBRT treatments. Conclusion: With this innovation of <span class="hlt">ultra-high</span> dose rate system, the margin of target is able to be significantly reduced. It will reduce treatment time of gating and allow <span class="hlt">precisely</span> specified gating window to improve the accuracy of dose delivering.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860030579&hterms=scientific+collections&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dscientific%2Bcollections','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860030579&hterms=scientific+collections&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dscientific%2Bcollections"><span>The future scientific <span class="hlt">CCD</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Janesick, J. R.; Elliott, T.; Collins, S.; Marsh, H.; Blouke, M. M.</p> <p>1984-01-01</p> <p>Since the first introduction of charge-coupled devices (CCDs) in 1970, CCDs have been considered for applications related to memories, logic circuits, and the detection of visible radiation. It is pointed out, however, that the mass market orientation of <span class="hlt">CCD</span> development has left largely untapped the enormous potential of these devices for advanced scientific instrumentation. The present paper has, therefore, the objective to introduce the <span class="hlt">CCD</span> characteristics to the scientific community, taking into account prospects for further improvement. Attention is given to evaluation criteria, a summary of current CCDs, <span class="hlt">CCD</span> performance characteristics, absolute calibration tools, quantum efficiency, aspects of charge collection, charge transfer efficiency, read noise, and predictions regarding the characteristics of the next generation of silicon scientific <span class="hlt">CCD</span> imagers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27805766','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27805766"><span>Determination of dasatinib in the tablet dosage form by <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography, capillary zone electrophoresis, and sequential injection analysis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gonzalez, Aroa Garcia; Taraba, Lukáš; Hraníček, Jakub; Kozlík, Petr; Coufal, Pavel</p> <p>2017-01-01</p> <p>Dasatinib is a novel oral prescription drug proposed for treating adult patients with chronic myeloid leukemia. Three analytical methods, namely <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography, capillary zone electrophoresis, and sequential injection analysis, were developed, validated, and compared for determination of the drug in the tablet dosage form. The total analysis time of optimized <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography and capillary zone electrophoresis methods was 2.0 and 2.2 min, respectively. Direct ultraviolet detection with detection wavelength of 322 nm was employed in both cases. The optimized sequential injection analysis method was based on spectrophotometric detection of dasatinib after a simple colorimetric reaction with folin ciocalteau reagent forming a blue-colored complex with an absorbance maximum at 745 nm. The total analysis time was 2.5 min. The <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography method provided the lowest detection and quantitation limits and the most <span class="hlt">precise</span> and accurate results. All three newly developed methods were demonstrated to be specific, linear, sensitive, <span class="hlt">precise</span>, and accurate, providing results satisfactorily meeting the requirements of the pharmaceutical industry, and can be employed for the routine determination of the active pharmaceutical ingredient in the tablet dosage form. © 2016 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_7 --> <div id="page_8" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="141"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS.986a2037C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS.986a2037C"><span>Research on subsurface deformed layer in <span class="hlt">ultra-precision</span> cutting of single crystal copper by focused ion beam etching method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Y.; Huang, X. J.; Kong, J. X.</p> <p>2018-03-01</p> <p>In this paper, the focused ion beam was used to study the subsurface deformed layer of single crystal copper caused by the nanoscale single-point diamond fly cutting, and the possibility of using nanometer <span class="hlt">ultra-precision</span> cutting to remove the larger deformation layer caused by traditional rough cutting process was explored. The maximum cutting thickness of single-point diamond cutting was about 146 nm, and the surface of the single-crystal copper after cutting was etched and observed by using the focused ion beam method. It was found that the morphology of the near-surface layer and the intermediate layer of the copper material were larger differences: the near-surface of the material was smaller and more compact, and the intermediate material layer of the material was more coarse sparse. The results showed that the traditional <span class="hlt">precision</span> cutting would residual significant subsurface deformed layer and the thickness was on micron level. Even more, the subsurface deformed layer was obviously removed from about 12μm to 5μm after single-point diamond fly cutting in this paper. This paper proved that the large-scale subsurface deformed layer caused by traditional cutting process could be removed by nanometer <span class="hlt">ultra-precision</span> cutting. It was of great significance to further establish the method that control of the deformation of weak rigid components by reducing the depth of the subsurface deformed layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040013331&hterms=chromatic&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dchromatic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040013331&hterms=chromatic&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dchromatic"><span>Chromatic Modulator for <span class="hlt">High</span> Resolution <span class="hlt">CCD</span> or APS Devices</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hartley, Frank T. (Inventor); Hull, Anthony B. (Inventor)</p> <p>2003-01-01</p> <p>A system for providing <span class="hlt">high</span>-resolution color separation in electronic imaging. Comb drives controllably oscillate a red-green-blue (RGB) color strip filter system (or otherwise) over an electronic imaging system such as a charge-coupled device (<span class="hlt">CCD</span>) or active pixel sensor (APS). The color filter is modulated over the imaging array at a rate three or more times the frame rate of the imaging array. In so doing, the underlying active imaging elements are then able to detect separate color-separated images, which are then combined to provide a color-accurate frame which is then recorded as the representation of the recorded image. <span class="hlt">High</span> pixel resolution is maintained. Registration is obtained between the color strip filter and the underlying imaging array through the use of electrostatic comb drives in conjunction with a spring suspension system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993SPIE.1801..470G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993SPIE.1801..470G"><span>Characterization of a 512x512-pixel 8-output full-frame <span class="hlt">CCD</span> for <span class="hlt">high</span>-speed imaging</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Graeve, Thorsten; Dereniak, Eustace L.</p> <p>1993-01-01</p> <p>The characterization of a 512 by 512 pixel, eight-output full frame <span class="hlt">CCD</span> manufactured by English Electric Valve under part number <span class="hlt">CCD</span>13 is discussed. This device is a <span class="hlt">high</span>- resolution Silicon-based array designed for visible imaging applications at readout periods as low as two milliseconds. The characterization of the device includes mean-variance analysis to determine read noise and dynamic range, as well as charge transfer efficiency, MTF, and quantum efficiency measurements. Dark current and non-uniformity issues on a pixel-to-pixel basis and between individual outputs are also examined. The characterization of the device is restricted by hardware limitations to a one MHz pixel rate, corresponding to a 40 ms readout time. However, subsections of the device have been operated at up to an equivalent 100 frames per second. To maximize the frame rate, the <span class="hlt">CCD</span> is illuminated by a synchronized strobe flash in between frame readouts. The effects of the strobe illumination on the imagery obtained from the device is discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4077219','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4077219"><span>Apical dominance in saffron and the involvement of the branching enzymes <span class="hlt">CCD</span>7 and <span class="hlt">CCD</span>8 in the control of bud sprouting</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2014-01-01</p> <p>Background In saffron (Crocus sativus), new corms develop at the base of every shoot developed from the maternal corm, a globular underground storage stem. Since the degree of bud sprouts influences the number and size of new corms, and strigolactones (SLs) suppress growth of pre-formed axillary bud, it was considered appropriate to investigate SL involvement in physiology and molecular biology in saffron. We focused on two of the genes within the SL pathway, <span class="hlt">CCD</span>7 and <span class="hlt">CCD</span>8, encoding carotenoid cleavage enzymes required for the production of SLs. Results The Cs<span class="hlt">CCD</span>7 and Cs<span class="hlt">CCD</span>8 genes are the first ones isolated and characterized from a non-grass monocotyledonous plant. Cs<span class="hlt">CCD</span>7 and Cs<span class="hlt">CCD</span>8 expression showed some overlapping, although they were not identical. Cs<span class="hlt">CCD</span>8 was <span class="hlt">highly</span> expressed in quiescent axillary buds and decapitation dramatically reduced its expression levels, suggesting its involvement in the suppression of axillary bud outgrowth. Furthermore, in vitro experiments showed also the involvement of auxin, cytokinin and jasmonic acid on the sprouting of axillary buds from corms in which the apical bud was removed. In addition, Cs<span class="hlt">CCD</span>8 expression, but not Cs<span class="hlt">CCD</span>7, was higher in the newly developed vascular tissue of axillary buds compared to the vascular tissue of the apical bud. Conclusions We showed that production and transport of auxin in saffron corms could act synergistically with SLs to arrest the outgrowth of the axillary buds, similar to the control of above-ground shoot branching. In addition, jasmonic acid seems to play a prominent role in bud dormancy in saffron. While cytokinins from roots promote bud outgrowth. In addition the expression results of Cs<span class="hlt">CCD</span>8 suggest that SLs could positively regulate procambial activity and the development of new vascular tissues connecting leaves with the mother corm. PMID:24947472</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JInst..12C2033S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JInst..12C2033S"><span>Trap pumping schemes for the Euclid <span class="hlt">CCD</span>273 detector: characterisation of electrodes and defects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Skottfelt, J.; Hall, D. J.; Dryer, B.; Bush, N.; Campa, J.; Gow, J. P. D.; Holland, A. D.; Jordan, D.; Burt, D.</p> <p>2017-12-01</p> <p>The VISible imager instrument (VIS) on board the Euclid mission will deliver <span class="hlt">high</span> resolution shape measurements of galaxies down to very faint limits (R ~ 25 at 10σ) in a large part of the sky, in order to infer the distribution of dark matter in the Universe. To help mitigate radiation damage effects that will accumulate in the detectors over the mission lifetime, the properties of the radiation induced traps needs to be known with as <span class="hlt">high</span> <span class="hlt">precision</span> as possible. For this purpose the trap pumping method will be employed as part of the in-orbit calibration routines. Using trap pumping it is possible to identify and characterise single traps in a Charge-Coupled Device (<span class="hlt">CCD</span>), thus providing information such as the density, emission time constants and sub-pixel positions of the traps in the detectors. This paper presents the trap pumping algorithms used for the radiation testing campaign of the <span class="hlt">CCD</span>273 detectors, performed by the Centre for Electronic Imaging (CEI) at the Open University, that will be used for the VIS instrument. The <span class="hlt">CCD</span>273 is a four-phase device with uneven phase widths, which complicates the trap pumping analysis. However, we find that by optimising the trap pumping algorithms and analysis routines, it is possible to obtain sub-pixel and even sub-phase positional information about the traps. Further, by comparing trap pumping data with simulations, it is possible to gain more information about the effective electrode widths of the device.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3471246','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3471246"><span>Quantile Regression for Analyzing Heterogeneity in <span class="hlt">Ultra-high</span> Dimension</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Wang, Lan; Wu, Yichao</p> <p>2012-01-01</p> <p><span class="hlt">Ultra-high</span> dimensional data often display heterogeneity due to either heteroscedastic variance or other forms of non-location-scale covariate effects. To accommodate heterogeneity, we advocate a more general interpretation of sparsity which assumes that only a small number of covariates influence the conditional distribution of the response variable given all candidate covariates; however, the sets of relevant covariates may differ when we consider different segments of the conditional distribution. In this framework, we investigate the methodology and theory of nonconvex penalized quantile regression in <span class="hlt">ultra-high</span> dimension. The proposed approach has two distinctive features: (1) it enables us to explore the entire conditional distribution of the response variable given the <span class="hlt">ultra-high</span> dimensional covariates and provides a more realistic picture of the sparsity pattern; (2) it requires substantially weaker conditions compared with alternative methods in the literature; thus, it greatly alleviates the difficulty of model checking in the <span class="hlt">ultra-high</span> dimension. In theoretic development, it is challenging to deal with both the nonsmooth loss function and the nonconvex penalty function in <span class="hlt">ultra-high</span> dimensional parameter space. We introduce a novel sufficient optimality condition which relies on a convex differencing representation of the penalized loss function and the subdifferential calculus. Exploring this optimality condition enables us to establish the oracle property for sparse quantile regression in the <span class="hlt">ultra-high</span> dimension under relaxed conditions. The proposed method greatly enhances existing tools for <span class="hlt">ultra-high</span> dimensional data analysis. Monte Carlo simulations demonstrate the usefulness of the proposed procedure. The real data example we analyzed demonstrates that the new approach reveals substantially more information compared with alternative methods. PMID:23082036</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SPIE10503E..2EU','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SPIE10503E..2EU"><span>Phase shifting white light interferometry using colour <span class="hlt">CCD</span> for optical metrology and bio-imaging applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Upputuri, Paul Kumar; Pramanik, Manojit</p> <p>2018-02-01</p> <p>Phase shifting white light interferometry (PSWLI) has been widely used for optical metrology applications because of their <span class="hlt">precision</span>, reliability, and versatility. White light interferometry using monochrome <span class="hlt">CCD</span> makes the measurement process slow for metrology applications. WLI integrated with Red-Green-Blue (RGB) <span class="hlt">CCD</span> camera is finding imaging applications in the fields optical metrology and bio-imaging. Wavelength dependent refractive index profiles of biological samples were computed from colour white light interferograms. In recent years, whole-filed refractive index profiles of red blood cells (RBCs), onion skin, fish cornea, etc. were measured from RGB interferograms. In this paper, we discuss the bio-imaging applications of colour <span class="hlt">CCD</span> based white light interferometry. The approach makes the measurement faster, easier, cost-effective, and even dynamic by using single fringe analysis methods, for industrial applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1187978','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1187978"><span><span class="hlt">Precision</span> Spectrophotometric Calibration System for Dark Energy Instruments</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>Schubnell, Michael S.</p> <p>2015-06-30</p> <p>For this research we build a <span class="hlt">precision</span> calibration system and carried out measurements to demonstrate the <span class="hlt">precision</span> that can be achieved with a <span class="hlt">high</span> <span class="hlt">precision</span> spectrometric calibration system. It was shown that the system is capable of providing a complete spectrophotometric calibration at the sub-pixel level. The calibration system uses a fast, <span class="hlt">high</span> <span class="hlt">precision</span> monochromator that can quickly and efficiently scan over an instrument’s entire spectral range with a spectral line width of less than 0.01 nm corresponding to a fraction of a pixel on the <span class="hlt">CCD</span>. The system was extensively evaluated in the laboratory. Our research showed that amore » complete spectrophotometric calibration standard for spectroscopic survey instruments such as DESI is possible. The monochromator <span class="hlt">precision</span> and repeatability to a small fraction of the DESI spectrograph LSF was demonstrated with re-initialization on every scan and thermal drift compensation by locking to multiple external line sources. A projector system that mimics telescope aperture for point source at infinity was demonstrated.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120006570','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120006570"><span><span class="hlt">CCD</span> Camera Lens Interface for Real-Time Theodolite Alignment</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wake, Shane; Scott, V. Stanley, III</p> <p>2012-01-01</p> <p>Theodolites are a common instrument in the testing, alignment, and building of various systems ranging from a single optical component to an entire instrument. They provide a <span class="hlt">precise</span> way to measure horizontal and vertical angles. They can be used to align multiple objects in a desired way at specific angles. They can also be used to reference a specific location or orientation of an object that has moved. Some systems may require a small margin of error in position of components. A theodolite can assist with accurately measuring and/or minimizing that error. The technology is an adapter for a <span class="hlt">CCD</span> camera with lens to attach to a Leica Wild T3000 Theodolite eyepiece that enables viewing on a connected monitor, and thus can be utilized with multiple theodolites simultaneously. This technology removes a substantial part of human error by relying on the <span class="hlt">CCD</span> camera and monitors. It also allows image recording of the alignment, and therefore provides a quantitative means to measure such error.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26724089','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26724089"><span>Note: <span class="hlt">Ultra</span>-low birefringence dodecagonal vacuum glass cell.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Brakhane, Stefan; Alt, Wolfgang; Meschede, Dieter; Robens, Carsten; Moon, Geol; Alberti, Andrea</p> <p>2015-12-01</p> <p>We report on an <span class="hlt">ultra</span>-low birefringence dodecagonal glass cell for <span class="hlt">ultra-high</span> vacuum applications. The epoxy-bonded trapezoidal windows of the cell are made of SF57 glass, which exhibits a very low stress-induced birefringence. We characterize the birefringence Δn of each window with the cell under vacuum conditions, obtaining values around 10(-8). After baking the cell at 150 °C, we reach a pressure below 10(-10) mbar. In addition, each window is antireflection coated on both sides, which is <span class="hlt">highly</span> desirable for quantum optics experiments and <span class="hlt">precision</span> measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060038662&hterms=Dinosaurs&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DDinosaurs','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060038662&hterms=Dinosaurs&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DDinosaurs"><span>Active Pixel Sensors: Are <span class="hlt">CCD</span>'s Dinosaurs?</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fossum, Eric R.</p> <p>1993-01-01</p> <p>Charge-coupled devices (<span class="hlt">CCD</span>'s) are presently the technology of choice for most imaging applications. In the 23 years since their invention in 1970, they have evolved to a sophisticated level of performance. However, as with all technologies, we can be certain that they will be supplanted someday. In this paper, the Active Pixel Sensor (APS) technology is explored as a possible successor to the <span class="hlt">CCD</span>. An active pixel is defined as a detector array technology that has at least one active transistor within the pixel unit cell. The APS eliminates the need for nearly perfect charge transfer -- the Achilles' heel of CCDs. This perfect charge transfer makes <span class="hlt">CCD</span>'s radiation 'soft,' difficult to use under low light conditions, difficult to manufacture in large array sizes, difficult to integrate with on-chip electronics, difficult to use at low temperatures, difficult to use at <span class="hlt">high</span> frame rates, and difficult to manufacture in non-silicon materials that extend wavelength response.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25037013','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25037013"><span><span class="hlt">Precise</span> montaging and metric quantification of retinal surface area from <span class="hlt">ultra</span>-widefield fundus photography and fluorescein angiography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Croft, Daniel E; van Hemert, Jano; Wykoff, Charles C; Clifton, David; Verhoek, Michael; Fleming, Alan; Brown, David M</p> <p>2014-01-01</p> <p>Accurate quantification of retinal surface area from <span class="hlt">ultra</span>-widefield (UWF) images is challenging due to warping produced when the retina is projected onto a two-dimensional plane for analysis. By accounting for this, the authors sought to <span class="hlt">precisely</span> montage and accurately quantify retinal surface area in square millimeters. Montages were created using Optos 200Tx (Optos, Dunfermline, U.K.) images taken at different gaze angles. A transformation projected the images to their correct location on a three-dimensional model. Area was quantified with spherical trigonometry. Warping, <span class="hlt">precision</span>, and accuracy were assessed. Uncorrected, posterior pixels represented up to 79% greater surface area than peripheral pixels. Assessing <span class="hlt">precision</span>, a standard region was quantified across 10 montages of the same eye (RSD: 0.7%; mean: 408.97 mm(2); range: 405.34-413.87 mm(2)). Assessing accuracy, 50 patients' disc areas were quantified (mean: 2.21 mm(2); SE: 0.06 mm(2)), and the results fell within the normative range. By accounting for warping inherent in UWF images, <span class="hlt">precise</span> montaging and accurate quantification of retinal surface area in square millimeters were achieved. Copyright 2014, SLACK Incorporated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013NIMPA.731...47S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013NIMPA.731...47S"><span>Developing a <span class="hlt">CCD</span> camera with <span class="hlt">high</span> spatial resolution for RIXS in the soft X-ray range</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Soman, M. R.; Hall, D. J.; Tutt, J. H.; Murray, N. J.; Holland, A. D.; Schmitt, T.; Raabe, J.; Schmitt, B.</p> <p>2013-12-01</p> <p>The Super Advanced X-ray Emission Spectrometer (SAXES) at the Swiss Light Source contains a <span class="hlt">high</span> resolution Charge-Coupled Device (<span class="hlt">CCD</span>) camera used for Resonant Inelastic X-ray Scattering (RIXS). Using the current <span class="hlt">CCD</span>-based camera system, the energy-dispersive spectrometer has an energy resolution (E/ΔE) of approximately 12,000 at 930 eV. A recent study predicted that through an upgrade to the grating and camera system, the energy resolution could be improved by a factor of 2. In order to achieve this goal in the spectral domain, the spatial resolution of the <span class="hlt">CCD</span> must be improved to better than 5 μm from the current 24 μm spatial resolution (FWHM). The 400 eV-1600 eV energy X-rays detected by this spectrometer primarily interact within the field free region of the <span class="hlt">CCD</span>, producing electron clouds which will diffuse isotropically until they reach the depleted region and buried channel. This diffusion of the charge leads to events which are split across several pixels. Through the analysis of the charge distribution across the pixels, various centroiding techniques can be used to pinpoint the spatial location of the X-ray interaction to the sub-pixel level, greatly improving the spatial resolution achieved. Using the PolLux soft X-ray microspectroscopy endstation at the Swiss Light Source, a beam of X-rays of energies from 200 eV to 1400 eV can be focused down to a spot size of approximately 20 nm. Scanning this spot across the 16 μm square pixels allows the sub-pixel response to be investigated. Previous work has demonstrated the potential improvement in spatial resolution achievable by centroiding events in a standard <span class="hlt">CCD</span>. An Electron-Multiplying <span class="hlt">CCD</span> (EM-<span class="hlt">CCD</span>) has been used to improve the signal to effective readout noise ratio achieved resulting in a worst-case spatial resolution measurement of 4.5±0.2 μm and 3.9±0.1 μm at 530 eV and 680 eV respectively. A method is described that allows the contribution of the X-ray spot size to be deconvolved from these</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9154E..1WK','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9154E..1WK"><span>Measurement of pixel response functions of a fully depleted <span class="hlt">CCD</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kobayashi, Yukiyasu; Niwa, Yoshito; Yano, Taihei; Gouda, Naoteru; Hara, Takuji; Yamada, Yoshiyuki</p> <p>2014-07-01</p> <p>We describe the measurement of detailed and <span class="hlt">precise</span> Pixel Response Functions (PRFs) of a fully depleted <span class="hlt">CCD</span>. Measurements were performed under different physical conditions, such as different wavelength light sources or <span class="hlt">CCD</span> operating temperatures. We determined the relations between these physical conditions and the forms of the PRF. We employ two types of PRFs: one is the model PRF (mPRF) that can represent the shape of a PRF with one characteristic parameter and the other is the simulated PRF (sPRF) that is the resultant PRF from simulating physical phenomena. By using measured, model, and simulated PRFs, we determined the relations between operational parameters and the PRFs. Using the obtained relations, we can now estimate a PRF under conditions that will be encountered during the course of Nano-JASMINE observations. These estimated PRFs will be utilized in the analysis of the Nano-JASMINE data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/870762','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/870762"><span>Enhanced performance <span class="hlt">CCD</span> output amplifier</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Dunham, Mark E.; Morley, David W.</p> <p>1996-01-01</p> <p>A low-noise FET amplifier is connected to amplify output charge from a che coupled device (<span class="hlt">CCD</span>). The FET has its gate connected to the <span class="hlt">CCD</span> in common source configuration for receiving the output charge signal from the <span class="hlt">CCD</span> and output an intermediate signal at a drain of the FET. An intermediate amplifier is connected to the drain of the FET for receiving the intermediate signal and outputting a low-noise signal functionally related to the output charge signal from the <span class="hlt">CCD</span>. The amplifier is preferably connected as a virtual ground to the FET drain. The inherent shunt capacitance of the FET is selected to be at least equal to the sum of the remaining capacitances.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910013744','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910013744"><span>Scientific <span class="hlt">CCD</span> technology at JPL</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Janesick, J.; Collins, S. A.; Fossum, E. R.</p> <p>1991-01-01</p> <p>Charge-coupled devices (<span class="hlt">CCD</span>'s) were recognized for their potential as an imaging technology almost immediately following their conception in 1970. Twenty years later, they are firmly established as the technology of choice for visible imaging. While consumer applications of <span class="hlt">CCD</span>'s, especially the emerging home video camera market, dominated manufacturing activity, the scientific market for <span class="hlt">CCD</span> imagers has become significant. Activity of the Jet Propulsion Laboratory and its industrial partners in the area of <span class="hlt">CCD</span> imagers for space scientific instruments is described. Requirements for scientific imagers are significantly different from those needed for home video cameras, and are described. An imager for an instrument on the CRAF/Cassini mission is described in detail to highlight achieved levels of performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000AJ....120.2131Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000AJ....120.2131Z"><span>The First US Naval Observatory <span class="hlt">CCD</span> Astrograph Catalog</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zacharias, N.; Urban, S. E.; Zacharias, M. I.; Hall, D. M.; Wycoff, G. L.; Rafferty, T. J.; Germain, M. E.; Holdenried, E. R.; Pohlman, J. W.; Gauss, F. S.; Monet, D. G.; Winter, L.</p> <p>2000-10-01</p> <p>The USNO <span class="hlt">CCD</span> Astrograph (UCA) started an astrometric survey in 1998 February at Cerro Tololo, Chile. This first, preliminary catalog (UCAC1) includes data taken up to 1999 November with about 80% of the Southern Hemisphere covered. Observing continues, and full sky coverage is expected by mid-2003 after moving the instrument to a Northern Hemisphere site in early 2001. The survey is performed in a single bandpass (579-642 nm), a twofold overlap pattern of fields, and with a long and a short exposure on each field. Stars in the magnitude range 10-14 have positional <span class="hlt">precisions</span> of <=20 mas. At the limiting magnitude of R~16 mag, the positional <span class="hlt">precision</span> is 70 mas. The UCAC aims at a density (stars per square degree) larger than that of the Guide Star Catalog (GSC) with a positional accuracy similar to Tycho. The UCAC program is a major step toward a <span class="hlt">high-precision</span> densification of the optical reference frame in the post-Hipparcos era, and the first stage, the UCAC1 contains over 27 million stars. Preliminary proper motions are included, which were derived from Tycho-2, Hipparcos, and ground-based transit circle and photographic surveys for the bright stars (V<=12.5 mag) and the USNO A2.0 for the fainter stars. The accuracy of the proper motions varies widely, from 1 to over 15 mas yr-1. The UCAC1 is available on CD-ROM from the US Naval Observatory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SMaS...23g4012K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SMaS...23g4012K"><span>Enhancing thermal reliability of fiber-optic sensors for bio-inspired applications at <span class="hlt">ultra-high</span> temperatures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kang, Donghoon; Kim, Heon-Young; Kim, Dae-Hyun</p> <p>2014-07-01</p> <p>The rapid growth of bio-(inspired) sensors has led to an improvement in modern healthcare and human-robot systems in recent years. Higher levels of reliability and better flexibility, essential features of these sensors, are very much required in many application fields (e.g. applications at <span class="hlt">ultra-high</span> temperatures). Fiber-optic sensors, and fiber Bragg grating (FBG) sensors in particular, are being widely studied as suitable sensors for improved structural health monitoring (SHM) due to their many merits. To enhance the thermal reliability of FBG sensors, thermal sensitivity, generally expressed as αf + ξf and considered a constant, should be investigated more <span class="hlt">precisely</span>. For this purpose, the governing equation of FBG sensors is modified using differential derivatives between the wavelength shift and the temperature change in this study. Through a thermal test ranging from RT to 900 °C, the thermal sensitivity of FBG sensors is successfully examined and this guarantees thermal reliability of FBG sensors at <span class="hlt">ultra-high</span> temperatures. In detail, αf + ξf has a non-linear dependence on temperature and varies from 6.0 × 10-6 °C-1 (20 °C) to 10.6 × 10-6 °C-1 (650 °C). Also, FBGs should be carefully used for applications at <span class="hlt">ultra-high</span> temperatures due to signal disappearance near 900 °C.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013SPIE.8910E..1KY','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013SPIE.8910E..1KY"><span>The research of digital circuit system for <span class="hlt">high</span> accuracy <span class="hlt">CCD</span> of portable Raman spectrometer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yin, Yu; Cui, Yongsheng; Zhang, Xiuda; Yan, Huimin</p> <p>2013-08-01</p> <p>The Raman spectrum technology is widely used for it can identify various types of molecular structure and material. The portable Raman spectrometer has become a hot direction of the spectrometer development nowadays for its convenience in handheld operation and real-time detection which is superior to traditional Raman spectrometer with heavy weight and bulky size. But there is still a gap for its measurement sensitivity between portable and traditional devices. However, portable Raman Spectrometer with Shell-Isolated Nanoparticle-Enhanced Raman Spectroscopy (SHINERS) technology can enhance the Raman signal significantly by several orders of magnitude, giving consideration in both measurement sensitivity and mobility. This paper proposed a design and implementation of driver and digital circuit for <span class="hlt">high</span> accuracy <span class="hlt">CCD</span> sensor, which is core part of portable spectrometer. The main target of the whole design is to reduce the dark current generation rate and increase signal sensitivity during the long integration time, and in the weak signal environment. In this case, we use back-thinned <span class="hlt">CCD</span> image sensor from Hamamatsu Corporation with <span class="hlt">high</span> sensitivity, low noise and large dynamic range. In order to maximize this <span class="hlt">CCD</span> sensor's performance and minimize the whole size of the device simultaneously to achieve the project indicators, we delicately designed a peripheral circuit for the <span class="hlt">CCD</span> sensor. The design is mainly composed with multi-voltage circuit, sequential generation circuit, driving circuit and A/D transition parts. As the most important power supply circuit, the multi-voltage circuits with 12 independent voltages are designed with reference power supply IC and set to specified voltage value by the amplifier making up the low-pass filter, which allows the user to obtain a <span class="hlt">highly</span> stable and accurate voltage with low noise. What's more, to make our design easy to debug, CPLD is selected to generate sequential signal. The A/D converter chip consists of a correlated</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4357991','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4357991"><span>Mandala Networks: <span class="hlt">ultra</span>-small-world and <span class="hlt">highly</span> sparse graphs</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Sampaio Filho, Cesar I. N.; Moreira, André A.; Andrade, Roberto F. S.; Herrmann, Hans J.; Andrade, José S.</p> <p>2015-01-01</p> <p>The increasing demands in security and reliability of infrastructures call for the optimal design of their embedded complex networks topologies. The following question then arises: what is the optimal layout to fulfill best all the demands? Here we present a general solution for this problem with scale-free networks, like the Internet and airline networks. <span class="hlt">Precisely</span>, we disclose a way to systematically construct networks which are robust against random failures. Furthermore, as the size of the network increases, its shortest path becomes asymptotically invariant and the density of links goes to zero, making it <span class="hlt">ultra</span>-small world and <span class="hlt">highly</span> sparse, respectively. The first property is ideal for communication and navigation purposes, while the second is interesting economically. Finally, we show that some simple changes on the original network formulation can lead to an improved topology against malicious attacks. PMID:25765450</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_8 --> <div id="page_9" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="161"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000115872','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000115872"><span>A Search for Planetary Transits of the Star HD 187123 by Spot Filter <span class="hlt">CCD</span> Differential Photometry</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Castellano, T.; DeVincenzi, D. (Technical Monitor)</p> <p>2000-01-01</p> <p>A novel method for performing <span class="hlt">high</span> <span class="hlt">precision</span>, time series <span class="hlt">CCD</span> differential photometry of bright stars using a spot filter, is demonstrated. Results for several nights of observing of the 51 Pegasi b-type planet bearing star HD 187123 are presented. Photometric <span class="hlt">precision</span> of 0.0015 - 0.0023 magnitudes is achieved. No transits are observed at the epochs predicted from the radial velocity observation. If the planet orbiting HD 187123 at 0.0415 AU is an inflated Jupiter similar in radius to HD 209458b it would have been detected at the greater than 6(sigma), level if the orbital inclination is near 90 degrees and at the greater than 3(sigma), level if the orbital inclination is as small as 82.7 degrees.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870023704&hterms=transfer+techniques&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dtransfer%2Btechniques','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870023704&hterms=transfer+techniques&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dtransfer%2Btechniques"><span><span class="hlt">CCD</span> charge collection efficiency and the photon transfer technique</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Janesick, J.; Klaasen, K.; Elliott, T.</p> <p>1985-01-01</p> <p>The charge-coupled device (<span class="hlt">CCD</span>) has shown unprecendented performance as a photon detector in the areas of spectral response, charge transfer, and readout noise. Recent experience indicates, however, that the full potential for the <span class="hlt">CCD</span>'s charge collection efficiency (CCE) lies well beyond that which is realized in currently available devices. A definition of CCE performance is presented and a standard test tool (the photon transfer technique) for measuring and optimizing this important <span class="hlt">CCD</span> parameter is introduced. CCE characteristics for different types of CCDs are compared; the primary limitations in achieving <span class="hlt">high</span> CCE performance are discussed, and the prospects for future improvement are outlined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040082308','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040082308"><span>Deflection Measurements of a Thermally Simulated Nuclear Core Using a <span class="hlt">High</span>-Resolution <span class="hlt">CCD</span>-Camera</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Stanojev, B. J.; Houts, M.</p> <p>2004-01-01</p> <p>Space fission systems under consideration for near-term missions all use compact. fast-spectrum reactor cores. Reactor dimensional change with increasing temperature, which affects neutron leakage. is the dominant source of reactivity feedback in these systems. Accurately measuring core dimensional changes during realistic non-nuclear testing is therefore necessary in predicting the system nuclear equivalent behavior. This paper discusses one key technique being evaluated for measuring such changes. The proposed technique is to use a Charged Couple Device (<span class="hlt">CCD</span>) sensor to obtain deformation readings of electrically heated prototypic reactor core geometry. This paper introduces a technique by which a single <span class="hlt">high</span> spatial resolution <span class="hlt">CCD</span> camera is used to measure core deformation in Real-Time (RT). Initial system checkout results are presented along with a discussion on how additional cameras could be used to achieve a three- dimensional deformation profile of the core during test.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1425004-high-performance-diesel-oxidation-catalysts-using-ultra-low-pt-loading-titania-nanowire-array-integrated-cordierite-honeycombs','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1425004-high-performance-diesel-oxidation-catalysts-using-ultra-low-pt-loading-titania-nanowire-array-integrated-cordierite-honeycombs"><span><span class="hlt">High</span> performance diesel oxidation catalysts using <span class="hlt">ultra</span>-low Pt loading on titania nanowire array integrated cordierite honeycombs</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>Hoang, Son; Lu, Xingxu; Tang, Wenxiang</p> <p></p> <p><span class="hlt">High</span> performance of an <span class="hlt">ultra</span>-low Pt loading diesel oxidation catalyst can be achieved by using a combination of novel nano-array structured support, <span class="hlt">precise</span> control of ultrafine active Pt particles, and an addition of H 2 as a promoter into the exhausts. <span class="hlt">Highly</span> stable mesoporous rutile TiO 2 nano-array was uniformly grown on three-dimensional (3-D) cordierite honeycomb monoliths using a solvothermal synthesis. Atomic layer deposition was employed for <span class="hlt">precise</span> dispersion of ultrafine Pt particles (0.95 ± 0.24 nm) on TiO 2 nano-array with a Pt loading of 1.1 g/ft 3. Despite low Pt loading, the Pt/TiO 2 nano-array catalyst shows impressivemore » low-temperature oxidation reactivity, with the conversion of CO and total hydrocarbon (THC) reaching 50% at 224 and 285 °C, respectively, in the clean diesel combustion (CDC) simulated exhaust conditions. The excellent activity is attributed to the unique nano-array structure that promotes gas-solid interaction and <span class="hlt">ultra</span>-small Pt particle dispersion that increase surface Pt atoms. We also demonstrate that addition of more H 2 into the exhaust can lower light-off temperature for CO and THC by up to ~60 °C and ~30 °C, respectively.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1425004-high-performance-diesel-oxidation-catalysts-using-ultra-low-pt-loading-titania-nanowire-array-integrated-cordierite-honeycombs','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1425004-high-performance-diesel-oxidation-catalysts-using-ultra-low-pt-loading-titania-nanowire-array-integrated-cordierite-honeycombs"><span><span class="hlt">High</span> performance diesel oxidation catalysts using <span class="hlt">ultra</span>-low Pt loading on titania nanowire array integrated cordierite honeycombs</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Hoang, Son; Lu, Xingxu; Tang, Wenxiang; ...</p> <p>2017-11-15</p> <p><span class="hlt">High</span> performance of an <span class="hlt">ultra</span>-low Pt loading diesel oxidation catalyst can be achieved by using a combination of novel nano-array structured support, <span class="hlt">precise</span> control of ultrafine active Pt particles, and an addition of H 2 as a promoter into the exhausts. <span class="hlt">Highly</span> stable mesoporous rutile TiO 2 nano-array was uniformly grown on three-dimensional (3-D) cordierite honeycomb monoliths using a solvothermal synthesis. Atomic layer deposition was employed for <span class="hlt">precise</span> dispersion of ultrafine Pt particles (0.95 ± 0.24 nm) on TiO 2 nano-array with a Pt loading of 1.1 g/ft 3. Despite low Pt loading, the Pt/TiO 2 nano-array catalyst shows impressivemore » low-temperature oxidation reactivity, with the conversion of CO and total hydrocarbon (THC) reaching 50% at 224 and 285 °C, respectively, in the clean diesel combustion (CDC) simulated exhaust conditions. The excellent activity is attributed to the unique nano-array structure that promotes gas-solid interaction and <span class="hlt">ultra</span>-small Pt particle dispersion that increase surface Pt atoms. We also demonstrate that addition of more H 2 into the exhaust can lower light-off temperature for CO and THC by up to ~60 °C and ~30 °C, respectively.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790017148','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790017148"><span><span class="hlt">CCD</span> research. [design, fabrication, and applications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gassaway, J. D.</p> <p>1976-01-01</p> <p>The fundamental problems encountered in designing, fabricating, and applying <span class="hlt">CCD</span>'s are reviewed. Investigations are described and results and conclusions are given for the following: (1) the development of design analyses employing computer aided techniques and their application to the design of a grapped structure; (2) the role of <span class="hlt">CCD</span>'s in applications to electronic functions, in particular, signal processing; (3) extending the <span class="hlt">CCD</span> to silicon films on sapphire (SOS); and (4) all aluminum transfer structure with low noise input-output circuits. Related work on <span class="hlt">CCD</span> imaging devices is summarized.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/874209','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/874209"><span>Printed circuit board for a <span class="hlt">CCD</span> camera head</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Conder, Alan D.</p> <p>2002-01-01</p> <p>A charge-coupled device (<span class="hlt">CCD</span>) camera head which can replace film for digital imaging of visible light, ultraviolet radiation, and soft to penetrating x-rays, such as within a target chamber where laser produced plasmas are studied. The camera head is small, capable of operating both in and out of a vacuum environment, and is versatile. The <span class="hlt">CCD</span> camera head uses PC boards with an internal heat sink connected to the chassis for heat dissipation, which allows for close (0.04" for example) stacking of the PC boards. Integration of this <span class="hlt">CCD</span> camera head into existing instrumentation provides a substantial enhancement of diagnostic capabilities for studying <span class="hlt">high</span> energy density plasmas, for a variety of military industrial, and medical imaging applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090028695','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090028695"><span><span class="hlt">Ultra-high</span> Temperature Emittance Measurements for Space and Missile Applications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rogers, Jan; Crandall, David</p> <p>2009-01-01</p> <p>Advanced modeling and design efforts for many aerospace components require <span class="hlt">high</span> temperature emittance data. Applications requiring emittance data include propulsion systems, radiators, aeroshells, heatshields/thermal protection systems, and leading edge surfaces. The objective of this work is to provide emittance data at <span class="hlt">ultra-high</span> temperatures. MSFC has a new instrument for the measurement of emittance at <span class="hlt">ultra-high</span> temperatures, the <span class="hlt">Ultra-High</span> Temperature Emissometer System (<span class="hlt">Ultra</span>-HITEMS). AZ Technology Inc. developed the instrument, designed to provide emittance measurements over the temperature range 700-3500K. The <span class="hlt">Ultra</span>-HITEMS instrument measures the emittance of samples, heated by lasers, in vacuum, using a blackbody source and a Fourier Transform Spectrometer. Detectors in a Nicolet 6700 FT-IR spectrometer measure emittance over the spectral range of 0.4-25 microns. Emitted energy from the specimen and output from a Mikron M390S blackbody source at the same temperature with matched collection geometry are measured. Integrating emittance over the spectral range yields the total emittance. The ratio provides a direct measure of total hemispherical emittance. Samples are heated using lasers. Optical pyrometry provides temperature data. Optical filters prevent interference from the heating lasers. Data for Inconel 718 show excellent agreement with results from literature and ASTM 835. Measurements taken from levitated spherical specimens provide total hemispherical emittance data; measurements taken from flat specimens mounted in the chamber provide near-normal emittance data. Data from selected characterization studies will be presented. The <span class="hlt">Ultra</span>-HITEMS technique could advance space and missile technologies by advancing the knowledge base and the technology readiness level for <span class="hlt">ultra-high</span> temperature materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22482680-note-ultra-low-birefringence-dodecagonal-vacuum-glass-cell','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22482680-note-ultra-low-birefringence-dodecagonal-vacuum-glass-cell"><span>Note: <span class="hlt">Ultra</span>-low birefringence dodecagonal vacuum glass cell</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>Brakhane, Stefan, E-mail: brakhane@iap.uni-bonn.de; Alt, Wolfgang; Meschede, Dieter</p> <p></p> <p>We report on an <span class="hlt">ultra</span>-low birefringence dodecagonal glass cell for <span class="hlt">ultra-high</span> vacuum applications. The epoxy-bonded trapezoidal windows of the cell are made of SF57 glass, which exhibits a very low stress-induced birefringence. We characterize the birefringence Δn of each window with the cell under vacuum conditions, obtaining values around 10{sup −8}. After baking the cell at 150 °C, we reach a pressure below 10{sup −10} mbar. In addition, each window is antireflection coated on both sides, which is <span class="hlt">highly</span> desirable for quantum optics experiments and <span class="hlt">precision</span> measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090016243','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090016243"><span>Chromatic Modulator for a <span class="hlt">High</span>-Resolution <span class="hlt">CCD</span> or APS</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hartley, Frank; Hull, Anthony</p> <p>2008-01-01</p> <p>A chromatic modulator has been proposed to enable the separate detection of the red, green, and blue (RGB) color components of the same scene by a single charge-coupled device (<span class="hlt">CCD</span>), active-pixel sensor (APS), or similar electronic image detector. Traditionally, the RGB color-separation problem in an electronic camera has been solved by use of either (1) fixed color filters over three separate image detectors; (2) a filter wheel that repeatedly imposes a red, then a green, then a blue filter over a single image detector; or (3) different fixed color filters over adjacent pixels. The use of separate image detectors necessitates <span class="hlt">precise</span> registration of the detectors and the use of complicated optics; filter wheels are expensive and add considerably to the bulk of the camera; and fixed pixelated color filters reduce spatial resolution and introduce color-aliasing effects. The proposed chromatic modulator would not exhibit any of these shortcomings. The proposed chromatic modulator would be an electromechanical device fabricated by micromachining. It would include a filter having a spatially periodic pattern of RGB strips at a pitch equal to that of the pixels of the image detector. The filter would be placed in front of the image detector, supported at its periphery by a spring suspension and electrostatic comb drive. The spring suspension would bias the filter toward a middle position in which each filter strip would be registered with a row of pixels of the image detector. Hard stops would limit the excursion of the spring suspension to <span class="hlt">precisely</span> one pixel row above and one pixel row below the middle position. In operation, the electrostatic comb drive would be actuated to repeatedly snap the filter to the upper extreme, middle, and lower extreme positions. This action would repeatedly place a succession of the differently colored filter strips in front of each pixel of the image detector. To simplify the processing, it would be desirable to encode information on</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NIMPA.880...28B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NIMPA.880...28B"><span>C2D8: An eight channel <span class="hlt">CCD</span> readout electronics dedicated to low energy neutron detection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bourrion, O.; Clement, B.; Tourres, D.; Pignol, G.; Xi, Y.; Rebreyend, D.; Nesvizhevsky, V. V.</p> <p>2018-02-01</p> <p>Position-sensitive detectors for cold and <span class="hlt">ultra</span>-cold neutrons (UCN) are in use in fundamental research. In particular, measuring the properties of the quantum states of bouncing neutrons requires micro-metric spatial resolution. To this end, a Charge Coupled Device (<span class="hlt">CCD</span>) coated with a thin conversion layer that allows a real time detection of neutron hits is under development at LPSC. In this paper, we present the design and performance of a dedicated electronic board designed to read-out eight CCDs simultaneously and operating under vacuum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9944E..0NT','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9944E..0NT"><span>Organic field effect transistor with <span class="hlt">ultra</span> <span class="hlt">high</span> amplification</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Torricelli, Fabrizio</p> <p>2016-09-01</p> <p><span class="hlt">High</span>-gain transistors are essential for the large-scale circuit integration, <span class="hlt">high</span>-sensitivity sensors and signal amplification in sensing systems. Unfortunately, organic field-effect transistors show limited gain, usually of the order of tens, because of the large contact resistance and channel-length modulation. Here we show organic transistors fabricated on plastic foils enabling unipolar amplifiers with <span class="hlt">ultra</span>-gain. The proposed approach is general and opens up new opportunities for <span class="hlt">ultra</span>-large signal amplification in organic circuits and sensors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JDSO...13...52H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JDSO...13...52H"><span>The Speckle Toolbox: A Powerful Data Reduction Tool for <span class="hlt">CCD</span> Astrometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harshaw, Richard; Rowe, David; Genet, Russell</p> <p>2017-01-01</p> <p>Recent advances in <span class="hlt">high</span>-speed low-noise <span class="hlt">CCD</span> and CMOS cameras, coupled with breakthroughs in data reduction software that runs on desktop PCs, has opened the domain of speckle interferometry and <span class="hlt">high</span>-accuracy <span class="hlt">CCD</span> measurements of double stars to amateurs, allowing them to do useful science of <span class="hlt">high</span> quality. This paper describes how to use a speckle interferometry reduction program, the Speckle Tool Box (STB), to achieve this level of result. For over a year the author (Harshaw) has been using STB (and its predecessor, Plate Solve 3) to obtain measurements of double stars based on <span class="hlt">CCD</span> camera technology for pairs that are either too wide (the stars not sharing the same isoplanatic patch, roughly 5 arc-seconds in diameter) or too faint to image in the coherence time required for speckle (usually under 40ms). This same approach - using speckle reduction software to measure <span class="hlt">CCD</span> pairs with greater accuracy than possible with lucky imaging - has been used, it turns out, for several years by the U. S. Naval Observatory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5509964','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5509964"><span>Formal thought disorder in people at <span class="hlt">ultra-high</span> risk of psychosis</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Weinstein, Sara; Stahl, Daniel; Day, Fern; Valmaggia, Lucia; Rutigliano, Grazia; De Micheli, Andrea; Fusar-Poli, Paolo; McGuire, Philip</p> <p>2017-01-01</p> <p>Background Formal thought disorder is a cardinal feature of psychosis. However, the extent to which formal thought disorder is evident in <span class="hlt">ultra-high</span>-risk individuals and whether it is linked to the progression to psychosis remains unclear. Aims Examine the severity of formal thought disorder in <span class="hlt">ultra-high</span>-risk participants and its association with future psychosis. Method The Thought and Language Index (TLI) was used to assess 24 <span class="hlt">ultra-high</span>-risk participants, 16 people with first-episode psychosis and 13 healthy controls. <span class="hlt">Ultra-high</span>-risk individuals were followed up for a mean duration of 7 years (s.d.=1.5) to determine the relationship between formal thought disorder at baseline and transition to psychosis. Results TLI scores were significantly greater in the <span class="hlt">ultra-high</span>-risk group compared with the healthy control group (effect size (ES)=1.2), but lower than in people with first-episode psychosis (ES=0.8). Total and negative TLI scores were higher in <span class="hlt">ultra-high</span>-risk individuals who developed psychosis, but this was not significant. Combining negative TLI scores with attenuated psychotic symptoms and basic symptoms predicted transition to psychosis (P=0.04; ES=1.04). Conclusions TLI is beneficial in evaluating formal thought disorder in <span class="hlt">ultra-high</span>-risk participants, and complements existing instruments for the evaluation of psychopathology in this group. Declaration of interests None. Copyright and usage © The Royal College of Psychiatrists 2017. This is an open access article distributed under the terms of the Creative Commons Non-Commercial, No Derivatives (CC BY-NC-ND) license. PMID:28713586</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997SPIE.3114..155K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997SPIE.3114..155K"><span>PN-<span class="hlt">CCD</span> camera for XMM: performance of <span class="hlt">high</span> time resolution/bright source operating modes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kendziorra, Eckhard; Bihler, Edgar; Grubmiller, Willy; Kretschmar, Baerbel; Kuster, Markus; Pflueger, Bernhard; Staubert, Ruediger; Braeuninger, Heinrich W.; Briel, Ulrich G.; Meidinger, Norbert; Pfeffermann, Elmar; Reppin, Claus; Stoetter, Diana; Strueder, Lothar; Holl, Peter; Kemmer, Josef; Soltau, Heike; von Zanthier, Christoph</p> <p>1997-10-01</p> <p>The pn-<span class="hlt">CCD</span> camera is developed as one of the focal plane instruments for the European photon imaging camera (EPIC) on board the x-ray multi mirror (XMM) mission to be launched in 1999. The detector consists of four quadrants of three pn-CCDs each, which are integrated on one silicon wafer. Each <span class="hlt">CCD</span> has 200 by 64 pixels (150 micrometer by 150 micrometers) with 280 micrometers depletion depth. One <span class="hlt">CCD</span> of a quadrant is read out at a time, while the four quadrants can be processed independently of each other. In standard imaging mode the CCDs are read out sequentially every 70 ms. Observations of point sources brighter than 1 mCrab will be effected by photon pile- up. However, special operating modes can be used to observe bright sources up to 150 mCrab in timing mode with 30 microseconds time resolution and very bright sources up to several crab in burst mode with 7 microseconds time resolution. We have tested one quadrant of the EPIC pn-<span class="hlt">CCD</span> camera at line energies from 0.52 keV to 17.4 keV at the long beam test facility Panter in the focus of the qualification mirror module for XMM. In order to test the time resolution of the system, a mechanical chopper was used to periodically modulate the beam intensity. Pulse periods down to 0.7 ms were generated. This paper describes the performance of the pn-<span class="hlt">CCD</span> detector in timing and burst readout modes with special emphasis on energy and time resolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080004673','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080004673"><span>Using a delta-doped <span class="hlt">CCD</span> to determine the energy of a low-energy particle</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nikzad, Shouleh (Inventor); Croley, Donald R. (Inventor); Murphy, Gerald B. (Inventor)</p> <p>2001-01-01</p> <p>The back surface of a thinned charged-coupled device (<span class="hlt">CCD</span>) is treated to eliminate the backside potential well that appears in a conventional thinned <span class="hlt">CCD</span> during backside illumination. The backside of the <span class="hlt">CCD</span> includes a delta layer of <span class="hlt">high</span>-concentration dopant confined to less than one monolayer of the crystal semiconductor. The thinned, delta-doped <span class="hlt">CCD</span> is used to determine the energy of a very low-energy particle that penetrates less than 1.0 nm into the <span class="hlt">CCD</span>, such as a proton having energy less than 10 keV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012SPIE.8453E..1AI','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012SPIE.8453E..1AI"><span>A compact <span class="hlt">high</span>-speed pn<span class="hlt">CCD</span> camera for optical and x-ray applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ihle, Sebastian; Ordavo, Ivan; Bechteler, Alois; Hartmann, Robert; Holl, Peter; Liebel, Andreas; Meidinger, Norbert; Soltau, Heike; Strüder, Lothar; Weber, Udo</p> <p>2012-07-01</p> <p>We developed a camera with a 264 × 264 pixel pn<span class="hlt">CCD</span> of 48 μm size (thickness 450 μm) for X-ray and optical applications. It has a <span class="hlt">high</span> quantum efficiency and can be operated up to 400 / 1000 Hz (noise≍ 2:5 ° ENC / ≍4:0 ° ENC). <span class="hlt">High</span>-speed astronomical observations can be performed with low light levels. Results of test measurements will be presented. The camera is well suitable for ground based preparation measurements for future X-ray missions. For X-ray single photons, the spatial position can be determined with significant sub-pixel resolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998SPIE.3301...27V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998SPIE.3301...27V"><span>6 x 6-cm fully depleted pn-junction <span class="hlt">CCD</span> for <span class="hlt">high</span>-resolution spectroscopy in the 0.1- to 15-keV photon energy range</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>von Zanthier, Christoph; Holl, Peter; Kemmer, Josef; Lechner, Peter; Maier, B.; Soltau, Heike; Stoetter, R.; Braeuninger, Heinrich W.; Dennerl, Konrad; Haberl, Frank; Hartmann, R.; Hartner, Gisela D.; Hippmann, H.; Kastelic, E.; Kink, W.; Krause, N.; Meidinger, Norbert; Metzner, G.; Pfeffermann, Elmar; Popp, M.; Reppin, Claus; Stoetter, Diana; Strueder, Lothar; Truemper, Joachim; Weber, U.; Carathanassis, D.; Engelhard, S.; Gebhart, Th.; Hauff, D.; Lutz, G.; Richter, R. H.; Seitz, H.; Solc, P.; Bihler, Edgar; Boettcher, H.; Kendziorra, Eckhard; Kraemer, J.; Pflueger, Bernhard; Staubert, Ruediger</p> <p>1998-04-01</p> <p>The concept and performance of the fully depleted pn- junction <span class="hlt">CCD</span> system, developed for the European XMM- and the German ABRIXAS-satellite missions for soft x-ray imaging and spectroscopy in the 0.1 keV to 15 keV photon range, is presented. The 58 mm X 60 mm large pn-<span class="hlt">CCD</span> array uses pn- junctions for registers and for the backside instead of MOS registers. This concept naturally allows to fully deplete the detector volume to make it an efficient detector to photons with energies up to 15 keV. For <span class="hlt">high</span> detection efficiency in the soft x-ray region down to 100 eV, an ultrathin pn-<span class="hlt">CCD</span> backside deadlayer has been realized. Each pn-<span class="hlt">CCD</span>-channel is equipped with an on-chip JFET amplifier which, in combination with the CAMEX-amplifier and multiplexing chip, facilitates parallel readout with a pixel read rate of 3 MHz and an electronic noise floor of ENC < e-. With the complete parallel readout, very fast pn-<span class="hlt">CCD</span> readout modi can be implemented in the system which allow for <span class="hlt">high</span> resolution photon spectroscopy of even the brightest x-ray sources in the sky.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009SPIE.7439E..05S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009SPIE.7439E..05S"><span>Modelling electron distributions within ESA's Gaia satellite <span class="hlt">CCD</span> pixels to mitigate radiation damage</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Seabroke, G. M.; Holland, A. D.; Burt, D.; Robbins, M. S.</p> <p>2009-08-01</p> <p>The Gaia satellite is a <span class="hlt">high-precision</span> astrometry, photometry and spectroscopic ESA cornerstone mission, currently scheduled for launch in 2012. Its primary science drivers are the composition, formation and evolution of the Galaxy. Gaia will achieve its unprecedented positional accuracy requirements with detailed calibration and correction for radiation damage. At L2, protons cause displacement damage in the silicon of CCDs. The resulting traps capture and emit electrons from passing charge packets in the <span class="hlt">CCD</span> pixel, distorting the image PSF and biasing its centroid. Microscopic models of Gaia's CCDs are being developed to simulate this effect. The key to calculating the probability of an electron being captured by a trap is the 3D electron density within each <span class="hlt">CCD</span> pixel. However, this has not been physically modelled for the Gaia <span class="hlt">CCD</span> pixels. In Seabroke, Holland & Cropper (2008), the first paper of this series, we motivated the need for such specialised 3D device modelling and outlined how its future results will fit into Gaia's overall radiation calibration strategy. In this paper, the second of the series, we present our first results using Silvaco's physics-based, engineering software: the ATLAS device simulation framework. Inputting a doping profile, pixel geometry and materials into ATLAS and comparing the results to other simulations reveals that ATLAS has a free parameter, fixed oxide charge, that needs to be calibrated. ATLAS is successfully benchmarked against other simulations and measurements of a test device, identifying how to use it to model Gaia pixels and highlighting the affect of different doping approximations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003ChPhL..20..806X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003ChPhL..20..806X"><span><span class="hlt">Ultra</span> <span class="hlt">High</span> Energy Cosmic Rays: Strangelets?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Ren-Xin; Wu, Fei</p> <p>2003-06-01</p> <p>The conjecture that <span class="hlt">ultra-high</span>-energy cosmic rays (UHECRs) are actually strangelets is discussed. Besides the reason that strangelets can do as cosmic rays beyond the Greisen-Zatsepin-Kuzmin-cutoff, another argument to support the conjecture is addressed by the study of formation of TeV-scale microscopic black holes when UHECRs bombarding bare strange stars. It is proposed that the exotic quark surface of a bare strange star could be an effective astro-laboratory in the investigations of the extra dimensions and of the detection of <span class="hlt">ultra-high</span>-energy neutrino fluxes. The flux of neutrinos (and other point-like particles) with energy larger than 2.3×1020 eV could be expected to be smaller than 10-26 cm-2 s-1 if there are two extra spatial dimensions.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_9 --> <div id="page_10" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="181"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997AJ....113.1925Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997AJ....113.1925Z"><span>Astrometric Quality of the USNO <span class="hlt">CCD</span> Astrograph (UCA)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zacharias, N.</p> <p>1997-05-01</p> <p>The USNO 8-inch astrograph has been equipped with a Kodak 1536x1024 pixel <span class="hlt">CCD</span> since June 1995, operating in a 570-650 nm bandpass. With 3-minute exposures well exposed images are obtained in the magnitude range R ~ 8.5 - 13.5(m) . An astrometric <span class="hlt">precision</span> of 10 to 15 mas for those stars is estimated from frame-to-frame comparisons. External comparisons reveal an accuracy of about 15 mas for those stars in a 20' field of view. For fainter stars, the error budget is dominated by the S/N ratio, reaching ~ 100 mas at R=16(m) under good observing conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010IJMPA..25..909A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010IJMPA..25..909A"><span>QCD <span class="hlt">Precision</span> Measurements and Structure Function Extraction at a <span class="hlt">High</span> Statistics, <span class="hlt">High</span> Energy Neutrino Scattering Experiment:. NuSOnG</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Adams, T.; Batra, P.; Bugel, L.; Camilleri, L.; Conrad, J. M.; de Gouvêa, A.; Fisher, P. H.; Formaggio, J. A.; Jenkins, J.; Karagiorgi, G.; Kobilarcik, T. R.; Kopp, S.; Kyle, G.; Loinaz, W. A.; Mason, D. A.; Milner, R.; Moore, R.; Morfín, J. G.; Nakamura, M.; Naples, D.; Nienaber, P.; Olness, F. I.; Owens, J. F.; Pate, S. F.; Pronin, A.; Seligman, W. G.; Shaevitz, M. H.; Schellman, H.; Schienbein, I.; Syphers, M. J.; Tait, T. M. P.; Takeuchi, T.; Tan, C. Y.; van de Water, R. G.; Yamamoto, R. K.; Yu, J. Y.</p> <p></p> <p>We extend the physics case for a new <span class="hlt">high</span>-energy, <span class="hlt">ultra-high</span> statistics neutrino scattering experiment, NuSOnG (Neutrino Scattering On Glass) to address a variety of issues including <span class="hlt">precision</span> QCD measurements, extraction of structure functions, and the derived Parton Distribution Functions (PDF's). This experiment uses a Tevatron-based neutrino beam to obtain a sample of Deep Inelastic Scattering (DIS) events which is over two orders of magnitude larger than past samples. We outline an innovative method for fitting the structure functions using a parametrized energy shift which yields reduced systematic uncertainties. <span class="hlt">High</span> statistics measurements, in combination with improved systematics, will enable NuSOnG to perform discerning tests of fundamental Standard Model parameters as we search for deviations which may hint of "Beyond the Standard Model" physics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AJ....153...77C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AJ....153...77C"><span>AstroImageJ: Image Processing and Photometric Extraction for <span class="hlt">Ultra-precise</span> Astronomical Light Curves</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Collins, Karen A.; Kielkopf, John F.; Stassun, Keivan G.; Hessman, Frederic V.</p> <p>2017-02-01</p> <p>ImageJ is a graphical user interface (GUI) driven, public domain, Java-based, software package for general image processing traditionally used mainly in life sciences fields. The image processing capabilities of ImageJ are useful and extendable to other scientific fields. Here we present AstroImageJ (AIJ), which provides an astronomy specific image display environment and tools for astronomy specific image calibration and data reduction. Although AIJ maintains the general purpose image processing capabilities of ImageJ, AIJ is streamlined for time-series differential photometry, light curve detrending and fitting, and light curve plotting, especially for applications requiring <span class="hlt">ultra-precise</span> light curves (e.g., exoplanet transits). AIJ reads and writes standard Flexible Image Transport System (FITS) files, as well as other common image formats, provides FITS header viewing and editing, and is World Coordinate System aware, including an automated interface to the astrometry.net web portal for plate solving images. AIJ provides research grade image calibration and analysis tools with a GUI driven approach, and easily installed cross-platform compatibility. It enables new users, even at the level of undergraduate student, <span class="hlt">high</span> school student, or amateur astronomer, to quickly start processing, modeling, and plotting astronomical image data with one tightly integrated software package.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27090589','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27090589"><span><span class="hlt">Ultra</span>-low fouling and <span class="hlt">high</span> antibody loading zwitterionic hydrogel coatings for sensing and detection in complex media.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chou, Ying-Nien; Sun, Fang; Hung, Hsiang-Chieh; Jain, Priyesh; Sinclair, Andrew; Zhang, Peng; Bai, Tao; Chang, Yung; Wen, Ten-Chin; Yu, Qiuming; Jiang, Shaoyi</p> <p>2016-08-01</p> <p>For surface-based diagnostic devices to achieve reliable biomarker detection in complex media such as blood, preventing nonspecific protein adsorption and incorporating <span class="hlt">high</span> loading of biorecognition elements are paramount. In this work, a novel method to produce nonfouling zwitterionic hydrogel coatings was developed to achieve these goals. Poly(carboxybetaine acrylamide) (pCBAA) hydrogel thin films (CBHTFs) prepared with a carboxybetaine diacrylamide crosslinker (CBAAX) were coated on gold and silicon dioxide surfaces via a simple spin coating process. The thickness of CBHTFs could be <span class="hlt">precisely</span> controlled between 15 and 150nm by varying the crosslinker concentration, and the films demonstrated excellent long-term stability. Protein adsorption from undiluted human blood serum onto the CBHTFs was measured with surface plasmon resonance (SPR). Hydrogel thin films greater than 20nm exhibited <span class="hlt">ultra</span>-low fouling (<5ng/cm(2)). In addition, the CBHTFs were capable of <span class="hlt">high</span> antibody functionalization for specific biomarker detection without compromising their nonfouling performance. This strategy provides a facile method to modify SPR biosensor chips with an advanced nonfouling material, and can be potentially expanded to a variety of implantable medical devices and diagnostic biosensors. In this work, we developed an approach to realize <span class="hlt">ultra</span>-low fouling and <span class="hlt">high</span> ligand loading with a <span class="hlt">highly</span>-crosslinked, purely zwitterionic, carboxybetaine thin film hydrogel (CBHTF) coating platform. The CBHTF on a hydrophilic surface demonstrated long-term stability. By varying the crosslinker content in the spin-coated hydrogel solution, the thickness of CBHTFs could be <span class="hlt">precisely</span> controlled. Optimized CBHTFs exhibited <span class="hlt">ultra</span>-low nonspecific protein adsorption below 5ng/cm(2) measured by a surface plasmon resonance (SPR) sensor, and their 3D architecture allowed antibody loading to reach 693ng/cm(2). This strategy provides a facile method to modify SPR biosensor chips with an advanced</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9555E..0NE','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9555E..0NE"><span>Fusion: <span class="hlt">ultra-high</span>-speed and IR image sensors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Etoh, T. Goji; Dao, V. T. S.; Nguyen, Quang A.; Kimata, M.</p> <p>2015-08-01</p> <p>Most targets of <span class="hlt">ultra-high</span>-speed video cameras operating at more than 1 Mfps, such as combustion, crack propagation, collision, plasma, spark discharge, an air bag at a car accident and a tire under a sudden brake, generate sudden heat. Researchers in these fields require tools to measure the <span class="hlt">high</span>-speed motion and heat simultaneously. <span class="hlt">Ultra-high</span> frame rate imaging is achieved by an in-situ storage image sensor. Each pixel of the sensor is equipped with multiple memory elements to record a series of image signals simultaneously at all pixels. Image signals stored in each pixel are read out after an image capturing operation. In 2002, we developed an in-situ storage image sensor operating at 1 Mfps 1). However, the fill factor of the sensor was only 15% due to a light shield covering the wide in-situ storage area. Therefore, in 2011, we developed a backside illuminated (BSI) in-situ storage image sensor to increase the sensitivity with 100% fill factor and a very <span class="hlt">high</span> quantum efficiency 2). The sensor also achieved a much higher frame rate,16.7 Mfps, thanks to the wiring on the front side with more freedom 3). The BSI structure has another advantage that it has less difficulties in attaching an additional layer on the backside, such as scintillators. This paper proposes development of an <span class="hlt">ultra-high</span>-speed IR image sensor in combination of advanced nano-technologies for IR imaging and the in-situ storage technology for <span class="hlt">ultra</span>-highspeed imaging with discussion on issues in the integration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PASP..129l5001S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PASP..129l5001S"><span>A Low-cost Environmental Control System for <span class="hlt">Precise</span> Radial Velocity Spectrometers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sliski, David H.; Blake, Cullen H.; Halverson, Samuel</p> <p>2017-12-01</p> <p>We present an environmental control system (ECS) designed to achieve milliKelvin (mK) level temperature stability for small-scale astronomical instruments. This ECS is inexpensive and is primarily built from commercially available components. The primary application for our ECS is the <span class="hlt">high-precision</span> Doppler spectrometer MINERVA-Red, where the thermal variations of the optical components within the instrument represent a major source of systematic error. We demonstrate ±2 mK temperature stability within a 0.5 m3 thermal enclosure using resistive heaters in conjunction with a commercially available PID controller and off-the-shelf thermal sensors. The enclosure is maintained above ambient temperature, enabling rapid cooling through heat dissipation into the surrounding environment. We demonstrate peak-to-valley (PV) temperature stability of better than 5 mK within the MINERVA-Red vacuum chamber, which is located inside the thermal enclosure, despite large temperature swings in the ambient laboratory environment. During periods of stable laboratory conditions, the PV variations within the vacuum chamber are less than 3 mK. This temperature stability is comparable to the best stability demonstrated for Doppler spectrometers currently achieving m s-1 radial velocity <span class="hlt">precision</span>. We discuss the challenges of using commercially available thermoelectrically cooled <span class="hlt">CCD</span> cameras in a temperature-stabilized environment, and demonstrate that the effects of variable heat output from the <span class="hlt">CCD</span> camera body can be mitigated using PID-controlled chilled water systems. The ECS presented here could potentially provide the stable operating environment required for future compact “astrophotonic” <span class="hlt">precise</span> radial velocity (PRV) spectrometers to achieve <span class="hlt">high</span> Doppler measurement <span class="hlt">precision</span> with a modest budget.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APh....84...82P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APh....84...82P"><span>GEM-based TPC with <span class="hlt">CCD</span> imaging for directional dark matter detection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Phan, N. S.; Lauer, R. J.; Lee, E. R.; Loomba, D.; Matthews, J. A. J.; Miller, E. H.</p> <p>2016-11-01</p> <p>The most mature directional dark matter experiments at present all utilize low-pressure gas Time Projection Chamber (TPC) technologies. We discuss some of the challenges for this technology, for which balancing the goal of achieving the best sensitivity with that of cost effective scale-up requires optimization over a large parameter space. Critical for this are the <span class="hlt">precision</span> measurements of the fundamental properties of both electron and nuclear recoil tracks down to the lowest detectable energies. Such measurements are necessary to provide a benchmark for background discrimination and directional sensitivity that could be used for future optimization studies for directional dark matter experiments. In this paper we describe a small, <span class="hlt">high</span> resolution, <span class="hlt">high</span> signal-to-noise GEM-based TPC with a 2D <span class="hlt">CCD</span> readout designed for this goal. The performance of the detector was characterized using alpha particles, X-rays, gamma-rays, and neutrons, enabling detailed measurements of electron and nuclear recoil tracks. Stable effective gas gains of greater than 1 × 105 were obtained in 100 Torr of pure CF4 by a cascade of three standard CERN GEMs each with a 140 μm pitch. The <span class="hlt">high</span> signal-to-noise and sub-millimeter spatial resolution of the GEM amplification and <span class="hlt">CCD</span> readout, together with low diffusion, allow for excellent background discrimination between electron and nuclear recoils down below ∼10 keVee (∼23 keVr fluorine recoil). Even lower thresholds, necessary for the detection of low mass WIMPs for example, might be achieved by lowering the pressure and utilizing full 3D track reconstruction. These and other paths for improvements are discussed, as are possible fundamental limitations imposed by the physics of energy loss.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25359822','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25359822"><span>Fast auto-acquisition tomography tilt series by using HD video camera in <span class="hlt">ultra-high</span> voltage electron microscope.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nishi, Ryuji; Cao, Meng; Kanaji, Atsuko; Nishida, Tomoki; Yoshida, Kiyokazu; Isakozawa, Shigeto</p> <p>2014-11-01</p> <p>The <span class="hlt">ultra-high</span> voltage electron microscope (UHVEM) H-3000 with the world highest acceleration voltage of 3 MV can observe remarkable three dimensional microstructures of microns-thick samples[1]. Acquiring a tilt series of electron tomography is laborious work and thus an automatic technique is <span class="hlt">highly</span> desired. We proposed the Auto-Focus system using image Sharpness (AFS)[2,3] for UHVEM tomography tilt series acquisition. In the method, five images with different defocus values are firstly acquired and the image sharpness are calculated. The sharpness are then fitted to a quasi-Gaussian function to decide the best focus value[3]. Defocused images acquired by the slow scan <span class="hlt">CCD</span> (SS-<span class="hlt">CCD</span>) camera (Hitachi F486BK) are of <span class="hlt">high</span> quality but one minute is taken for acquisition of five defocused images.In this study, we introduce a <span class="hlt">high</span>-definition video camera (HD video camera; Hamamatsu Photonics K. K. C9721S) for fast acquisition of images[4]. It is an analog camera but the camera image is captured by a PC and the effective image resolution is 1280×1023 pixels. This resolution is lower than that of the SS-<span class="hlt">CCD</span> camera of 4096×4096 pixels. However, the HD video camera captures one image for only 1/30 second. In exchange for the faster acquisition the S/N of images are low. To improve the S/N, 22 captured frames are integrated so that each image sharpness is enough to become lower fitting error. As countermeasure against low resolution, we selected a large defocus step, which is typically five times of the manual defocus step, to discriminate different defocused images.By using HD video camera for autofocus process, the time consumption for each autofocus procedure was reduced to about six seconds. It took one second for correction of an image position and the total correction time was seven seconds, which was shorter by one order than that using SS-<span class="hlt">CCD</span> camera. When we used SS-<span class="hlt">CCD</span> camera for final image capture, it took 30 seconds to record one tilt image. We can obtain a tilt</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009MeScT..20j4007B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009MeScT..20j4007B"><span><span class="hlt">High-precision</span> shape representation using a neuromorphic vision sensor with synchronous address-event communication interface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Belbachir, A. N.; Hofstätter, M.; Litzenberger, M.; Schön, P.</p> <p>2009-10-01</p> <p>A synchronous communication interface for neuromorphic temporal contrast vision sensors is described and evaluated in this paper. This interface has been designed for <span class="hlt">ultra</span> <span class="hlt">high</span>-speed synchronous arbitration of a temporal contrast image sensors pixels' data. Enabling <span class="hlt">high-precision</span> timestamping, this system demonstrates its uniqueness for handling peak data rates and preserving the main advantage of the neuromorphic electronic systems, that is <span class="hlt">high</span> and accurate temporal resolution. Based on a synchronous arbitration concept, the timestamping has a resolution of 100 ns. Both synchronous and (state-of-the-art) asynchronous arbiters have been implemented in a neuromorphic dual-line vision sensor chip in a standard 0.35 µm CMOS process. The performance analysis of both arbiters and the advantages of the synchronous arbitration over asynchronous arbitration in capturing <span class="hlt">high</span>-speed objects are discussed in detail.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013NIMPA.731..160M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013NIMPA.731..160M"><span>Proton radiation damage experiment on P-Channel <span class="hlt">CCD</span> for an X-ray <span class="hlt">CCD</span> camera onboard the ASTRO-H satellite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mori, Koji; Nishioka, Yusuke; Ohura, Satoshi; Koura, Yoshiaki; Yamauchi, Makoto; Nakajima, Hiroshi; Ueda, Shutaro; Kan, Hiroaki; Anabuki, Naohisa; Nagino, Ryo; Hayashida, Kiyoshi; Tsunemi, Hiroshi; Kohmura, Takayoshi; Ikeda, Shoma; Murakami, Hiroshi; Ozaki, Masanobu; Dotani, Tadayasu; Maeda, Yukie; Sagara, Kenshi</p> <p>2013-12-01</p> <p>We report on a proton radiation damage experiment on P-channel <span class="hlt">CCD</span> newly developed for an X-ray <span class="hlt">CCD</span> camera onboard the ASTRO-H satellite. The device was exposed up to 109 protons cm-2 at 6.7 MeV. The charge transfer inefficiency (CTI) was measured as a function of radiation dose. In comparison with the CTI currently measured in the <span class="hlt">CCD</span> camera onboard the Suzaku satellite for 6 years, we confirmed that the new type of P-channel <span class="hlt">CCD</span> is radiation tolerant enough for space use. We also confirmed that a charge-injection technique and lowering the operating temperature efficiently work to reduce the CTI for our device. A comparison with other P-channel <span class="hlt">CCD</span> experiments is also discussed. We performed a proton radiation damage experiment on a new P-channel <span class="hlt">CCD</span>. The device was exposed up to 109 protons cm-2 at 6.7 MeV. We confirmed that it is radiation tolerant enough for space use. We confirmed that a charge-injection technique reduces the CTI. We confirmed that lowering the operating temperature also reduces the CTI.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994mst..symp..669S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994mst..symp..669S"><span>Future <span class="hlt">ultra</span>-speed tube-flight</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Salter, Robert M.</p> <p>1994-05-01</p> <p>Future long-link, <span class="hlt">ultra</span>-speed, surface transport systems will require electromagnetically (EM) driven and restrained vehicles operating under reduced-atmosphere in very straight tubes. Such tube-flight trains will be safe, energy conservative, pollution-free, and in a protected environment. Hypersonic (and even hyperballistic) speeds are theoretically achievable. Ultimate system choices will represent tradeoffs between amoritized capital costs (ACC) and operating costs. For example, long coasting links might employ aerodynamic lift coupled with EM restraint and drag make-up. Optimized, combined EM lift, and thrust vectors could reduce energy costs but at increased ACC. (Repulsive levitation can produce lift-over-drag l/d ratios a decade greater than aerodynamic), Alternatively, vehicle-emanated, induced-mirror fields in a conducting (aluminum sheet) road bed could reduce ACC but at substantial energy costs. <span class="hlt">Ultra</span>-speed tube flight will demand fast-acting, <span class="hlt">high-precision</span> sensors and computerized magnetic shimming. This same control system can maintain a magnetic 'guide way' invariant in inertial space with inertial detectors imbedded in tube structures to sense and correct for earth tremors. <span class="hlt">Ultra</span>-speed tube flight can complete with aircraft for transit time and can provide even greater passenger convenience by single-model connections with local subways and feeder lines. Although cargo transport generally will not need to be performed at <span class="hlt">ultra</span> speeds, such speeds may well be desirable for <span class="hlt">high</span> throughput to optimize channel costs. Thus, a large and expensive pipeline might be replaced with small EM-driven pallets at <span class="hlt">high</span> speeds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940031411','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940031411"><span>Future <span class="hlt">ultra</span>-speed tube-flight</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Salter, Robert M.</p> <p>1994-01-01</p> <p>Future long-link, <span class="hlt">ultra</span>-speed, surface transport systems will require electromagnetically (EM) driven and restrained vehicles operating under reduced-atmosphere in very straight tubes. Such tube-flight trains will be safe, energy conservative, pollution-free, and in a protected environment. Hypersonic (and even hyperballistic) speeds are theoretically achievable. Ultimate system choices will represent tradeoffs between amoritized capital costs (ACC) and operating costs. For example, long coasting links might employ aerodynamic lift coupled with EM restraint and drag make-up. Optimized, combined EM lift, and thrust vectors could reduce energy costs but at increased ACC. (Repulsive levitation can produce lift-over-drag l/d ratios a decade greater than aerodynamic), Alternatively, vehicle-emanated, induced-mirror fields in a conducting (aluminum sheet) road bed could reduce ACC but at substantial energy costs. <span class="hlt">Ultra</span>-speed tube flight will demand fast-acting, <span class="hlt">high-precision</span> sensors and computerized magnetic shimming. This same control system can maintain a magnetic 'guide way' invariant in inertial space with inertial detectors imbedded in tube structures to sense and correct for earth tremors. <span class="hlt">Ultra</span>-speed tube flight can complete with aircraft for transit time and can provide even greater passenger convenience by single-model connections with local subways and feeder lines. Although cargo transport generally will not need to be performed at <span class="hlt">ultra</span> speeds, such speeds may well be desirable for <span class="hlt">high</span> throughput to optimize channel costs. Thus, a large and expensive pipeline might be replaced with small EM-driven pallets at <span class="hlt">high</span> speeds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012SPIE.8446E..5YC','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012SPIE.8446E..5YC"><span>Cryostat and <span class="hlt">CCD</span> for MEGARA at GTC</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Castillo-Domínguez, E.; Ferrusca, D.; Tulloch, S.; Velázquez, M.; Carrasco, E.; Gallego, J.; Gil de Paz, A.; Sánchez, F. M.; Vílchez Medina, J. M.</p> <p>2012-09-01</p> <p>MEGARA (Multi-Espectrógrafo en GTC de Alta Resolución para Astronomía) is the new integral field unit (IFU) and multi-object spectrograph (MOS) instrument for the GTC. The spectrograph subsystems include the pseudo-slit, the shutter, the collimator with a focusing mechanism, pupil elements on a volume phase holographic grating (VPH) wheel and the camera joined to the cryostat through the last lens, with a <span class="hlt">CCD</span> detector inside. In this paper we describe the full preliminary design of the cryostat which will harbor the <span class="hlt">CCD</span> detector for the spectrograph. The selected cryogenic device is an LN2 open-cycle cryostat which has been designed by the "Astronomical Instrumentation Lab for Millimeter Wavelengths" at INAOE. A complete description of the cryostat main body and <span class="hlt">CCD</span> head is presented as well as all the vacuum and temperature sub-systems to operate it. The <span class="hlt">CCD</span> is surrounded by a radiation shield to improve its performance and is placed in a custom made mechanical mounting which will allow physical adjustments for alignment with the spectrograph camera. The 4k x 4k pixel <span class="hlt">CCD</span>231 is our selection for the cryogenically cooled detector of MEGARA. The characteristics of this <span class="hlt">CCD</span>, the internal cryostat cabling and <span class="hlt">CCD</span> controller hardware are discussed. Finally, static structural finite element modeling and thermal analysis results are shown to validate the cryostat model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SPIE.7658E..5YS','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SPIE.7658E..5YS"><span>Timing generator of scientific grade <span class="hlt">CCD</span> camera and its implementation based on FPGA technology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Si, Guoliang; Li, Yunfei; Guo, Yongfei</p> <p>2010-10-01</p> <p>The Timing Generator's functions of Scientific Grade <span class="hlt">CCD</span> Camera is briefly presented: it generates various kinds of impulse sequence for the TDI-<span class="hlt">CCD</span>, video processor and imaging data output, acting as the synchronous coordinator for time in the <span class="hlt">CCD</span> imaging unit. The IL-E2TDI-<span class="hlt">CCD</span> sensor produced by DALSA Co.Ltd. use in the Scientific Grade <span class="hlt">CCD</span> Camera. Driving schedules of IL-E2 TDI-<span class="hlt">CCD</span> sensor has been examined in detail, the timing generator has been designed for Scientific Grade <span class="hlt">CCD</span> Camera. FPGA is chosen as the hardware design platform, schedule generator is described with VHDL. The designed generator has been successfully fulfilled function simulation with EDA software and fitted into XC2VP20-FF1152 (a kind of FPGA products made by XILINX). The experiments indicate that the new method improves the integrated level of the system. The Scientific Grade <span class="hlt">CCD</span> camera system's <span class="hlt">high</span> reliability, stability and low power supply are achieved. At the same time, the period of design and experiment is sharply shorted.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29771893','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29771893"><span>[Extreme (complicated, <span class="hlt">ultra-high</span>) refractive errors: terminological misconceptions!?</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Avetisov, S E</p> <p>2018-01-01</p> <p>The article reviews development mechanisms of different refractive errors accompanied by marked defocus of light rays reaching the retina. Terminology used for such ametropias includes terms extreme, <span class="hlt">ultra-high</span> and complicated. Justification of their usage for primary ametropias, whose symptom complex is based on changes in axial eye length, is an ongoing discussion. To comply with thesaurus definitions of 'diagnosis' and 'pathogenesis', to characterize refractive and anatomical-functional disorders in patients with primary ametropias it is proposed to use the terms 'hyperaxial and hypoaxial syndromes' with elaboration of specific symptoms instead of such expressions as extreme (<span class="hlt">ultra-high</span>) myopia and hypermetropia.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24921572','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24921572"><span><span class="hlt">Ultra</span>-long <span class="hlt">high</span>-sensitivity Φ-OTDR for <span class="hlt">high</span> spatial resolution intrusion detection of pipelines.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Peng, Fei; Wu, Han; Jia, Xin-Hong; Rao, Yun-Jiang; Wang, Zi-Nan; Peng, Zheng-Pu</p> <p>2014-06-02</p> <p>An <span class="hlt">ultra</span>-long phase-sensitive optical time domain reflectometry (Φ-OTDR) that can achieve <span class="hlt">high</span>-sensitivity intrusion detection over 131.5km fiber with <span class="hlt">high</span> spatial resolution of 8m is presented, which is the longest Φ-OTDR reported to date, to the best of our knowledge. It is found that the combination of distributed Raman amplification with heterodyne detection can extend the sensing distance and enhances the sensitivity substantially, leading to the realization of <span class="hlt">ultra</span>-long Φ-OTDR with <span class="hlt">high</span> sensitivity and spatial resolution. Furthermore, the feasibility of applying such an <span class="hlt">ultra</span>-long Φ-OTDR to pipeline security monitoring is demonstrated and the features of intrusion signal can be extracted with improved SNR by using the wavelet detrending/denoising method proposed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950005071','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950005071"><span>Analysis of trace halocarbon contaminants in <span class="hlt">ultra</span> <span class="hlt">high</span> purity helium</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fewell, Larry L.</p> <p>1994-01-01</p> <p>This study describes the analysis of <span class="hlt">ultra</span> <span class="hlt">high</span> purity helium. Purification studies were conducted and containment removal was effected by the utilization of solid adsorbent purge-trap systems at cryogenic temperatures. Volatile organic compounds in <span class="hlt">ultra</span> <span class="hlt">high</span> purity helium were adsorbed on a solid adsorbent-cryogenic trap, and thermally desorbed trace halocarbon and other contaminants were analyzed by combined gas chromatography-mass spectrometry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900000257&hterms=Silicide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DSilicide','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900000257&hterms=Silicide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DSilicide"><span>Silicide Schottky Barrier For Back-Surface-Illuminated <span class="hlt">CCD</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hecht, Michael H.</p> <p>1990-01-01</p> <p>Quantum efficiency of back-surface-illuminated charge-coupled device (<span class="hlt">CCD</span>) increased by coating back surface with thin layer of PtSi or IrSi on thin layer of SiO2. In its interaction with positively-doped bulk Si of <span class="hlt">CCD</span>, silicide/oxide layer forms Schottky barrier that repels electrons, promoting accumulation of photogenerated charge carriers in front-side <span class="hlt">CCD</span> potential wells. Physical principle responsible for improvement explained in "Metal Film Increases <span class="hlt">CCD</span> Output" (NPO-16815).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007SPIE.6279E..6YB','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007SPIE.6279E..6YB"><span>A novel imaging method for photonic crystal fiber fusion splicer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bi, Weihong; Fu, Guangwei; Guo, Xuan</p> <p>2007-01-01</p> <p>Because the structure of Photonic Crystal Fiber (PCF) is very complex, and it is very difficult that traditional fiber fusion splice obtains optical axial information of PCF. Therefore, we must search for a bran-new optical imaging method to get section information of Photonic Crystal Fiber. Based on complex trait of PCF, a novel <span class="hlt">high-precision</span> optics imaging system is presented in this article. The system uses a thinned electron-bombarded <span class="hlt">CCD</span> (EBCCD) which is a kind of image sensor as imaging element, the thinned electron-bombarded <span class="hlt">CCD</span> can offer low light level performance superior to conventional image intensifier coupled <span class="hlt">CCD</span> approaches, this <span class="hlt">high</span>-performance device can provide <span class="hlt">high</span> contrast <span class="hlt">high</span> resolution in low light level surveillance imaging; in order to realize <span class="hlt">precision</span> focusing of image, we use a <span class="hlt">ultra</span>-highprecision pace motor to adjust position of imaging lens. In this way, we can obtain legible section information of PCF. We may realize further concrete analysis for section information of PCF by digital image processing technology. Using this section information may distinguish different sorts of PCF, compute some parameters such as the size of PCF ventage, cladding structure of PCF and so on, and provide necessary analysis data for PCF fixation, adjustment, regulation, fusion and cutting system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994SPIE.2248...16C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994SPIE.2248...16C"><span><span class="hlt">High-precision</span> gauging of metal rings</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carlin, Mats; Lillekjendlie, Bjorn</p> <p>1994-11-01</p> <p>Raufoss AS designs and produces air brake fittings for trucks and buses on the international market. One of the critical components in the fittings is a small, circular metal ring, which is going through 100% dimension control. This article describes a low-price, <span class="hlt">high</span> accuracy solution developed at SINTEF Instrumentation based on image metrology and a subpixel resolution algorithm. The measurement system consists of a PC-plugg-in transputer video board, a <span class="hlt">CCD</span> camera, telecentric optics and a machine vision strobe. We describe the measurement technique in some detail, as well as the robust statistical techniques found to be essential in the real life environment.</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://hdl.handle.net/2060/20110016564','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110016564"><span>Event-Driven Random-Access-Windowing <span class="hlt">CCD</span> Imaging System</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Monacos, Steve; Portillo, Angel; Ortiz, Gerardo; Alexander, James; Lam, Raymond; Liu, William</p> <p>2004-01-01</p> <p>A charge-coupled-device (<span class="hlt">CCD</span>) based <span class="hlt">high</span>-speed imaging system, called a realtime, event-driven (RARE) camera, is undergoing development. This camera is capable of readout from multiple subwindows [also known as regions of interest (ROIs)] within the <span class="hlt">CCD</span> field of view. Both the sizes and the locations of the ROIs can be controlled in real time and can be changed at the camera frame rate. The predecessor of this camera was described in <span class="hlt">High</span>-Frame-Rate <span class="hlt">CCD</span> Camera Having Subwindow Capability (NPO- 30564) NASA Tech Briefs, Vol. 26, No. 12 (December 2002), page 26. The architecture of the prior camera requires tight coupling between camera control logic and an external host computer that provides commands for camera operation and processes pixels from the camera. This tight coupling limits the attainable frame rate and functionality of the camera. The design of the present camera loosens this coupling to increase the achievable frame rate and functionality. From a host computer perspective, the readout operation in the prior camera was defined on a per-line basis; in this camera, it is defined on a per-ROI basis. In addition, the camera includes internal timing circuitry. This combination of features enables real-time, event-driven operation for adaptive control of the camera. Hence, this camera is well suited for applications requiring autonomous control of multiple ROIs to track multiple targets moving throughout the <span class="hlt">CCD</span> field of view. Additionally, by eliminating the need for control intervention by the host computer during the pixel readout, the present design reduces ROI-readout times to attain higher frame rates. This camera (see figure) includes an imager card consisting of a commercial <span class="hlt">CCD</span> imager and two signal-processor chips. The imager card converts transistor/ transistor-logic (TTL)-level signals from a field programmable gate array (FPGA) controller card. These signals are transmitted to the imager card via a low-voltage differential signaling (LVDS) cable</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007JASS...24..367O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007JASS...24..367O"><span>A Design and Development of Multi-Purpose <span class="hlt">CCD</span> Camera System with Thermoelectric Cooling: Software</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Oh, S. H.; Kang, Y. W.; Byun, Y. I.</p> <p>2007-12-01</p> <p>We present a software which we developed for the multi-purpose <span class="hlt">CCD</span> camera. This software can be used on the all 3 types of <span class="hlt">CCD</span> - KAF-0401E (768×512), KAF-1602E (15367times;1024), KAF-3200E (2184×1472) made in KODAK Co.. For the efficient <span class="hlt">CCD</span> camera control, the software is operated with two independent processes of the <span class="hlt">CCD</span> control program and the temperature/shutter operation program. This software is designed to fully automatic operation as well as manually operation under LINUX system, and is controled by LINUX user signal procedure. We plan to use this software for all sky survey system and also night sky monitoring and sky observation. As our results, the read-out time of each <span class="hlt">CCD</span> are about 15sec, 64sec, 134sec for KAF-0401E, KAF-1602E, KAF-3200E., because these time are limited by the data transmission speed of parallel port. For larger format <span class="hlt">CCD</span>, the data transmission is required more <span class="hlt">high</span> speed. we are considering this control software to one using USB port for <span class="hlt">high</span> speed data transmission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA103970','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA103970"><span><span class="hlt">Ultra-High</span> Surface Speed for Metal Removal, Artillery Shell</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1981-07-01</p> <p>TECHNICAL LIBRARY "y/a^^cr^ AD-E400 660 CONTRACTOR REPORT ARLCD-CR- 81019 <span class="hlt">ULTRA-HIGH</span> SURFACE SPEED FOR METAL REMOVAL, ARTILLERY SHELL RICHARD F...Report ARLCD-CR- 81019 2. GOVT ACCESSION NO. 3. RECIPIENT’S CATALOG NUMBER 4. TITLE (and Subtitle) <span class="hlt">ULTRA-HIGH</span> SURFACE SPEED FOR METAL...UNIT* tuiPPtO 1 MIL -STD-43CA i, ASTM A-274-64 EF A1SI~1340 SEHI FIN FORGING STEEL 6 RC SQ ■ IP 120093* a LIFTS 38 PCS</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SPIE10486E..0NG','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SPIE10486E..0NG"><span><span class="hlt">Ultra</span>-low noise supercontinuum source for <span class="hlt">ultra-high</span> resolution optical coherence tomography at 1300 nm</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gonzalo, I. B.; Maria, M.; Engelsholm, R. D.; Feuchter, T.; Leick, L.; Moselund, P. M.; Podoleanu, A.; Bang, O.</p> <p>2018-02-01</p> <p>Supercontinuum (SC) sources are of great interest for many applications due to their <span class="hlt">ultra</span>-broad optical bandwidth, good beam quality and <span class="hlt">high</span> power spectral density [1]. In particular, the <span class="hlt">high</span> average power over large bandwidths makes SC light sources excellent candidates for <span class="hlt">ultra-high</span> resolution optical coherence tomography (UHR-OCT) [2-5]. However, conventional SC sources suffer from <span class="hlt">high</span> pulse-to-pulse intensity fluctuations as a result of the noise-sensitive nonlinear effects involved in the SC generation process [6-9]. This intensity noise from the SC source can limit the performance of OCT, resulting in a reduced signal-to-noise ratio (SNR) [10-12]. Much work has been done to reduce the noise of the SC sources for instance with fiber tapers [7,8] or increasing the repetition rate of the pump laser for averaging in the spectrometer [10,12]. An alternative approach is to use all-normal dispersion (ANDi) fibers [13,14] to generate SC light from well-known coherent nonlinear processes [15-17]. In fact, reduction of SC noise using ANDi fibers compared to anomalous dispersion SC pumped by sub-picosecond pulses has been recently demonstrated [18], but a cladding mode was used to stabilize the ANDi SC. In this work, we characterize the noise performance of a femtosecond pumped ANDi based SC and a commercial SC source in an UHR-OCT system at 1300 nm. We show that the ANDi based SC presents exceptional noise properties compared to a commercial source. An improvement of 5 dB in SNR is measured in the UHR-OCT system, and the noise behavior resembles that of a superluminiscent diode. This preliminary study is a step forward towards development of an <span class="hlt">ultra</span>-low noise SC source at 1300 nm for <span class="hlt">ultra-high</span> resolution OCT.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AnShO..26..110Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AnShO..26..110Y"><span>A FORTRAN realization of the block adjustment of <span class="hlt">CCD</span> frames</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yu, Yong; Tang, Zhenghong; Li, Jinling; Zhao, Ming</p> <p></p> <p>A FORTRAN version realization of the block adjustment (BA) of overlapping <span class="hlt">CCD</span> frames is developed. The flowchart is introduced including (a) data collection, (b) preprocessing, and (c) BA and object positioning. The subroutines and their functions are also demonstrated. The program package is tested by simulated data with/without the application of white noises. It is also preliminarily applied to the reduction of optical positions of four extragalactic radio sources. The results show that because of the increase in the sky coverage and number of reference stars, the <span class="hlt">precision</span> of deducted positions is improved compared with single plate adjustment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1992StaUN.148.....L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1992StaUN.148.....L"><span>SCP -- A Simple <span class="hlt">CCD</span> Processing Package</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lewis, J. R.</p> <p></p> <p>This note describes a small set of programs, written at RGO, which deal with basic <span class="hlt">CCD</span> frame processing (e.g. bias subtraction, flat fielding, trimming etc.). The need to process large numbers of <span class="hlt">CCD</span> frames from devices such as FOS or ISIS in order to extract spectra has prompted the writing of routines which will do the basic hack-work with a minimal amount of interaction from the user. Although they were written with spectral data in mind, there are no ``spectrum-specific'' features in the software which means they can be applied to any <span class="hlt">CCD</span> data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24610829','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24610829"><span>Rapid determination of quinolones in cosmetic products by <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography with tandem mass spectrometry.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Shao-Ying; Huang, Xi-Hui; Wang, Xiao-Fang; Jin, Quan; Zhu, Guo-Nian</p> <p>2014-05-01</p> <p>This study developed an improved analytical method for the simultaneous quantification of 13 quinolones in cosmetics by <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography combined with ESI triple quadrupole MS/MS under the multiple reaction monitoring mode. The analytes were extracted and purified by using an SPE cartridge. The limits of quantification ranged from 0.03 to 3.02 μg/kg. The <span class="hlt">precision</span> for determining the quinolones was <19.39%. The proposed method was successfully developed for the determination of quinolones in real cosmetic samples. © 2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NatCo...713383L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NatCo...713383L"><span>Mid-infrared <span class="hlt">ultra-high</span>-Q resonators based on fluoride crystalline materials</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lecaplain, C.; Javerzac-Galy, C.; Gorodetsky, M. L.; Kippenberg, T. J.</p> <p>2016-11-01</p> <p>The unavailability of <span class="hlt">highly</span> transparent materials in the mid-infrared has been the main limitation in the development of <span class="hlt">ultra</span>-sensitive molecular sensors or cavity-based spectroscopy applications. Whispering gallery mode microresonators have attained <span class="hlt">ultra-high</span>-quality (Q) factor resonances in the near-infrared and visible. Here we report <span class="hlt">ultra-high</span> Q factors in the mid-infrared using polished alkaline earth metal fluoride crystals. Using an uncoated chalcogenide tapered fibre as a <span class="hlt">high</span>-ideality coupler in the mid-infrared, we study via cavity ringdown technique the losses of BaF2, CaF2, MgF2 and SrF2 microresonators. We show that MgF2 is limited by multiphonon absorption by studying the temperature dependence of the Q factor. In contrast, in SrF2 and BaF2 the lower multiphonon absorption leads to <span class="hlt">ultra-high</span> Q factors at 4.5 μm. These values correspond to an optical finesse of , the highest value achieved for any type of mid-infrared resonator to date.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5121327','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5121327"><span>Mid-infrared <span class="hlt">ultra-high</span>-Q resonators based on fluoride crystalline 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>Lecaplain, C.; Javerzac-Galy, C.; Gorodetsky, M. L.; Kippenberg, T. J.</p> <p>2016-01-01</p> <p>The unavailability of <span class="hlt">highly</span> transparent materials in the mid-infrared has been the main limitation in the development of <span class="hlt">ultra</span>-sensitive molecular sensors or cavity-based spectroscopy applications. Whispering gallery mode microresonators have attained <span class="hlt">ultra-high</span>-quality (Q) factor resonances in the near-infrared and visible. Here we report <span class="hlt">ultra-high</span> Q factors in the mid-infrared using polished alkaline earth metal fluoride crystals. Using an uncoated chalcogenide tapered fibre as a <span class="hlt">high</span>-ideality coupler in the mid-infrared, we study via cavity ringdown technique the losses of BaF2, CaF2, MgF2 and SrF2 microresonators. We show that MgF2 is limited by multiphonon absorption by studying the temperature dependence of the Q factor. In contrast, in SrF2 and BaF2 the lower multiphonon absorption leads to <span class="hlt">ultra-high</span> Q factors at 4.5 μm. These values correspond to an optical finesse of , the highest value achieved for any type of mid-infrared resonator to date. PMID:27869119</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27869119','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27869119"><span>Mid-infrared <span class="hlt">ultra-high</span>-Q resonators based on fluoride crystalline materials.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lecaplain, C; Javerzac-Galy, C; Gorodetsky, M L; Kippenberg, T J</p> <p>2016-11-21</p> <p>The unavailability of <span class="hlt">highly</span> transparent materials in the mid-infrared has been the main limitation in the development of <span class="hlt">ultra</span>-sensitive molecular sensors or cavity-based spectroscopy applications. Whispering gallery mode microresonators have attained <span class="hlt">ultra-high</span>-quality (Q) factor resonances in the near-infrared and visible. Here we report <span class="hlt">ultra-high</span> Q factors in the mid-infrared using polished alkaline earth metal fluoride crystals. Using an uncoated chalcogenide tapered fibre as a <span class="hlt">high</span>-ideality coupler in the mid-infrared, we study via cavity ringdown technique the losses of BaF 2 , CaF 2 , MgF 2 and SrF 2 microresonators. We show that MgF 2 is limited by multiphonon absorption by studying the temperature dependence of the Q factor. In contrast, in SrF 2 and BaF 2 the lower multiphonon absorption leads to <span class="hlt">ultra-high</span> Q factors at 4.5 μm. These values correspond to an optical finesse of , the highest value achieved for any type of mid-infrared resonator to date.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.V43B3144P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.V43B3144P"><span><span class="hlt">High-Precision</span> Isotope Ratio Measurements of Sub-Picogram Actinide Samples</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pollington, A. D.; Kinman, W.</p> <p>2016-12-01</p> <p>One of the most exciting trends in analytical geochemistry over the past decade is the push towards smaller and smaller sample sizes while simultaneously achieving <span class="hlt">high</span> <span class="hlt">precision</span> isotope ratio measurements. This trend has been driven by advances in clean chemistry protocols, and by significant breakthroughs in mass spectrometer ionization efficiency and detector quality (stability and noise for low signals). In this presentation I will focus on new techniques currently being developed at Los Alamos National Laboratory for the characterization of <span class="hlt">ultra</span>-small samples (pg, fg, ag), with particular focus on actinide measurements by MC-ICP-MS. Analyses of U, Pu, Th and Am are routinely carried out in our facility using multi-ion counting techniques. I will describe some of the challenges associated with using exclusively ion counting methods (e.g., stability, detector cross calibration, etc.), and how we work to mitigate them. While the focus of much of the work currently being carried out is in the broad field of nuclear forensics and safeguards, the techniques that are being developed are directly applicable to many geologic questions that require analyses of small samples of U and Th, for example. In addition to the description of the technique development, I will present case studies demonstrating the <span class="hlt">precision</span> and accuracy of the method as applied to real-world samples.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080004667','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080004667"><span><span class="hlt">Ultra</span> <span class="hlt">precision</span> and reliable bonding method</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gwo, Dz-Hung (Inventor)</p> <p>2001-01-01</p> <p>The bonding of two materials through hydroxide-catalyzed hydration/dehydration is achieved at room temperature by applying hydroxide ions to at least one of the two bonding surfaces and by placing the surfaces sufficiently close to each other to form a chemical bond between them. The surfaces may be placed sufficiently close to each other by simply placing one surface on top of the other. A silicate material may also be used as a filling material to help fill gaps between the surfaces caused by surface figure mismatches. A powder of a silica-based or silica-containing material may also be used as an additional filling material. The hydroxide-catalyzed bonding method forms bonds which are not only as <span class="hlt">precise</span> and transparent as optical contact bonds, but also as strong and reliable as <span class="hlt">high</span>-temperature frit bonds. The hydroxide-catalyzed bonding method is also simple and inexpensive.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGeod.tmp..473L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGeod.tmp..473L"><span><span class="hlt">High-precision</span> GNSS ocean positioning with BeiDou short-message communication</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Bofeng; Zhang, Zhiteng; Zang, Nan; Wang, Siyao</p> <p>2018-04-01</p> <p>The current popular GNSS RTK technique would be not applicable on ocean due to the limited communication access for transmitting differential corrections. A new technique is proposed for <span class="hlt">high-precision</span> ocean RTK, referred to as ORTK, where the corrections are transmitted by employing the function of BeiDou satellite short-message communication (SMC). To overcome the limitation of narrow bandwidth of BeiDou SMC, a new strategy of simplifying and encoding corrections is proposed instead of standard differential corrections, which reduces the single-epoch corrections from more than 1000 to less than 300 bytes. To solve the problems of correction delays, cycle slips, blunders and abnormal epochs over <span class="hlt">ultra</span>-long baseline ORTK, a series of powerful algorithms were designed at the user-end software for achieving the stable and <span class="hlt">precise</span> kinematic solutions on far ocean applications. The results from two long baselines of 240 and 420 km and real ocean experiments reveal that the kinematic solutions with horizontal accuracy of 5 cm and vertical accuracy of better than 15 cm are achievable by convergence time of 3-10 min. Compared to commercial ocean PPP with satellite telecommunication, ORTK is of much cheaper expense, higher accuracy and shorter convergence. It will be very prospective in many location-based ocean services.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/6614390','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/6614390"><span>Follow-up study of children with cerebral coordination disturbance (<span class="hlt">CCD</span>, Vojta).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Imamura, S; Sakuma, K; Takahashi, T</p> <p>1983-01-01</p> <p>713 children (from newborn to 12-month-old) with delayed motor development were carefully examined and classified into normal, very light cerebral coordination disturbance (<span class="hlt">CCD</span>, Vojta), light <span class="hlt">CCD</span>, moderate <span class="hlt">CCD</span>, severe <span class="hlt">CCD</span>, suspected cerebral palsy (CP) and other diseases at their first visit, and were followed up carefully. Finally, 89.0% of very light <span class="hlt">CCD</span>, 71.4% of light <span class="hlt">CCD</span>, 56.0% of moderate <span class="hlt">CCD</span> and 30.0% of severe <span class="hlt">CCD</span> developed into normal. 59.5% of moderate <span class="hlt">CCD</span> and 45.5% of severe <span class="hlt">CCD</span> among children who were given Vojta's physiotherapy developed into normal. The classification of cases with delayed motor development into very light, light, moderate and severe <span class="hlt">CCD</span> based on the extent of abnormality in their postural reflexes is useful and well correlated with their prognosis. Treatment by Vojta's method seems to be efficient and helpful for young children with delayed motor development.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994SPIE.2172..100L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994SPIE.2172..100L"><span>Multiport backside-illuminated <span class="hlt">CCD</span> imagers for <span class="hlt">high</span>-frame-rate camera applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Levine, Peter A.; Sauer, Donald J.; Hseuh, Fu-Lung; Shallcross, Frank V.; Taylor, Gordon C.; Meray, Grazyna M.; Tower, John R.; Harrison, Lorna J.; Lawler, William B.</p> <p>1994-05-01</p> <p>Two multiport, second-generation <span class="hlt">CCD</span> imager designs have been fabricated and successfully tested. They are a 16-port 512 X 512 array and a 32-port 1024 X 1024 array. Both designs are back illuminated, have on-chip CDS, lateral blooming control, and use a split vertical frame transfer architecture with full frame storage. The 512 X 512 device has been operated at rates over 800 frames per second. The 1024 X 1024 device has been operated at rates over 300 frames per second. The major changes incorporated in the second-generation design are, reduction in gate length in the output area to give improved <span class="hlt">high</span>-clock-rate performance, modified on-chip CDS circuitry for reduced noise, and optimized implants to improve performance of blooming control at lower clock amplitude. This paper discusses the imager design improvements and presents measured performance results at <span class="hlt">high</span> and moderate frame rates. The design and performance of three moderate frame rate cameras are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29632301','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29632301"><span>Designable <span class="hlt">ultra</span>-smooth <span class="hlt">ultra</span>-thin solid-electrolyte interphases of three alkali metal anodes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gu, Yu; Wang, Wei-Wei; Li, Yi-Juan; Wu, Qi-Hui; Tang, Shuai; Yan, Jia-Wei; Zheng, Ming-Sen; Wu, De-Yin; Fan, Chun-Hai; Hu, Wei-Qiang; Chen, Zhao-Bin; Fang, Yuan; Zhang, Qing-Hong; Dong, Quan-Feng; Mao, Bing-Wei</p> <p>2018-04-09</p> <p>Dendrite growth of alkali metal anodes limited their lifetime for charge/discharge cycling. Here, we report near-perfect anodes of lithium, sodium, and potassium metals achieved by electrochemical polishing, which removes microscopic defects and creates <span class="hlt">ultra</span>-smooth <span class="hlt">ultra</span>-thin solid-electrolyte interphase layers at metal surfaces for providing a homogeneous environment. <span class="hlt">Precise</span> characterizations by AFM force probing with corroborative in-depth XPS profile analysis reveal that the <span class="hlt">ultra</span>-smooth <span class="hlt">ultra</span>-thin solid-electrolyte interphase can be designed to have alternating inorganic-rich and organic-rich/mixed multi-layered structure, which offers mechanical property of coupled rigidity and elasticity. The polished metal anodes exhibit significantly enhanced cycling stability, specifically the lithium anodes can cycle for over 200 times at a real current density of 2 mA cm -2 with 100% depth of discharge. Our work illustrates that an <span class="hlt">ultra</span>-smooth <span class="hlt">ultra</span>-thin solid-electrolyte interphase may be robust enough to suppress dendrite growth and thus serve as an initial layer for further improved protection of alkali metal anodes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013SPIE.8796E..0DS','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013SPIE.8796E..0DS"><span>Experimental research on femto-second laser damaging array <span class="hlt">CCD</span> cameras</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shao, Junfeng; Guo, Jin; Wang, Ting-feng; Wang, Ming</p> <p>2013-05-01</p> <p>Charged Coupled Devices (<span class="hlt">CCD</span>) are widely used in military and security applications, such as airborne and ship based surveillance, satellite reconnaissance and so on. Homeland security requires effective means to negate these advanced overseeing systems. Researches show that <span class="hlt">CCD</span> based EO systems can be significantly dazzled or even damaged by <span class="hlt">high</span>-repetition rate pulsed lasers. Here, we report femto - second laser interaction with <span class="hlt">CCD</span> camera, which is probable of great importance in future. Femto - second laser is quite fresh new lasers, which has unique characteristics, such as extremely short pulse width (1 fs = 10-15 s), extremely <span class="hlt">high</span> peak power (1 TW = 1012W), and especially its unique features when interacting with matters. Researches in femto second laser interaction with materials (metals, dielectrics) clearly indicate non-thermal effect dominates the process, which is of vast difference from that of long pulses interaction with matters. Firstly, the damage threshold test are performed with femto second laser acting on the <span class="hlt">CCD</span> camera. An 800nm, 500μJ, 100fs laser pulse is used to irradiate interline <span class="hlt">CCD</span> solid-state image sensor in the experiment. In order to focus laser energy onto tiny <span class="hlt">CCD</span> active cells, an optical system of F/5.6 is used. A Sony production CCDs are chose as typical targets. The damage threshold is evaluated with multiple test data. Point damage, line damage and full array damage were observed when the irradiated pulse energy continuously increase during the experiment. The point damage threshold is found 151.2 mJ/cm2.The line damage threshold is found 508.2 mJ/cm2.The full-array damage threshold is found to be 5.91 J/cm2. Although the phenomenon is almost the same as that of nano laser interaction with <span class="hlt">CCD</span>, these damage thresholds are substantially lower than that of data obtained from nano second laser interaction with <span class="hlt">CCD</span>. Then at the same time, the electric features after different degrees of damage are tested with electronic multi</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15948447','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15948447"><span>Mobile-bearing knee systems: <span class="hlt">ultra-high</span> molecular weight polyethylene wear and design issues.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Greenwald, A Seth; Heim, Christine S</p> <p>2005-01-01</p> <p>In June 2004, the U.S. Food and Drug Administration Orthopaedic Advisory Panel recommended the reclassification of mobile-bearing knee systems for general use. This reflects the increasing use of mobile-bearing knee systems internationally, which is currently limited in the United States by regulatory requirement. Mobile-bearing knee systems are distinguished from conventional, fixed-plateau systems in that they allow dual-surface articulation between an <span class="hlt">ultra-high</span> molecular weight polyethylene insert and metallic femoral and tibial tray components. Their in vivo success is dependent on patient selection, design, and material choice, as well as surgical <span class="hlt">precision</span> during implantation. Laboratory and clinical experience extending over 25 years with individual systems suggests that mobile-bearing knee systems represent a viable treatment option for patients with knee arthrosis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/872992','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/872992"><span><span class="hlt">Ultra</span>-compact Marx-type <span class="hlt">high</span>-voltage generator</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Goerz, David A.; Wilson, Michael J.</p> <p>2000-01-01</p> <p>An <span class="hlt">ultra</span>-compact Marx-type <span class="hlt">high</span>-voltage generator includes individual <span class="hlt">high</span>-performance components that are closely coupled and integrated into an extremely compact assembly. In one embodiment, a repetitively-switched, <span class="hlt">ultra</span>-compact Marx generator includes low-profile, annular-shaped, <span class="hlt">high</span>-voltage, ceramic capacitors with contoured edges and coplanar extended electrodes used for primary energy storage; low-profile, low-inductance, <span class="hlt">high</span>-voltage, pressurized gas switches with compact gas envelopes suitably designed to be integrated with the annular capacitors; feed-forward, <span class="hlt">high</span>-voltage, ceramic capacitors attached across successive switch-capacitor-switch stages to couple the necessary energy forward to sufficiently overvoltage the spark gap of the next in-line switch; optimally shaped electrodes and insulator surfaces to reduce electric field stresses in the weakest regions where dissimilar materials meet, and to spread the fields more evenly throughout the dielectric materials, allowing them to operate closer to their intrinsic breakdown levels; and uses manufacturing and assembly methods to integrate the capacitors and switches into stages that can be arranged into a low-profile Marx generator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5513415','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5513415"><span>Colony Collapse Disorder (<span class="hlt">CCD</span>) and bee age impact honey bee pathophysiology</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Traynor, Kirsten S.; Andree, Michael; Lichtenberg, Elinor M.; Chen, Yanping; Saegerman, Claude; Cox-Foster, Diana L.</p> <p>2017-01-01</p> <p>Honey bee (Apis mellifera) colonies continue to experience <span class="hlt">high</span> annual losses that remain poorly explained. Numerous interacting factors have been linked to colony declines. Understanding the pathways linking pathophysiology with symptoms is an important step in understanding the mechanisms of disease. In this study we examined the specific pathologies associated with honey bees collected from colonies suffering from Colony Collapse Disorder (<span class="hlt">CCD</span>) and compared these with bees collected from apparently healthy colonies. We identified a set of pathological physical characteristics that occurred at different rates in <span class="hlt">CCD</span> diagnosed colonies prior to their collapse: rectum distension, Malpighian tubule iridescence, fecal matter consistency, rectal enteroliths (hard concretions), and venom sac color. The multiple differences in rectum symptomology in bees from <span class="hlt">CCD</span> apiaries and colonies suggest effected bees had trouble regulating water. To ensure that pathologies we found associated with <span class="hlt">CCD</span> were indeed pathologies and not due to normal changes in physical appearances that occur as an adult bee ages (<span class="hlt">CCD</span> colonies are assumed to be composed mostly of young bees), we documented the changes in bees of different ages taken from healthy colonies. We found that young bees had much greater incidences of white nodules than older cohorts. Prevalent in newly-emerged bees, these white nodules or cellular encapsulations indicate an active immune response. Comparing the two sets of characteristics, we determined a subset of pathologies that reliably predict <span class="hlt">CCD</span> status rather than bee age (fecal matter consistency, rectal distension size, rectal enteroliths and Malpighian tubule iridescence) and that may serve as biomarkers for colony health. In addition, these pathologies suggest that <span class="hlt">CCD</span> bees are experiencing disrupted excretory physiology. Our identification of these symptoms is an important first step in understanding the physiological pathways that underlie <span class="hlt">CCD</span> and 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_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/28715431','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28715431"><span>Colony Collapse Disorder (<span class="hlt">CCD</span>) and bee age impact honey bee pathophysiology.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>vanEngelsdorp, Dennis; Traynor, Kirsten S; Andree, Michael; Lichtenberg, Elinor M; Chen, Yanping; Saegerman, Claude; Cox-Foster, Diana L</p> <p>2017-01-01</p> <p>Honey bee (Apis mellifera) colonies continue to experience <span class="hlt">high</span> annual losses that remain poorly explained. Numerous interacting factors have been linked to colony declines. Understanding the pathways linking pathophysiology with symptoms is an important step in understanding the mechanisms of disease. In this study we examined the specific pathologies associated with honey bees collected from colonies suffering from Colony Collapse Disorder (<span class="hlt">CCD</span>) and compared these with bees collected from apparently healthy colonies. We identified a set of pathological physical characteristics that occurred at different rates in <span class="hlt">CCD</span> diagnosed colonies prior to their collapse: rectum distension, Malpighian tubule iridescence, fecal matter consistency, rectal enteroliths (hard concretions), and venom sac color. The multiple differences in rectum symptomology in bees from <span class="hlt">CCD</span> apiaries and colonies suggest effected bees had trouble regulating water. To ensure that pathologies we found associated with <span class="hlt">CCD</span> were indeed pathologies and not due to normal changes in physical appearances that occur as an adult bee ages (<span class="hlt">CCD</span> colonies are assumed to be composed mostly of young bees), we documented the changes in bees of different ages taken from healthy colonies. We found that young bees had much greater incidences of white nodules than older cohorts. Prevalent in newly-emerged bees, these white nodules or cellular encapsulations indicate an active immune response. Comparing the two sets of characteristics, we determined a subset of pathologies that reliably predict <span class="hlt">CCD</span> status rather than bee age (fecal matter consistency, rectal distension size, rectal enteroliths and Malpighian tubule iridescence) and that may serve as biomarkers for colony health. In addition, these pathologies suggest that <span class="hlt">CCD</span> bees are experiencing disrupted excretory physiology. Our identification of these symptoms is an important first step in understanding the physiological pathways that underlie <span class="hlt">CCD</span> and factors</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.V43B3161D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.V43B3161D"><span><span class="hlt">High</span> <span class="hlt">precision</span> measurements of 16O12C17O using a new type of cavity ring down spectrometer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Daëron, M.; Stoltmann, T.; Kassi, S.; Burkhart, J.; Kerstel, E.</p> <p>2016-12-01</p> <p>Laser absorption techniques for the measurement of isotopologue abundances in gases have been dripping into the geoscientific community over the past decade. In the field of carbon dioxide such instruments have mostly been restricted to measurements of the most abundant stable isotopologues. Distinct advantages of CRDS techniques are non-destructiveness and the ability to resolve isobaric isotopologues. The determination of low-abundance isotopologues is predominantly limited by the linewidth of the probing laser, laser jitter, laser drift and system stability. Here we present first measurements of 16O12C17O abundances using a new type of <span class="hlt">ultra-precise</span> cavity ring down spectrometer. By the use of Optical Feedback Frequency Stabilization, we achieved a laser line width in the sub-kHz regime with a frequency drift of less than 20 Hz/s. A tight coupling with an <span class="hlt">ultra</span>-stable ring down cavity combined with a frequency tuning mechanism which enables us to arbitrarily position spectral points (Burkart et al., 2013) allowed us to demonstrate a single-scan (2 minutes) <span class="hlt">precision</span> of 40 ppm on the determination of the 16O12C17O abundance. These promising results imply that routine, direct, <span class="hlt">high-precision</span> measurements of 17O-anomalies in CO2 using this non-destructive method are in reach. References:Burkart J, Romanini D, Kassi S; Optical feedback stabilized laser tuned by single-sideband modulation; Optical Letters 12:2062-2063 (2013)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900056229&hterms=MgF2&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DMgF2','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900056229&hterms=MgF2&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DMgF2"><span>Low temperature multi-alkali photocathode processing technique for sealed intensified <span class="hlt">CCD</span> tubes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Doliber, D. L.; Dozier, E. E.; Wenzel, H.; Beaver, E. A.; Hier, R. G.</p> <p>1989-01-01</p> <p>A low temperature photocathode process has been used to fabricate an intensified <span class="hlt">CCD</span> visual photocathode image tube, by incorporating a thinned, backside-illumined <span class="hlt">CCD</span> as the target anode of a digicon tube of Hubble Space Telescope (HST) design. The <span class="hlt">CCD</span> digicon tube employs the HST's sodium bialkali photocathode and MgF2 substrate, thereby allowing a direct photocathode quantum efficiency comparison between photocathodes produced by the presently employed low temperature process and those of the conventional <span class="hlt">high</span> temperature process. Attention is given to the processing chamber used, as well as the details of gas desorption and photocathode processing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4151678','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4151678"><span>On the characterization of <span class="hlt">ultra-precise</span> X-ray optical components: advances and challenges in ex situ metrology</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Siewert, F.; Buchheim, J.; Zeschke, T.; Störmer, M.; Falkenberg, G.; Sankari, R.</p> <p>2014-01-01</p> <p>To fully exploit the ultimate source properties of the next-generation light sources, such as free-electron lasers (FELs) and diffraction-limited storage rings (DLSRs), the quality requirements for gratings and reflective synchrotron optics, especially mirrors, have significantly increased. These coherence-preserving optical components for <span class="hlt">high</span>-brightness sources will feature nanoscopic shape accuracies over macroscopic length scales up to 1000 mm. To enable <span class="hlt">high</span> efficiency in terms of photon flux, such optics will be coated with application-tailored single or multilayer coatings. Advanced thin-film fabrication of today enables the synthesis of layers on the sub-nanometre <span class="hlt">precision</span> level over a deposition length of up to 1500 mm. Specifically dedicated metrology instrumentation of comparable accuracy has been developed to characterize such optical elements. Second-generation slope-measuring profilers like the nanometre optical component measuring machine (NOM) at the BESSY-II Optics laboratory allow the inspection of up to 1500 mm-long reflective optical components with an accuracy better than 50 nrad r.m.s. Besides measuring the shape on top of the coated mirror, it is of particular interest to characterize the internal material properties of the mirror coating, which is the domain of X-rays. Layer thickness, density and interface roughness of single and multilayer coatings are investigated by means of X-ray reflectometry. In this publication recent achievements in the field of slope measuring metrology are shown and the characterization of different types of mirror coating demonstrated. Furthermore, upcoming challenges to the inspection of <span class="hlt">ultra-precise</span> optical components designed to be used in future FEL and DLSR beamlines are discussed. PMID:25177985</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006PASP..118.1448Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006PASP..118.1448Y"><span><span class="hlt">CCD</span> Centroiding Experiment for Correcting a Distorted Image on the Focal Plane</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yano, Taihei; Araki, Hiroshi; Gouda, Naoteru; Kobayashi, Yukiyasu; Tsujimoto, Takuji; Nakajima, Tadashi; Kawano, Nobuyuki; Tazawa, Seiichi; Yamada, Yoshiyuki; Hanada, Hideo; Asari, Kazuyoshi; Tsuruta, Seiitsu</p> <p>2006-10-01</p> <p>JASMINE (Japan Astrometry Satellite Mission for Infrared Exploration) and ILOM (In situ Lunar Orientation Measurement) are space missions that are in progress at the National Astronomical Observatory of Japan. These two projects require a common astrometric technique to obtain <span class="hlt">precise</span> positions of star images on solid-state detectors in order to accomplish their objectives. In the laboratory, we have carried out measurements of the centroid of artificial star images on a <span class="hlt">CCD</span> array in order to investigate the <span class="hlt">precision</span> of the positions of the stars, using an algorithm for estimating them from photon-weighted means of the stars. In the calibration of the position of a star image at the focal plane, we have also taken into account the lowest order distortion due to optical aberrations, which is proportional to the cube of the distance from the optical axis. Accordingly, we find that the <span class="hlt">precision</span> of the measurement for the positions of the stars reaches below 1/100 pixel for one measurement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002ITNS...49..559P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002ITNS...49..559P"><span>Modeling the impact of preflushing on CTE in proton irradiated <span class="hlt">CCD</span>-based detectors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Philbrick, R. H.</p> <p>2002-04-01</p> <p>A software model is described that performs a "real world" simulation of the operation of several types of charge-coupled device (<span class="hlt">CCD</span>)-based detectors in order to accurately predict the impact that <span class="hlt">high</span>-energy proton radiation has on image distortion and modulation transfer function (MTF). The model was written primarily to predict the effectiveness of vertical preflushing on the custom full frame <span class="hlt">CCD</span>-based detectors intended for use on the proposed Kepler Discovery mission, but it is capable of simulating many other types of <span class="hlt">CCD</span> detectors and operating modes as well. The model keeps track of the occupancy of all phosphorous-silicon (P-V), divacancy (V-V) and oxygen-silicon (O-V) defect centers under every <span class="hlt">CCD</span> electrode over the entire detector area. The integrated image is read out by simulating every electrode-to-electrode charge transfer in both the vertical and horizontal <span class="hlt">CCD</span> registers. A signal level dependency on the capture and emission of signal is included and the current state of each electrode (e.g., barrier or storage) is considered when distributing integrated and emitted signal. Options for performing preflushing, preflashing, and including mini-channels are available on both the vertical and horizontal <span class="hlt">CCD</span> registers. In addition, dark signal generation and image transfer smear can be selectively enabled or disabled. A comparison of the charge transfer efficiency (CTE) data measured on the Hubble space telescope imaging spectrometer (STIS) <span class="hlt">CCD</span> with the CTE extracted from model simulations of the STIS <span class="hlt">CCD</span> show good agreement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006SPIE.6265E..43Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006SPIE.6265E..43Y"><span><span class="hlt">CCD</span> centroiding experiment for JASMINE and ILOM</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yano, Taihei; Araki, Hiroshi; Gouda, Naoteru; Kobayashi, Yukiyasu; Tsujimoto, Takuji; Nakajima, Tadashi; Kawano, Nobuyuki; Tazawa, Seiichi; Yamada, Yoshiyuki; Hanada, Hideo; Asari, Kazuyoshi; Tsuruta, Seiitsu</p> <p>2006-06-01</p> <p>JASMINE and ILOM are space missions which are in progress at the National Astronomical Observatory of Japan. These two projects need a common astrometric technique to obtain <span class="hlt">precise</span> positions of star images on solid state detectors to accomplish the objectives. We have carried out measurements of centroid of artificial star images on a <span class="hlt">CCD</span> to investigate the accuracy of the positions of the stars, using an algorithm for estimating them from photon weighted means of the stars. We find that the accuracy of the star positions reaches 1/300 pixel for one measurement. We also measure positions of stars, using an algorithm for correcting the distorted optical image. Finally, we find that the accuracy of the measurement for the positions of the stars from the strongly distorted image is under 1/150 pixel for one measurement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19780023370&hterms=chirp+analysis&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dchirp%2Banalysis','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19780023370&hterms=chirp+analysis&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dchirp%2Banalysis"><span>Spectral analysis using the <span class="hlt">CCD</span> Chirp Z-transform</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Eversole, W. L.; Mayer, D. J.; Bosshart, P. W.; Dewit, M.; Howes, C. R.; Buss, D. D.</p> <p>1978-01-01</p> <p>The charge coupled device (<span class="hlt">CCD</span>) Chirp Z transformation (CZT) spectral analysis techniques were reviewed and results on state-of-the-art <span class="hlt">CCD</span> CZT technology are presented. The CZT algorithm was examined and the advantages of <span class="hlt">CCD</span> implementation are discussed. The sliding CZT which is useful in many spectral analysis applications is described, and the performance limitations of the CZT are studied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JDSO...12...45A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JDSO...12...45A"><span><span class="hlt">CCD</span> Astrometry with Robotic Telescopes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>AlZaben, Faisal; Li, Dewei; Li, Yongyao; Dennis, Aren Fene, Michael; Boyce, Grady; Boyce, Pat</p> <p>2016-01-01</p> <p><span class="hlt">CCD</span> images were acquired of three binary star systems: WDS06145+1148, WDS06206+1803, and WDS06224+2640. The astrometric solution, position angle, and separation of each system were calculated with MaximDL v6 and Mira Pro x64 software suites. The results were consistent with historical measurements in the Washington Double Star Catalog. Our analysis found some differences in measurements between single-shot color <span class="hlt">CCD</span> cameras and traditional monochrome CCDs using a filter wheel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9915E..29S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9915E..29S"><span>Comparing simulations and test data of a radiation damaged <span class="hlt">CCD</span> for the Euclid mission</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Skottfelt, Jesper; Hall, David; Gow, Jason; Murray, Neil; Holland, Andrew; Prod'homme, Thibaut</p> <p>2016-07-01</p> <p>The radiation damage effects from the harsh radiative environment outside the Earth's atmosphere can be a cause for concern for most space missions. With the science goals becoming ever more demanding, the requirements on the <span class="hlt">precision</span> of the instruments on board these missions also increases, and it is therefore important to investigate how the radiation induced damage affects the Charge-Coupled Devices (CCDs) that most of these instruments rely on. The primary goal of the Euclid mission is to study the nature of dark matter and dark energy using weak lensing and baryonic acoustic oscillation techniques. The weak lensing technique depends on very <span class="hlt">precise</span> shape measurements of distant galaxies obtained by a large <span class="hlt">CCD</span> array. It is anticipated that over the 6 year nominal lifetime of mission, the CCDs will be degraded to an extent that these measurements will not be possible unless the radiation damage effects are corrected. We have therefore created a Monte Carlo model that simulates the physical processes taking place when transferring signal through a radiation damaged <span class="hlt">CCD</span>. The software is based on Shockley-Read-Hall theory, and is made to mimic the physical properties in the <span class="hlt">CCD</span> as close as possible. The code runs on a single electrode level and takes charge cloud size and density, three dimensional trap position, and multi-level clocking into account. A key element of the model is that it takes device specific simulations of electron density as a direct input, thereby avoiding to make any analytical assumptions about the size and density of the charge cloud. This paper illustrates how test data and simulated data can be compared in order to further our understanding of the positions and properties of the individual radiation-induced traps.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApPhL.110n1906P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhL.110n1906P"><span><span class="hlt">Ultra-high</span> strain in epitaxial silicon carbide nanostructures utilizing residual stress amplification</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Phan, Hoang-Phuong; Nguyen, Tuan-Khoa; Dinh, Toan; Ina, Ginnosuke; Kermany, Atieh Ranjbar; Qamar, Afzaal; Han, Jisheng; Namazu, Takahiro; Maeda, Ryutaro; Dao, Dzung Viet; Nguyen, Nam-Trung</p> <p>2017-04-01</p> <p>Strain engineering has attracted great attention, particularly for epitaxial films grown on a different substrate. Residual strains of SiC have been widely employed to form <span class="hlt">ultra-high</span> frequency and <span class="hlt">high</span> Q factor resonators. However, to date, the highest residual strain of SiC was reported to be limited to approximately 0.6%. Large strains induced into SiC could lead to several interesting physical phenomena, as well as significant improvement of resonant frequencies. We report an unprecedented nanostrain-amplifier structure with an <span class="hlt">ultra-high</span> residual strain up to 8% utilizing the natural residual stress between epitaxial 3C-SiC and Si. In addition, the applied strain can be tuned by changing the dimensions of the amplifier structure. The possibility of introducing such a controllable and <span class="hlt">ultra-high</span> strain will open the door to investigating the physics of SiC in large strain regimes and the development of <span class="hlt">ultra</span> sensitive mechanical sensors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApPhB.124..114Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApPhB.124..114Z"><span><span class="hlt">High</span>-power all-fiber <span class="hlt">ultra</span>-low noise laser</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Jian; Guiraud, Germain; Pierre, Christophe; Floissat, Florian; Casanova, Alexis; Hreibi, Ali; Chaibi, Walid; Traynor, Nicholas; Boullet, Johan; Santarelli, Giorgio</p> <p>2018-06-01</p> <p><span class="hlt">High</span>-power <span class="hlt">ultra</span>-low noise single-mode single-frequency lasers are in great demand for interferometric metrology. Robust, compact all-fiber lasers represent one of the most promising technologies to replace the current laser sources in use based on injection-locked ring resonators or multi-stage solid-state amplifiers. Here, a linearly polarized <span class="hlt">high</span>-power <span class="hlt">ultra</span>-low noise all-fiber laser is demonstrated at a power level of 100 W. Special care has been taken in the study of relative intensity noise (RIN) and its reduction. Using an optimized servo actuator to directly control the driving current of the pump laser diode, we obtain a large feedback bandwidth of up to 1.3 MHz. The RIN reaches - 160 dBc/Hz between 3 and 20 kHz.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/551041','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/551041"><span><span class="hlt">Ultra</span> <span class="hlt">high</span> vacuum broad band <span class="hlt">high</span> power microwave window</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Nguyen-Tuong, V.; Dylla, H.F. III</p> <p>1997-11-04</p> <p>An improved <span class="hlt">high</span> vacuum microwave window has been developed that utilizes <span class="hlt">high</span> density polyethylene coated on two sides with SiOx, SiNx, or a combination of the two. The resultant low dielectric and low loss tangent window creates a low outgassing, low permeation seal through which broad band, <span class="hlt">high</span> power microwave energy may be passed. No matching device is necessary and the sealing technique is simple. The features of the window are broad band transmission, <span class="hlt">ultra-high</span> vacuum compatibility with a simple sealing technique, low voltage standing wave ratio, <span class="hlt">high</span> power transmission and low cost. 5 figs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/871212','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/871212"><span><span class="hlt">Ultra</span> <span class="hlt">high</span> vacuum broad band <span class="hlt">high</span> power microwave window</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Nguyen-Tuong, Viet; Dylla, III, Henry Frederick</p> <p>1997-01-01</p> <p>An improved <span class="hlt">high</span> vacuum microwave window has been developed that utilizes <span class="hlt">high</span> density polyethylene coated on two sides with SiOx, SiNx, or a combination of the two. The resultant low dielectric and low loss tangent window creates a low outgassing, low permeation seal through which broad band, <span class="hlt">high</span> power microwave energy may be passed. No matching device is necessary and the sealing technique is simple. The features of the window are broad band transmission, <span class="hlt">ultra-high</span> vacuum compatibility with a simple sealing technique, low voltage standing wave ratio, <span class="hlt">high</span> power transmission and low cost.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AstL...40..125B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AstL...40..125B"><span><span class="hlt">CCD</span> BVI c observations of Cepheids</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Berdnikov, L. N.; Kniazev, A. Yu.; Sefako, R.; Kravtsov, V. V.; Zhujko, S. V.</p> <p>2014-02-01</p> <p>In 2008-2013, we obtained 11333 <span class="hlt">CCD</span> BVI c frames for 57 Cepheids from the General Catalogue of Variable Stars. We performed our observations with the 76-cm telescope of the South African Astronomical Observatory (SAAO, South Africa) and the 40-cm telescope of the Cerro Armazones Astronomical Observatory of the Universidad Católica del Norte (OCA, Chile) using the SBIG ST-10XME <span class="hlt">CCD</span> camera. The tables of observations, the plots of light curves, and the current light elements are presented. Comparison of our light curves with those constructed from photoelectric observations shows that the differences between their mean magnitudes exceed 0ṃ05 in 20% of the cases. This suggests the necessity of performing <span class="hlt">CCD</span> observations for all Cepheids.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/919845','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/919845"><span>Robotic <span class="hlt">CCD</span> microscope for enhanced crystal recognition</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Segelke, Brent W.; Toppani, Dominique</p> <p>2007-11-06</p> <p>A robotic <span class="hlt">CCD</span> microscope and procedures to automate crystal recognition. The robotic <span class="hlt">CCD</span> microscope and procedures enables more accurate crystal recognition, leading to fewer false negative and fewer false positives, and enable detection of smaller crystals compared to other methods available today.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011SPIE.8148E..0SN','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011SPIE.8148E..0SN"><span>Atmospheric turbulence and <span class="hlt">high-precision</span> ground-based solar polarimetry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nagaraju, K.; Feller, A.; Ihle, S.; Soltau, H.</p> <p>2011-10-01</p> <p><span class="hlt">High-precision</span> full-Stokes polarimetry at near diffraction limited spatial resolution is important to understand numerous physical processes on the Sun. In view of the next generation of ground based solar telescopes, we have explored, through numerical simulation, how polarimetric accuracy is affected by atmospheric seeing, especially in the case of large aperture telescopes with increasing ratio between mirror diameter and Fried parameter. In this work we focus on higher-order wavefront aberrations. The numerical generation of time-dependent turbulence phase screens is based on the well-known power spectral method and on the assumption that the temporal evolution is mainly caused by wind driven propagation of frozen-in turbulence across the telescope. To analyze the seeing induced cross-talk between the Stokes parameters we consider polarization modulation scheme based on a continuously rotating waveplate with rotation frequencies between 1 Hz and several 100 Hz. Further, we have started the development of a new fast solar imaging polarimeter, based on pn<span class="hlt">CCD</span> detector technology from PNSensor. The first detector will have a size of 264 x 264 pixels and will work at frame rates of up to 1kHz, combined with a very low readout noise of 2-3 e- ENC. The camera readout electronics will allow for buffering and accumulation of images corresponding to the different phases of the fast polarization modulation. A <span class="hlt">high</span> write-out rate (about 30 to 50 frames/s) will allow for post-facto image reconstruction. We will present the concept and the expected performance of the new polarimeter, based on the above-mentioned simulations of atmospheric seeing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007SPIE.6616E..21J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007SPIE.6616E..21J"><span><span class="hlt">Precision</span> mechatronics based on <span class="hlt">high-precision</span> measuring and positioning systems and machines</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jäger, Gerd; Manske, Eberhard; Hausotte, Tino; Mastylo, Rostyslav; Dorozhovets, Natalja; Hofmann, Norbert</p> <p>2007-06-01</p> <p><span class="hlt">Precision</span> mechatronics is defined in the paper as the science and engineering of a new generation of <span class="hlt">high</span> <span class="hlt">precision</span> systems and machines. Nanomeasuring and nanopositioning engineering represents important fields of <span class="hlt">precision</span> mechatronics. The nanometrology is described as the today's limit of the <span class="hlt">precision</span> engineering. The problem, how to design nanopositioning machines with uncertainties as small as possible will be discussed. The integration of several optical and tactile nanoprobes makes the 3D-nanopositioning machine suitable for various tasks, such as long range scanning probe microscopy, mask and wafer inspection, nanotribology, nanoindentation, free form surface measurement as well as measurement of microoptics, <span class="hlt">precision</span> molds, microgears, ring gauges and small holes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28740818','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28740818"><span>Disrupted latent inhibition in individuals at <span class="hlt">ultra</span> <span class="hlt">high</span>-risk for developing psychosis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kraus, Michael; Rapisarda, Attilio; Lam, Max; Thong, Jamie Y J; Lee, Jimmy; Subramaniam, Mythily; Collinson, Simon L; Chong, Siow Ann; Keefe, Richard S E</p> <p>2016-12-01</p> <p>The addition of off-the-shelf cognitive measures to established prodromal criteria has resulted in limited improvement in the prediction of conversion to psychosis. Tests that assess cognitive processes central to schizophrenia might better identify those at highest risk. The latent inhibition paradigm assesses a subject's tendency to ignore irrelevant stimuli, a process integral to healthy perceptual and cognitive function that has been hypothesized to be a key deficit underlying the development of schizophrenia. In this study, 142 young people at <span class="hlt">ultra</span> <span class="hlt">high</span>-risk for developing psychosis and 105 controls were tested on a within-subject latent inhibition paradigm. Additionally, we later inquired about the strategy that each subject employed to complete the test, and further investigated the relationship between reported strategy and the extent of latent inhibition exhibited. Unlike controls, <span class="hlt">ultra</span> <span class="hlt">high</span>-risk subjects did not demonstrate a significant latent inhibition effect. This difference between groups became greater when controlling for strategy. The lack of latent inhibition effect in our <span class="hlt">ultra</span> <span class="hlt">high</span>-risk sample suggests that individuals at <span class="hlt">ultra</span> <span class="hlt">high</span>-risk for psychosis are impaired in their allocation of attentional resources based on past predictive value of repeated stimuli. This fundamental deficit in the allocation of attention may contribute to the broader array of cognitive impairments and clinical symptoms displayed by individuals at <span class="hlt">ultra</span> <span class="hlt">high</span>-risk for psychosis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10385E..0BY','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10385E..0BY"><span>A portable device for calibration of autocollimators with nanoradian <span class="hlt">precision</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yandayan, Tanfer</p> <p>2017-09-01</p> <p>A portable device has been developed in TUBITAK UME to calibrate <span class="hlt">high</span> <span class="hlt">precision</span> autocollimators with nanoradian <span class="hlt">precision</span>. The device can operate in the range of +/-4500" which is far enough for the calibration of the available autocollimators and can generate <span class="hlt">ultra</span>-small angles in measurement steps of 0.0005" (2.5 nrad). Description of the device with the performance tests using the calibrated <span class="hlt">precise</span> autocollimators and novel methods will be reported. The test results indicate that the device is a good candidate for application to on-site/in-situ calibration of autocollimators with expanded uncertainties of 0.01" (50 nrad) particularly those used in slope measuring profilers.</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/2010PhDT.......173R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhDT.......173R"><span>Search for <span class="hlt">ultra</span> <span class="hlt">high</span> energy astrophysical neutrinos with the ANITA experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Romero-Wolf, Andrew</p> <p>2010-12-01</p> <p>This work describes a search for cosmogenic neutrinos at energies above 1018 eV with the Antarctic Impulsive Transient Antenna (ANITA). ANITA is a balloon-borne radio interferometer designed to measure radio impulsive emission from particle showers produced in the Antarctic ice-sheet by <span class="hlt">ultra-high</span> energy neutrinos (UHEnu). Flying at 37 km altitude the ANITA detector is sensitive to 1M km3 of ice and is expected to produce the highest exposure to <span class="hlt">ultra</span> <span class="hlt">high</span> energy neutrinos to date. The design, flight performance, and analysis of the first flight of ANITA in 2006 are the subject of this dissertation. Due to sparse anthropogenic backgrounds throughout the Antarctic continent, the ANITA analysis depends on <span class="hlt">high</span> resolution directional reconstruction. An interferometric method was developed that not only provides <span class="hlt">high</span> resolution but is also sensitive to very weak radio emissions. The results of ANITA provide the strongest constraints on current <span class="hlt">ultra-high</span> energy neutrino models. In addition there was a serendipitous observation of <span class="hlt">ultra-high</span> energy cosmic ray geosynchrotron emissions that are of distinct character from the expected neutrino signal. This thesis includes a study of the radio Cherenkov emission from <span class="hlt">ultra-high</span> energy electromagnetic showers in ice in the time-domain. All previous simulations computed the radio pulse frequency spectrum. I developed a purely time-domain algorithm for computing radiation using the vector potentials of charged particle tracks. The results are fully consistent with previous frequency domain calculations and shed new light into the properties of the radio pulse in the time domain. The shape of the pulse in the time domain is directly related to the depth development of the excess charge in the shower and its width to the observation angle with respect to the Cherenkov direction. This information can be of great practical importance for interpreting actual data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15753238','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15753238"><span>Imaging frontostriatal function in <span class="hlt">ultra-high</span>-risk, early, and chronic schizophrenia during executive processing.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Morey, Rajendra A; Inan, Seniha; Mitchell, Teresa V; Perkins, Diana O; Lieberman, Jeffrey A; Belger, Aysenil</p> <p>2005-03-01</p> <p>Individuals experiencing prodromal symptoms of schizophrenia (<span class="hlt">ultra-high</span>-risk group) demonstrate impaired performance on tasks of executive function, attention, and working memory. The neurobiological underpinnings of such executive deficits in <span class="hlt">ultra-high</span>-risk individuals remains unclear. We assessed frontal and striatal functions during a visual oddball continuous performance task, in <span class="hlt">ultra-high</span>-risk, early, and chronic schizophrenic patients with the use of functional magnetic resonance imaging. Cross-sectional case-control design. Community; outpatient clinic. Patients Fifty-two individuals (control, n = 16; <span class="hlt">ultra-high</span> risk, n = 10; early, n = 15; chronic, n = 11) from a referred clinical sample and age- and sex-matched control volunteers underwent scanning. Percentage of active voxels and percentage signal change calculated for the anterior cingulate gyrus (ACG), middle frontal gyrus (MFG), inferior frontal gyrus (IFG), basal ganglia, and thalamus. Performance on the visual oddball task was measured with percentage of hits and d' (a measure based on the hit rate and the false-alarm rate). The <span class="hlt">ultra-high</span>-risk group showed significantly smaller differential activation between task-relevant and task-irrelevant stimuli in the frontal regions (ACG, IFG, MFG) than the control group. Frontostriatal activation associated with target stimuli in the early and chronic groups was significantly lower than the control group, while the <span class="hlt">ultra-high</span>-risk group showed a trend toward the early group. Our findings suggest that prefrontal function begins to decline before the onset of syndromally defined illness and hence may represent a vulnerability marker in assessing the risk of developing psychotic disorders among <span class="hlt">ultra-high</span>-risk individuals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9152E..1YZ','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9152E..1YZ"><span>A <span class="hlt">CCD</span> experimental platform for large telescope in Antarctica based on FPGA</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Yuhua; Qi, Yongjun</p> <p>2014-07-01</p> <p>The <span class="hlt">CCD</span> , as a detector , is one of the important components of astronomical telescopes. For a large telescope in Antarctica, a set of <span class="hlt">CCD</span> detector system with large size, <span class="hlt">high</span> sensitivity and low noise is indispensable. Because of the extremely low temperatures and unattended, system maintenance and software and hardware upgrade become hard problems. This paper introduces a general <span class="hlt">CCD</span> controller experiment platform, using Field programmable gate array FPGA, which is, in fact, a large-scale field reconfigurable array. Taking the advantage of convenience to modify the system, construction of driving circuit, digital signal processing module, network communication interface, control algorithm validation, and remote reconfigurable module may realize. With the concept of integrated hardware and software, the paper discusses the key technology of building scientific <span class="hlt">CCD</span> system suitable for the special work environment in Antarctica, focusing on the method of remote reconfiguration for controller via network and then offering a feasible hardware and software solution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EntIS..10..970H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EntIS..10..970H"><span>Ontological modelling of knowledge management for human-machine integrated design of <span class="hlt">ultra-precision</span> grinding machine</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hong, Haibo; Yin, Yuehong; Chen, Xing</p> <p>2016-11-01</p> <p>Despite the rapid development of computer science and information technology, an efficient human-machine integrated enterprise information system for designing complex mechatronic products is still not fully accomplished, partly because of the inharmonious communication among collaborators. Therefore, one challenge in human-machine integration is how to establish an appropriate knowledge management (KM) model to support integration and sharing of heterogeneous product knowledge. Aiming at the diversity of design knowledge, this article proposes an ontology-based model to reach an unambiguous and normative representation of knowledge. First, an ontology-based human-machine integrated design framework is described, then corresponding ontologies and sub-ontologies are established according to different purposes and scopes. Second, a similarity calculation-based ontology integration method composed of ontology mapping and ontology merging is introduced. The ontology searching-based knowledge sharing method is then developed. Finally, a case of human-machine integrated design of a large <span class="hlt">ultra-precision</span> grinding machine is used to demonstrate the effectiveness of the method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9543E..0AZ','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9543E..0AZ"><span>Typical effects of laser dazzling <span class="hlt">CCD</span> camera</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Zhen; Zhang, Jianmin; Shao, Bibo; Cheng, Deyan; Ye, Xisheng; Feng, Guobin</p> <p>2015-05-01</p> <p>In this article, an overview of laser dazzling effect to buried channel <span class="hlt">CCD</span> camera is given. The CCDs are sorted into staring and scanning types. The former includes the frame transfer and interline transfer types. The latter includes linear and time delay integration types. All CCDs must perform four primary tasks in generating an image, which are called charge generation, charge collection, charge transfer and charge measurement. In camera, the lenses are needed to input the optical signal to the <span class="hlt">CCD</span> sensors, in which the techniques for erasing stray light are used. And the electron circuits are needed to process the output signal of <span class="hlt">CCD</span>, in which many electronic techniques are used. The dazzling effects are the conjunct result of light distribution distortion and charge distribution distortion, which respectively derive from the lens and the sensor. Strictly speaking, in lens, the light distribution is not distorted. In general, the lens are so well designed and fabricated that its stray light can be neglected. But the laser is of much enough intensity to make its stray light obvious. In <span class="hlt">CCD</span> image sensors, laser can induce a so large electrons generation. Charges transfer inefficiency and charges blooming will cause the distortion of the charge distribution. Commonly, the largest signal outputted from <span class="hlt">CCD</span> sensor is restricted by capability of the collection well of <span class="hlt">CCD</span>, and can't go beyond the dynamic range for the subsequent electron circuits maintaining normal work. So the signal is not distorted in the post-processing circuits. But some techniques in the circuit can make some dazzling effects present different phenomenon in final image.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA637199','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA637199"><span><span class="hlt">Ultra</span> Fast, <span class="hlt">High</span> Rep Rate, <span class="hlt">High</span> Voltage Spark Gap Pulser</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1995-07-01</p> <p>current rise time. The spark gap was designed to have a coaxial geometry reducing its inductance. Provisions were made to pass flowing gas between the...<span class="hlt">ULTRA</span> FAST, <span class="hlt">HIGH</span> REP RATE, <span class="hlt">HIGH</span> VOLTAGE SPARK GAP PULSER Robert A. Pastore Jr., Lawrence E. Kingsley, Kevin Fonda, Erik Lenzing Electrophysics and...Modeling Branch AMSRL-PS-EA Tel.: (908)-532-0271 FAX: (908)-542-3348 U.S. Army Research Laboratory Physical Sciences Directorate Ft. Monmouth</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AzAJ....4c..42A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AzAJ....4c..42A"><span><span class="hlt">CCD</span> Photometer Installed on the Telescope - 600 OF the Shamakhy Astrophysical Observatory II. The Technique of Observation and Data Processing of <span class="hlt">CCD</span> Photometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Abdullayev, B. I.; Gulmaliyev, N. I.; Majidova, S. O.; Mikayilov, Kh. M.; Rustamov, B. N.</p> <p>2009-12-01</p> <p>Basic technical characteristics of <span class="hlt">CCD</span> matrix U-47 made by the Apogee Alta Instruments Inc. are provided. Short description and features of various noises introduced by optical system and <span class="hlt">CCD</span> camera are presented. The technique of getting calibration frames: bias, dark, flat field and main stages of processing of results <span class="hlt">CCD</span> photometry are described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19960018811&hterms=succession&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dsuccession','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19960018811&hterms=succession&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dsuccession"><span><span class="hlt">CCD</span> Detects Two Images In Quick Succession</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Janesick, James R.; Collins, Andy</p> <p>1996-01-01</p> <p>Prototype special-purpose charge-coupled device (<span class="hlt">CCD</span>) designed to detect two 1,024 x 1,024-pixel images in rapid succession. Readout performed slowly to minimize noise. <span class="hlt">CCD</span> operated in synchronism with pulsed laser, stroboscope, or other pulsed source of light to form pairs of images of rapidly moving objects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/4771031','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/4771031"><span>BAKABLE <span class="hlt">ULTRA-HIGH</span> VACUUM VALVE</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Mark, J.T.; Gantz, I.H.</p> <p>1962-07-10</p> <p>S>This patent relates to a valve useful in applications involving successively closing and opening a communication between a chamber evacuated to an <span class="hlt">ultra-high</span> vacuum condition of the order of 10/sup -10/ millimeters of mercury and another chamber or the ambient. The valve is capable of withstanding extended baking at 450 deg C and repeated opening and closing without repiacement of the valve seat (approximately 200 cycle limit). The seal is formed by mutual interdiffusion weld, coerced by a pneumatic actuator. (AEC)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-jsc2017m000655_Spacewalking_in_Ultra_High_Definition-YT4K.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-jsc2017m000655_Spacewalking_in_Ultra_High_Definition-YT4K.html"><span>Spacewalking_in_<span class="hlt">Ultra_High</span>_Definition</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2017-07-21</p> <p>Ever wonder what the spacewalker sees while you’re looking at him or her? Here’s your answer, courtesy of NASA astronaut Jack Fischer. This <span class="hlt">Ultra</span> <span class="hlt">High</span> Definition clip shows Fischer outside the International Space Station during a spacewalk on Expedition 51 in May 2017, and the view from a small camera attached to his spacesuit at the same time. Music by Joakim Karud. _______________________________________ FOLLOW THE SPACE STATION! Twitter: https://twitter.com/Space_Station Facebook: https://www.facebook.com/ISS Instagram: https://instagram.com/iss/</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PTEP.2017lA107C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PTEP.2017lA107C"><span>Observation of <span class="hlt">ultra</span> <span class="hlt">high</span> energy cosmic rays from space: Status and perspectives</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Casolino, M.; Klimov, P.; Piotrowski, L.</p> <p>2017-12-01</p> <p>The study of <span class="hlt">ultra</span> <span class="hlt">high</span> energy cosmic rays (UHECRs) offers unique possibilities to probe the energies currently inaccessible by man-made accelerators. Recent years have shed light on several characteristics of these particles, but—due to their extremely low flux—their origin, nature, and acceleration mechanisms are still unclear. Space-based observations have the potential for an increase in statistics, up to several orders of magnitude, and would be able to cover the whole sky, allowing for a direct comparison of spectra and direction of arrival. A detector with the exposure of a few times that of the Pierre Auger Observatory would be able to clarify the observed differences between the northern and southern skies, confirm the existence of TA hot spot, and measure multipolar anisotropies with <span class="hlt">high</span> <span class="hlt">precision</span>. A number of novel technologies—from optics to sensors, front-end and read-out electronics—have been developed over the years to achieve this goal. In this paper we describe the progress and results obtained so far and discuss the perspectives of UHECR physics observation from space.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/9889815','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/9889815"><span>Design principles and applications of a cooled <span class="hlt">CCD</span> camera for electron microscopy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Faruqi, A R</p> <p>1998-01-01</p> <p>Cooled <span class="hlt">CCD</span> cameras offer a number of advantages in recording electron microscope images with CCDs rather than film which include: immediate availability of the image in a digital format suitable for further computer processing, <span class="hlt">high</span> dynamic range, excellent linearity and a <span class="hlt">high</span> detective quantum efficiency for recording electrons. In one important respect however, film has superior properties: the spatial resolution of <span class="hlt">CCD</span> detectors tested so far (in terms of point spread function or modulation transfer function) are inferior to film and a great deal of our effort has been spent in designing detectors with improved spatial resolution. Various instrumental contributions to spatial resolution have been analysed and in this paper we discuss the contribution of the phosphor-fibre optics system in this measurement. We have evaluated the performance of a number of detector components and parameters, e.g. different phosphors (and a scintillator), optical coupling with lens or fibre optics with various demagnification factors, to improve the detector performance. The camera described in this paper, which is based on this analysis, uses a tapered fibre optics coupling between the phosphor and the <span class="hlt">CCD</span> and is installed on a Philips CM12 electron microscope equipped to perform cryo-microscopy. The main use of the camera so far has been in recording electron diffraction patterns from two dimensional crystals of bacteriorhodopsin--from wild type and from different trapped states during the photocycle. As one example of the type of data obtained with the <span class="hlt">CCD</span> camera a two dimensional Fourier projection map from the trapped O-state is also included. With faster computers, it will soon be possible to undertake this type of work on an on-line basis. Also, with improvements in detector size and resolution, <span class="hlt">CCD</span> detectors, already ideal for diffraction, will be able to compete with film in the recording of <span class="hlt">high</span> resolution images.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9372E..0FK','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9372E..0FK"><span>Bringing mirrors to rest: grating concepts for <span class="hlt">ultra-precise</span> interferometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kroker, Stefanie; Kley, Ernst-Bernhard; Tünnermann, Andreas</p> <p>2015-02-01</p> <p>Experiments in the field of <span class="hlt">high</span> <span class="hlt">precision</span> metrology such as the detection of gravitational waves are crucially limited by the thermal fluctuations of the optical components. In this contribution we present the current state of knowledge of <span class="hlt">high</span> contrast gratings (HCGs) as low-noise elements for gravitational wave interferometers. We discuss how the properties of HCGs can be tailored such that beside <span class="hlt">highly</span> reflective mirrors also diffractive beam splitters can be realized. Further, we show the impact of such gratings on the sensitivity of future gravitational wave detectors which can pave the way for the new field of gravitational wave astronomy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27645769','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27645769"><span>A rapid method for the simultaneous determination of 25 anti-hypertensive compounds in dietary supplements using <span class="hlt">ultra-high</span>-pressure liquid chromatography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Heo, Seok; Yoo, Geum Joo; Choi, Ji Yeon; Park, Hyoung Joon; Park, Sung-Kwan; Baek, Sun Young</p> <p>2016-11-01</p> <p>A novel, stable, simple and specific <span class="hlt">ultra</span>-performance liquid chromatography method with ultraviolet detection (205 nm) for the simultaneous analysis of 25 anti-hypertensive substances was developed. The method was validated according to the International Conference of Harmonisation guidelines with respect to linearity, accuracy, <span class="hlt">precision</span>, limit of detection (LOD), limit of quantitation (LOQ) and stability. From the <span class="hlt">ultra</span>-performance liquid chromatography results, we identified the LOD and LOQ of solid samples to be 0.20-1.00 and 0.60-3.00 μg ml -1 , respectively, while those of liquid samples were 0.30-1.20 and 0.90-3.60 μg ml -1 , respectively. The linearity exceeded 0.9999, and the intra- and inter-day <span class="hlt">precisions</span> were 0.15-6.48% and 0.28-8.67%, respectively. The intra- and inter-day accuracies were 82.25-111.42% and 80.70-115.64%, respectively, and the stability was lower than 12.9% (relative standard deviation). This method was applied to the monitoring of 97 commercially available dietary supplements obtained in Korea, such as pills, soft capsules, hard capsules, liquids, powders and tablets. The proposed method is accurate, <span class="hlt">precise</span> and of <span class="hlt">high</span> quality, and can be used for the routine, reproducible analysis and control of 25 anti-hypertensive substances in various dietary supplements. The work presented herein may help to prevent incidents related to food adulteration and restrict the illegal food market.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19770010321&hterms=transversal+study&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dtransversal%2Bstudy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19770010321&hterms=transversal+study&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dtransversal%2Bstudy"><span><span class="hlt">CCD</span> filter and transform techniques for interference excision</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Borsuk, G. M.; Dewitt, R. N.</p> <p>1976-01-01</p> <p>The theoretical and some experimental results of a study aimed at applying <span class="hlt">CCD</span> filter and transform techniques to the problem of interference excision within communications channels were presented. Adaptive noise (interference) suppression was achieved by the modification of received signals such that they were orthogonal to the recently measured noise field. <span class="hlt">CCD</span> techniques were examined to develop real-time noise excision processing. They were recursive filters, circulating filter banks, transversal filter banks, an optical implementation of the chirp Z transform, and a <span class="hlt">CCD</span> analog FFT.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1988NIMPA.266..563S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1988NIMPA.266..563S"><span><span class="hlt">CCD</span> sensors in synchrotron X-ray detectors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Strauss, M. G.; Naday, I.; Sherman, I. S.; Kraimer, M. R.; Westbrook, E. M.; Zaluzec, N. J.</p> <p>1988-04-01</p> <p>The intense photon flux from advanced synchrotron light sources, such as the 7-GeV synchrotron being designed at Argonne, require integrating-type detectors. Charge-coupled devices (CCDs) are well suited as synchrotron X-ray detectors. When irradiated indirectly via a phosphor followed by reducing optics, diffraction patterns of 100 cm 2 can be imaged on a 2 cm 2 <span class="hlt">CCD</span>. With a conversion efficiency of ˜ 1 <span class="hlt">CCD</span> electron/X-ray photon, a peak saturation capacity of > 10 6 X-rays can be obtained. A programmable <span class="hlt">CCD</span> controller operating at a clock frequency of 20 MHz has been developed. The readout rate is 5 × 10 6 pixels/s and the shift rate in the parallel registers is 10 6 lines/s. The test detector was evaluated in two experiments. In protein crystallography diffraction patterns have been obtained from a lysozyme crystal using a conventional rotating anode X-ray generator. Based on these results we expect to obtain at a synchrotron diffraction images at a rate of ˜ 1 frame/s or a complete 3-dimensional data set from a single crystal in ˜ 2 min. In electron energy-loss spectroscopy (EELS), the <span class="hlt">CCD</span> was used in a parallel detection mode which is similar to the mode array detectors are used in dispersive EXAFS. With a beam current corresponding to 3 × 10 9 electron/s on the detector, a series of 64 spectra were recorded on the <span class="hlt">CCD</span> in a continuous sequence without interruption due to readout. The frame-to-frame pixel signal fluctuations had σ = 0.4% from which DQE = 0.4 was obtained, where the detector conversion efficiency was 2.6 <span class="hlt">CCD</span> electrons/X-ray photon. These multiple frame series also showed the time-resolved modulation of the electron microscope optics by stray magnetic fields.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9284E..16L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9284E..16L"><span>Design of area array <span class="hlt">CCD</span> image acquisition and display system based on FPGA</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Lei; Zhang, Ning; Li, Tianting; Pan, Yue; Dai, Yuming</p> <p>2014-09-01</p> <p>With the development of science and technology, <span class="hlt">CCD</span>(Charge-coupled Device) has been widely applied in various fields and plays an important role in the modern sensing system, therefore researching a real-time image acquisition and display plan based on <span class="hlt">CCD</span> device has great significance. This paper introduces an image data acquisition and display system of area array <span class="hlt">CCD</span> based on FPGA. Several key technical challenges and problems of the system have also been analyzed and followed solutions put forward .The FPGA works as the core processing unit in the system that controls the integral time sequence .The ICX285AL area array <span class="hlt">CCD</span> image sensor produced by SONY Corporation has been used in the system. The FPGA works to complete the driver of the area array <span class="hlt">CCD</span>, then analog front end (AFE) processes the signal of the <span class="hlt">CCD</span> image, including amplification, filtering, noise elimination, CDS correlation double sampling, etc. AD9945 produced by ADI Corporation to convert analog signal to digital signal. Developed Camera Link <span class="hlt">high</span>-speed data transmission circuit, and completed the PC-end software design of the image acquisition, and realized the real-time display of images. The result through practical testing indicates that the system in the image acquisition and control is stable and reliable, and the indicators meet the actual project requirements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19760021746','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19760021746"><span>A 128K-bit <span class="hlt">CCD</span> buffer memory system</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Siemens, K. H.; Wallace, R. W.; Robinson, C. R.</p> <p>1976-01-01</p> <p>A prototype system was implemented to demonstrate that <span class="hlt">CCD</span>'s can be applied advantageously to the problem of low power digital storage and particularly to the problem of interfacing widely varying data rates. 8K-bit <span class="hlt">CCD</span> shift register memories were used to construct a feasibility model 128K-bit buffer memory system. Peak power dissipation during a data transfer is less than 7 W., while idle power is approximately 5.4 W. The system features automatic data input synchronization with the recirculating <span class="hlt">CCD</span> memory block start address. Descriptions are provided of both the buffer memory system and a custom tester that was used to exercise the memory. The testing procedures and testing results are discussed. Suggestions are provided for further development with regards to the utilization of advanced versions of <span class="hlt">CCD</span> memory devices to both simplified and expanded memory system applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018OptLE.105..125Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018OptLE.105..125Z"><span>Self-cleaning effect in <span class="hlt">high</span> quality percussion ablating of cooling hole by picosecond <span class="hlt">ultra</span>-short pulse laser</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Wanqin; Yu, Zhishui</p> <p>2018-06-01</p> <p>Comparing with the trepanning technology, cooling hole could be processed based on the percussion drilling with higher processing efficiency. However, it is widely believed that the ablating <span class="hlt">precision</span> of hole is lower for percussion drilling than for trepanning, wherein, the melting spatter materials around the hole surface and the recast layer inside the hole are the two main issues for reducing the ablating <span class="hlt">precision</span> of hole, especially for the recast layer, it can't be eliminated completely even through the trepanning technology. In this paper, the self-cleaning effect which is a particular property just for percussion ablating of holes has been presented in detail. In addition, the reasons inducing the self-cleaning effect have been discussed. At last, based on the self-cleaning effect of percussion drilling, <span class="hlt">high</span> quality cooling hole without the melting spatter materials around the hole surface and recast layer inside the hole could be ablated in nickel-based superalloy by picosecond <span class="hlt">ultra</span>-short pulse laser.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016RScI...87f3909B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016RScI...87f3909B"><span><span class="hlt">Ultra-high</span> vacuum compatible induction-heated rod casting furnace</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bauer, A.; Neubauer, A.; Münzer, W.; Regnat, A.; Benka, G.; Meven, M.; Pedersen, B.; Pfleiderer, C.</p> <p>2016-06-01</p> <p>We report the design of a radio-frequency induction-heated rod casting furnace that permits the preparation of polycrystalline ingots of intermetallic compounds under <span class="hlt">ultra-high</span> vacuum compatible conditions. The central part of the system is a bespoke water-cooled Hukin crucible supporting a casting mold. Depending on the choice of the mold, typical rods have a diameter between 6 mm and 10 mm and a length up to 90 mm, suitable for single-crystal growth by means of float-zoning. The setup is all-metal sealed and may be baked out. We find that the resulting <span class="hlt">ultra-high</span> vacuum represents an important precondition for processing compounds with <span class="hlt">high</span> vapor pressures under a <span class="hlt">high</span>-purity argon atmosphere up to 3 bars. Using the rod casting furnace, we succeeded to prepare large <span class="hlt">high</span>-quality single crystals of two half-Heusler compounds, namely, the itinerant antiferromagnet CuMnSb and the half-metallic ferromagnet NiMnSb.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_13 --> <div id="page_14" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="261"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27370472','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27370472"><span><span class="hlt">Ultra-high</span> vacuum compatible induction-heated rod casting furnace.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bauer, A; Neubauer, A; Münzer, W; Regnat, A; Benka, G; Meven, M; Pedersen, B; Pfleiderer, C</p> <p>2016-06-01</p> <p>We report the design of a radio-frequency induction-heated rod casting furnace that permits the preparation of polycrystalline ingots of intermetallic compounds under <span class="hlt">ultra-high</span> vacuum compatible conditions. The central part of the system is a bespoke water-cooled Hukin crucible supporting a casting mold. Depending on the choice of the mold, typical rods have a diameter between 6 mm and 10 mm and a length up to 90 mm, suitable for single-crystal growth by means of float-zoning. The setup is all-metal sealed and may be baked out. We find that the resulting <span class="hlt">ultra-high</span> vacuum represents an important precondition for processing compounds with <span class="hlt">high</span> vapor pressures under a <span class="hlt">high</span>-purity argon atmosphere up to 3 bars. Using the rod casting furnace, we succeeded to prepare large <span class="hlt">high</span>-quality single crystals of two half-Heusler compounds, namely, the itinerant antiferromagnet CuMnSb and the half-metallic ferromagnet NiMnSb.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SPIE.7544E..6KM','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SPIE.7544E..6KM"><span>Theoretical and experimental research on machine tool servo system for <span class="hlt">ultra-precision</span> position compensation on CNC lathe</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ma, Zhichao; Hu, Leilei; Zhao, Hongwei; Wu, Boda; Peng, Zhenxing; Zhou, Xiaoqin; Zhang, Hongguo; Zhu, Shuai; Xing, Lifeng; Hu, Huang</p> <p>2010-08-01</p> <p>The theories and techniques for improving machining accuracy via position control of diamond tool's tip and raising resolution of cutting depth on <span class="hlt">precise</span> CNC lathes have been extremely focused on. A new piezo-driven <span class="hlt">ultra-precision</span> machine tool servo system is designed and tested to improve manufacturing accuracy of workpiece. The mathematical model of machine tool servo system is established and the finite element analysis is carried out on parallel plate flexure hinges. The output position of diamond tool's tip driven by the machine tool servo system is tested via a contact capacitive displacement sensor. Proportional, integral, derivative (PID) feedback is also implemented to accommodate and compensate dynamical change owing cutting forces as well as the inherent non-linearity factors of the piezoelectric stack during cutting process. By closed loop feedback controlling strategy, the tracking error is limited to 0.8 μm. Experimental results have shown the proposed machine tool servo system could provide a tool positioning resolution of 12 nm, which is much accurate than the inherent CNC resolution magnitude. The stepped shaft of aluminum specimen with a step increment of cutting depth of 1 μm is tested, and the obtained contour illustrates the displacement command output from controller is accurately and real-time reflected on the machined part.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22251160-precision-control-multiple-quantum-cascade-lasers-calibration-systems','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22251160-precision-control-multiple-quantum-cascade-lasers-calibration-systems"><span><span class="hlt">Precision</span> control of multiple quantum cascade lasers for calibration 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>Taubman, Matthew S., E-mail: Matthew.Taubman@pnnl.gov; Myers, Tanya L.; Pratt, Richard M.</p> <p></p> <p>We present a <span class="hlt">precision</span>, 1-A, digitally interfaced current controller for quantum cascade lasers, with demonstrated temperature coefficients for continuous and 40-kHz full-depth square-wave modulated operation, of 1–2 ppm/ °C and 15 ppm/ °C, respectively. <span class="hlt">High</span> <span class="hlt">precision</span> digital to analog converters (DACs) together with an <span class="hlt">ultra-precision</span> voltage reference produce <span class="hlt">highly</span> stable, <span class="hlt">precision</span> voltages, which are selected by a multiplexer (MUX) chip to set output currents via a linear current regulator. The controller is operated in conjunction with a power multiplexing unit, allowing one of three lasers to be driven by the controller, while ensuring protection of controller and all lasers during operation, standby,more » and switching. Simple ASCII commands sent over a USB connection to a microprocessor located in the current controller operate both the controller (via the DACs and MUX chip) and the power multiplexer.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1438536','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1438536"><span>Search for <span class="hlt">Ultra-High</span> Energy Photons with the Pierre Auger Observatory</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>Homola, Piotr</p> <p></p> <p>One of key scientific objectives of the Pierre Auger Observatory is the search for <span class="hlt">ultra-high</span> energy photons. Such photons could originate either in the interactions of energetic cosmic-ray nuclei with the cosmic microwave background (so-called cosmogenic photons) or in the exotic scenarios, e.g. those assuming a production and decay of some hypothetical super-massive particles. The latter category of models would imply relatively large fluxes of photons with <span class="hlt">ultra-high</span> energies at Earth, while the former, involving interactions of cosmic-ray nuclei with the microwave background - just the contrary: very small fractions. The investigations on the data collected so far in themore » Pierre Auger Observatory led to placing very stringent limits to <span class="hlt">ultra-high</span> energy photon fluxes: below the predictions of the most of the exotic models and nearing the predicted fluxes of the cosmogenic photons. In this paper the status of these investigations and perspectives for further studies are summarized.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22007424','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22007424"><span>[Atmospheric correction of HJ-1 <span class="hlt">CCD</span> data for water imagery based on dark object model].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhou, Li-Guo; Ma, Wei-Chun; Gu, Wan-Hua; Huai, Hong-Yan</p> <p>2011-08-01</p> <p>The <span class="hlt">CCD</span> multi-band data of HJ-1A has great potential in inland water quality monitoring, but the <span class="hlt">precision</span> of atmospheric correction is a premise and necessary procedure for its application. In this paper, a method based on dark pixel for water-leaving radiance retrieving is proposed. Beside the Rayleigh scattering, the aerosol scattering is important to atmospheric correction, the water quality of inland lakes always are case II water and the value of water leaving radiance is not zero. So the synchronous MODIS shortwave infrared data was used to obtain the aerosol parameters, and in virtue of the characteristic that aerosol scattering is relative stabilized in 560 nm, the water-leaving radiance for each visible and near infrared band were retrieved and normalized, accordingly the remotely sensed reflectance of water was computed. The results show that the atmospheric correction method based on the imagery itself is more effective for the retrieval of water parameters for HJ-1A <span class="hlt">CCD</span> data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/266729','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/266729"><span>A simple, low-cost, versatile <span class="hlt">CCD</span> spectrometer for plasma 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>Den Hartog, D. J.; Holly, D. J.</p> <p>1996-06-01</p> <p>The authors have constructed a simple, low-cost <span class="hlt">CCD</span> spectrometer capable of both <span class="hlt">high</span> resolution ({Delta}{lambda} {le} 0.015 nm) and large bandpass (110 nm with {Delta}{lambda} {approximately}0.3 nm). These two modes of operation provide two broad areas of capability for plasma spectroscopy. The first major application is measurement of emission line broadening; the second is emission line surveys from the ultraviolet to the near infrared. Measurements have been made on a low-temperature plasma produced by a miniature electrostatic plasma source and the <span class="hlt">high</span>-temperature plasma in the MST Reversed-Field Pinch. The spectrometer is a modified Jarrell-Ash 0.5 m Ebert-Fastie monochromator. Light ismore » coupled into the entrance slit with a fused silica fiber optic bundle. The exposure time (2 ms minimum) is controlled by a fast electromechanical shutter. The exit plane detector is a compact and robust <span class="hlt">CCD</span> detector developed for amateur astronomy by Santa Barbara Instrument Group. The <span class="hlt">CCD</span> detector is controlled and read out by a Macintosh{reg_sign} computer. This spectrometer is sophisticated enough to serve well in a research laboratory, yet is simple and inexpensive enough to be affordable for instructional use.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001SPIE.4540..309M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001SPIE.4540..309M"><span>Quadrilinear <span class="hlt">CCD</span> sensors for the multispectral channel of spaceborne imagers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Materne, Alex; Gili, Bruno; Laubier, David; Gimenez, Thierry</p> <p>2001-12-01</p> <p>The PLEIADES-HR Earth Observation satellites will combine a <span class="hlt">high</span> resolution panchromatic channel -- 0.7 m at nadir -- and a multispectral channel allowing a 2.8 m resolution. This paper presents the main specifications, design and performances of a 52 microns pitch quadrilinear <span class="hlt">CCD</span> sensor developed by ATMEL under CNES contract, for the multispectral channel of the PLEIADES-HR instrument. The monolithic <span class="hlt">CCD</span> device includes four lines of 1500 pixels, each line dedicated to a narrow spectral band within blue to near infra red spectrum. The design of the photodiodes and <span class="hlt">CCD</span> registers, with larger size than those developed up to now for CNES spaceborne imagers, needed some specific structures to break the large equipotential areas where charge do not flow properly. Results are presented on the options which were experimented to improve sensitivity, maintain transfer efficiency and reduce power dissipation. The four spectral bands are achieved by four stripe filters made by SAGEM-REOSC PRODUCTS on a glass substrate, to be assembled on the sensor window. Line to line spacing on the silicon die takes into account the results of straylight analysis. A mineral layer, with <span class="hlt">high</span> optical absorption performances is deposited between photosensitive lines to further reduce straylight.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9356E..0DD','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9356E..0DD"><span>Laser beam welding of new <span class="hlt">ultra-high</span> strength and supra-ductile steels</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dahmen, Martin</p> <p>2015-03-01</p> <p><span class="hlt">Ultra-high</span> strength and supra-ductile are entering fields of new applications. Those materials are excellent candidates for modern light-weight construction and functional integration. As <span class="hlt">ultra-high</span> strength steels the stainless martensitic grade 1.4034 and the bainitic steel UNS 53835 are investigated. For the supra-ductile steels stand two <span class="hlt">high</span> austenitic steels with 18 and 28 % manganese. As there are no processing windows an approach from the metallurgical base on is required. Adjusting the weld microstructure the Q+P and the QT steels require weld heat treatment. The HSD steel is weldable without. Due to their applications the <span class="hlt">ultra-high</span> strength steels are welded in as-rolled and strengthened condition. Also the reaction of the weld on hot stamping is reflected for the martensitic grades. The supra-ductile steels are welded as solution annealed and work hardened by 50%. The results show the general suitability for laser beam welding.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014MeScT..25f5207L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014MeScT..25f5207L"><span><span class="hlt">CCD</span> image sensor induced error in PIV applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Legrand, M.; Nogueira, J.; Vargas, A. A.; Ventas, R.; Rodríguez-Hidalgo, M. C.</p> <p>2014-06-01</p> <p>The readout procedure of charge-coupled device (<span class="hlt">CCD</span>) cameras is known to generate some image degradation in different scientific imaging fields, especially in astrophysics. In the particular field of particle image velocimetry (PIV), widely extended in the scientific community, the readout procedure of the interline <span class="hlt">CCD</span> sensor induces a bias in the registered position of particle images. This work proposes simple procedures to predict the magnitude of the associated measurement error. Generally, there are differences in the position bias for the different images of a certain particle at each PIV frame. This leads to a substantial bias error in the PIV velocity measurement (˜0.1 pixels). This is the order of magnitude that other typical PIV errors such as peak-locking may reach. Based on modern <span class="hlt">CCD</span> technology and architecture, this work offers a description of the readout phenomenon and proposes a modeling for the <span class="hlt">CCD</span> readout bias error magnitude. This bias, in turn, generates a velocity measurement bias error when there is an illumination difference between two successive PIV exposures. The model predictions match the experiments performed with two 12-bit-depth interline <span class="hlt">CCD</span> cameras (MegaPlus ES 4.0/E incorporating the Kodak KAI-4000M <span class="hlt">CCD</span> sensor with 4 megapixels). For different cameras, only two constant values are needed to fit the proposed calibration model and predict the error from the readout procedure. Tests by different researchers using different cameras would allow verification of the model, that can be used to optimize acquisition setups. Simple procedures to obtain these two calibration values are also described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013Nanos...5.4119W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013Nanos...5.4119W"><span>Manganese oxide micro-supercapacitors with <span class="hlt">ultra-high</span> areal capacitance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Xu; Myers, Benjamin D.; Yan, Jian; Shekhawat, Gajendra; Dravid, Vinayak; Lee, Pooi See</p> <p>2013-05-01</p> <p>A symmetric micro-supercapacitor is constructed by electrochemically depositing manganese oxide onto micro-patterned current collectors. <span class="hlt">High</span> surface-to-volume ratio of manganese oxide and short diffusion distance between electrodes give an <span class="hlt">ultra-high</span> areal capacitance of 56.3 mF cm-2 at a current density of 27.2 μA cm-2.A symmetric micro-supercapacitor is constructed by electrochemically depositing manganese oxide onto micro-patterned current collectors. <span class="hlt">High</span> surface-to-volume ratio of manganese oxide and short diffusion distance between electrodes give an <span class="hlt">ultra-high</span> areal capacitance of 56.3 mF cm-2 at a current density of 27.2 μA cm-2. Electronic supplementary information (ESI) available: Experimental procedures; optical images of micro-supercapacitors; areal capacitances of samples M-0.3C, M-0.6C and M-0.9C; illustration of interdigital finger electrodes; Nyquist plot of Co(OH)2 deposited on micro-electrodes. See DOI: 10.1039/c3nr00210a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080012382','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080012382"><span><span class="hlt">CCD</span> imaging sensors</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Janesick, James R. (Inventor); Elliott, Stythe T. (Inventor)</p> <p>1989-01-01</p> <p>A method for promoting quantum efficiency (QE) of a <span class="hlt">CCD</span> imaging sensor for UV, far UV and low energy x-ray wavelengths by overthinning the back side beyond the interface between the substrate and the photosensitive semiconductor material, and flooding the back side with UV prior to using the sensor for imaging. This UV flooding promotes an accumulation layer of positive states in the oxide film over the thinned sensor to greatly increase QE for either frontside or backside illumination. A permanent or semipermanent image (analog information) may be stored in a frontside SiO.sub.2 layer over the photosensitive semiconductor material using implanted ions for a permanent storage and intense photon radiation for a semipermanent storage. To read out this stored information, the gate potential of the <span class="hlt">CCD</span> is biased more negative than that used for normal imaging, and excess charge current thus produced through the oxide is integrated in the pixel wells for subsequent readout by charge transfer from well to well in the usual manner.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27331147','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27331147"><span><span class="hlt">Ultra</span>-wide-field imaging in diabetic retinopathy; an overview.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ghasemi Falavarjani, Khalil; Wang, Kang; Khadamy, Joobin; Sadda, Srinivas R</p> <p>2016-06-01</p> <p>To present an overview on <span class="hlt">ultra</span>-wide-field imaging in diabetic retinopathy. A comprehensive search of the pubmed database was performed using the search terms of "<span class="hlt">ultra</span>-wide-field imaging", "<span class="hlt">ultra</span>-wide-field fluorescein angiography" and "diabetic retinopathy". The relevant original articles were reviewed. New advances in <span class="hlt">ultra</span>-wide-field imaging allow for <span class="hlt">precise</span> measurements of the peripheral retinal lesions. A consistent finding amongst these articles was that <span class="hlt">ultra</span>-wide-field imaging improved detection of peripheral lesion. There was discordance among the studies, however, on the correlation between peripheral diabetic lesions and diabetic macular edema. Visualization of the peripheral retina using <span class="hlt">ultra</span>-wide-field imaging improves diagnosis and classification of diabetic retinopathy. Additional studies are needed to better define the association of peripheral diabetic lesions with diabetic macular edema.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900005584','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900005584"><span><span class="hlt">CCD</span> TV focal plane guider development and comparison to SIRTF applications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rank, David M.</p> <p>1989-01-01</p> <p>It is expected that the SIRTF payload will use a <span class="hlt">CCD</span> TV focal plane fine guidance sensor to provide acquisition of sources and tracking stability of the telescope. Work has been done to develop <span class="hlt">CCD</span> TV cameras and guiders at Lick Observatory for several years and have produced state of the art <span class="hlt">CCD</span> TV systems for internal use. NASA decided to provide additional support so that the limits of this technology could be established and a comparison between SIRTF requirements and practical systems could be put on a more quantitative basis. The results of work carried out at Lick Observatory which was designed to characterize present <span class="hlt">CCD</span> autoguiding technology and relate it to SIRTF applications is presented. Two different design types of <span class="hlt">CCD</span> cameras were constructed using virtual phase and burred channel <span class="hlt">CCD</span> sensors. A simple autoguider was built and used on the KAO, Mt. Lemon and Mt. Hamilton telescopes. A video image processing system was also constructed in order to characterize the performance of the auto guider and <span class="hlt">CCD</span> cameras.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/205425-new-type-steel-plate-ultra-high-crack-arrestability','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/205425-new-type-steel-plate-ultra-high-crack-arrestability"><span>New-type steel plate with <span class="hlt">ultra</span> <span class="hlt">high</span> crack-arrestability</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>Ishikawa, T.; Nomiyama, Y.; Hagiwara, Y.</p> <p>1995-12-31</p> <p>A new-type steel plate has been developed by controlling the microstructure of the surface layers. The surface layer consists of <span class="hlt">ultra</span> fine grain ferrite microstructure, which provides excellent fracture toughness even at cryogenic temperature. When an unstable brittle crack propagates in the developed steel plate, shear-lips can be easily formed due to the surface layers with <span class="hlt">ultra</span> fine grain microstructure. Since unstable running crack behavior is strongly affected by side-ligaments (shear-lips), which are associated with extensive plastic deformation, enhanced formation of the shear-lips can improve crack arrestability. This paper describes the developed steel plates of HT500MPa tensile strength class formore » shipbuilding use. Fracture mechanics investigations using large-scale fracture testings (including ultrawide duplex ESSO tests) clarified that the developed steel plates have <span class="hlt">ultra</span> <span class="hlt">high</span> crack-arrestability. It was also confirmed that the plates possess sufficient properties, including weldability and workability, for ship building use.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997Sonne..21..141B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997Sonne..21..141B"><span>Sonnenaufnahmen mit einer Starlight X-Press <span class="hlt">CCD</span>-Kamera.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bernhard, K.</p> <p>1997-03-01</p> <p>To take-up the sun, most amateurastronomers use the photographic method. In this article the author shows, that <span class="hlt">CCD</span> is also a suitable method to do this. Especially the possibilities to see immediately the result of focusing on the screen and the electronic processing are very useful to get sharp and <span class="hlt">high</span>-contrast images of the sun.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/25282','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/25282"><span>Application of <span class="hlt">ultra-high</span> performance concrete to bridge girders.</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2009-02-01</p> <p>"<span class="hlt">Ultra-High</span> Performance Concrete (UHPC) is a new class of concrete that has superior performance characteristics : compared to conventional concrete. The enhanced strength and durability properties of UHPC are mainly due to optimized : particle grada...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23635215','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23635215"><span><span class="hlt">Precise</span> measurement of a magnetic field generated by the electromagnetic flux compression technique.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nakamura, D; Sawabe, H; Matsuda, Y H; Takeyama, S</p> <p>2013-04-01</p> <p>The <span class="hlt">precision</span> of the values of a magnetic field generated by electromagnetic flux compression was investigated in <span class="hlt">ultra-high</span> magnetic fields of up to 700 T. In an attempt to calibrate the magnetic field measured by pickup coils, <span class="hlt">precise</span> Faraday rotation (FR) measurements were conducted on optical (quartz and crown) glasses. A discernible "turn-around" phenomenon was observed in the FR signal as well as the pickup coils before the end of a liner implosion. We found that the magnetic field measured by pickup coils should be corrected by taking into account the <span class="hlt">high</span>-frequency response of the signal transmission line. Near the peak magnetic field, however, the pickup coils failed to provide reliable values, leaving the FR measurement as the only method to <span class="hlt">precisely</span> measure extremely <span class="hlt">high</span> magnetic fields.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1955b0025P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1955b0025P"><span>Study on creep of fiber reinforced <span class="hlt">ultra-high</span> strength concrete based on strength</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peng, Wenjun; Wang, Tao</p> <p>2018-04-01</p> <p>To complement the creep performance of <span class="hlt">ultra-high</span> strength concrete, the long creep process of fiber reinforced concrete was studied in this paper. The long-term creep process and regularity of <span class="hlt">ultra-high</span> strength concrete with 0.5% PVA fiber under the same axial compression were analyzed by using concrete strength (C80/C100/C120) as a variable. The results show that the creep coefficient of <span class="hlt">ultra-high</span> strength concrete decreases with the increase of concrete strength. Compared with ACI209R (92), GL2000 models, it is found that the predicted value of ACI209R (92) are close to the experimental value, and the creep prediction model suitable for this experiment is proposed based on ACI209R (92).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApPhL.111j3502F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhL.111j3502F"><span><span class="hlt">Ultra</span>-broadband and planar sound diffuser with <span class="hlt">high</span> uniformity of reflected intensity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fan, Xu-Dong; Zhu, Yi-Fan; Liang, Bin; Yang, Jing; Yang, Jun; Cheng, Jian-Chun</p> <p>2017-09-01</p> <p>Schroeder diffusers, as a classical design of acoustic diffusers proposed over 40 years ago, play key roles in many practical scenarios ranging from architectural acoustics to noise control to particle manipulation. Despite the great success of conventional acoustic diffusers, it is still worth pursuing ideal acoustic diffusers that are essentially expected to produce perfect sound diffuse reflection within the unlimited bandwidth. Here, we propose a different mechanism for designing acoustic diffusers to overcome the basic limits in intensity uniformity and working bandwidth in the previous designs and demonstrate a practical implementation by acoustic metamaterials with dispersionless phase-steering capability. In stark contrast to the existing production of diffuse fields relying on random scattering of sound energy by using a specific mathematical number sequence of periodically distributed unit cells, we directly mold the reflected wavefront into the desired shape by <span class="hlt">precisely</span> manipulating the local phases of individual subwavelength metastructures. We also benchmark our design via numerical simulation with a commercially available Schroeder diffuser, and the results verify that our proposed diffuser scatters incident acoustic energy into all directions more uniformly within an <span class="hlt">ultra</span>-broad band regardless of the incident angle. Furthermore, our design enables further improvement of the working bandwidth just by simply downscaling each individual element. With <span class="hlt">ultra</span>-broadband functionality and <span class="hlt">high</span> uniformity of reflected intensity, our metamaterial-based production of the diffusive field opens a route to the design and application of acoustic diffusers and may have a significant impact on various fields such as architectural acoustics and medical ultrasound imaging/treatment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.osti.gov/sciencecinema/biblio/987385','SCIGOVIMAGE-SCICINEMA'); return false;" href="http://www.osti.gov/sciencecinema/biblio/987385"><span><span class="hlt">Precision</span> Crystal Calorimeters in <span class="hlt">High</span> Energy Physics</span></a></p> <p><a target="_blank" href="http://www.osti.gov/sciencecinema/">ScienceCinema</a></p> <p>Ren-Yuan Zhu</p> <p>2017-12-09</p> <p><span class="hlt">Precision</span> crystal calorimeters traditionally play an important role in <span class="hlt">high</span> energy physics experiments. In the last two decades, it faces a challenge to maintain its <span class="hlt">precision</span> in a hostile radiation environment. This paper reviews the performance of crystal calorimeters constructed for <span class="hlt">high</span> energy physics experiments and the progress achieved in understanding crystal’s radiation damage as well as in developing <span class="hlt">high</span> quality scintillating crystals for particle physics. Potential applications of new generation scintillating crystals of <span class="hlt">high</span> density and <span class="hlt">high</span> light yield, such as LSO and LYSO, in particle physics experiments is also 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('http://www.dtic.mil/docs/citations/ADA601902','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA601902"><span>Field Evaluation of <span class="hlt">Ultra-High</span> Pressure Water Systems for Runway Rubber Removal</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2014-04-01</p> <p>ER D C/ G SL T R- 14 -1 1 Field Evaluation of <span class="hlt">Ultra-High</span> Pressure Water Systems for Runway Rubber Removal G eo te ch ni ca l a nd S tr...Field Evaluation of <span class="hlt">Ultra-High</span> Pressure Water Systems for Runway Rubber Removal Aaron B. Pullen Applied Research Associates, Inc. 421 Oak Avenue...collaboration with Applied Research Associates, Inc. (ARA). Several types of commercial UHPW water blasting systems were tested on an ungrooved portland cement</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008JPhCS.114a2061P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008JPhCS.114a2061P"><span><span class="hlt">Ultra</span> <span class="hlt">high</span> vacuum test setup for electron gun</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pandiyar, M. L.; Prasad, M.; Jain, S. K.; Kumar, R.; Hannurkar, P. R.</p> <p>2008-05-01</p> <p><span class="hlt">Ultra</span> <span class="hlt">High</span> Vacuum (UHV) test setup for electron gun testing has been developed. The development of next generation light sources and accelerators require development of klystron as a radio frequency power source, and in turn electron gun. This UHV electron gun test setup can be used to test the electron guns ranging from <span class="hlt">high</span> average current, quasi-continuous wave to <span class="hlt">high</span> peak current, single pulse etc. An electron gun has been designed, fabricated, assembled and tested for insulation up to 80 kV under the programme to develop <span class="hlt">high</span> power klystron for future accelerators. Further testing includes the electron emission parameters characterization of the cathode, as it determines the development of a reliable and efficient electron gun with <span class="hlt">high</span> electron emission current and <span class="hlt">high</span> life time as well. This needs a clean <span class="hlt">ultra</span> <span class="hlt">high</span> vacuum to study these parameters particularly at <span class="hlt">high</span> emission current. The cathode emission current, work function and vapour pressure of cathode surface material at <span class="hlt">high</span> temperature studies will further help in design and development of <span class="hlt">high</span> power electron gun The UHV electron gun test setup consists of Turbo Molecular Pump (TMP), Sputter Ion Pump (SIP), pressure gauge, <span class="hlt">high</span> voltage and cathode power supplies, current measurement device, solenoid magnet and its power supply, residual gas analyser etc. The ultimate vacuum less than 2×10-9 mbar was achieved. This paper describes the UHV test setup for electron gun testing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/28118','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/28118"><span>Bond behavior of reinforcing steel in <span class="hlt">ultra-high</span> performance concrete.</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2014-10-01</p> <p><span class="hlt">Ultra-High</span> Performance Concrete (UHPC) is a relatively new class of advanced cementitious composite : materials, which exhibits <span class="hlt">high</span> compressive [above 21.7 ksi (150 MPa)] and tensile [above 0.72 ksi (5 MPa)] : strengths. The discrete steel fiber rei...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MeScT..28k5401H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MeScT..28k5401H"><span><span class="hlt">High</span>-speed imaging using 3<span class="hlt">CCD</span> camera and multi-color LED flashes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hijazi, Ala; Friedl, Alexander; Cierpka, Christian; Kähler, Christian; Madhavan, Vis</p> <p>2017-11-01</p> <p>This paper demonstrates the possibility of capturing full-resolution, <span class="hlt">high</span>-speed image sequences using a regular 3<span class="hlt">CCD</span> color camera in conjunction with <span class="hlt">high</span>-power light emitting diodes of three different colors. This is achieved using a novel approach, referred to as spectral-shuttering, where a <span class="hlt">high</span>-speed image sequence is captured using short duration light pulses of different colors that are sent consecutively in very close succession. The work presented in this paper demonstrates the feasibility of configuring a <span class="hlt">high</span>-speed camera system using low cost and readily available off-the-shelf components. This camera can be used for recording six-frame sequences at frame rates up to 20 kHz or three-frame sequences at even higher frame rates. Both color crosstalk and spatial matching between the different channels of the camera are found to be within acceptable limits. A small amount of magnification difference between the different channels is found and a simple calibration procedure for correcting the images is introduced. The images captured using the approach described here are of good quality to be used for obtaining full-field quantitative information using techniques such as digital image correlation and particle image velocimetry. A sequence of six <span class="hlt">high</span>-speed images of a bubble splash recorded at 400 Hz is presented as a demonstration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007SPIE.6673E..0RD','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007SPIE.6673E..0RD"><span><span class="hlt">High-precision</span> thermal expansion measurements using small Fabry-Perot etalons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Davis, Mark J.; Hayden, Joseph S.; Farber, Daniel L.</p> <p>2007-09-01</p> <p>Coefficient of thermal expansion (CTE) measurements using small Fabry-Perot etalons were conducted on <span class="hlt">high</span> and low thermal expansion materials differing in CTE by a factor of nearly 400. The smallest detectable change in length was ~10 -12 m. The sample consisted of a mm-sized Fabry-Perot etalon equipped with spherical mirrors; the material-under-test served as the 2.5 mm-thick spacer between the mirrors. A heterodyne optical setup was used with one laser locked to an ~780 nm hyperfine line of Rb gas and the other locked to a resonance of the sample etalon; changes in the beat frequency between the two lasers as a function of temperature directly provided a CTE value. The measurement system was tested using the <span class="hlt">high</span>-CTE SCHOTT optical glass N-KF9 (CTE = 9.5 ppm/K at 23 °C). Measurements conducted under reproducibility conditions using five identically-prepared N-KF9 etalons demonstrate a <span class="hlt">precision</span> of 0.1 ppm/K; absolute values (accuracy) are within 2-sigma errors with those made using mechanical dilatometers with 100-mm long sample rods. Etalon-based CTE measurements were also made on a <span class="hlt">high</span>-CTE (~10.5 ppm/K), proprietary glass-ceramic used for <span class="hlt">high</span> peak-pressure electrical feedthroughs and revealed statistically significant differences among parts made under what were assumed to be identical conditions. Finally, CTE measurements were made on etalons constructed from SCHOTT's <span class="hlt">ultra</span>-low CTE Zerodur (R) glass-ceramic (CTE about -20 ppb/K at 50 °C for the material tested herein).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1130233-precision-control-multiple-quantum-cascade-lasers-calibration-systems','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1130233-precision-control-multiple-quantum-cascade-lasers-calibration-systems"><span><span class="hlt">Precision</span> Control of Multiple Quantum Cascade Lasers for Calibration 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>Taubman, Matthew S.; Myers, Tanya L.; Pratt, Richard M.</p> <p></p> <p>We present a <span class="hlt">precision</span>, digitally interfaced current controller for quantum cascade lasers, with demonstrated DC and modulated temperature coefficients of 1- 2 ppm/ºC and 15 ppm/ºC respectively. <span class="hlt">High</span> linearity digital to analog converters (DACs) together with an <span class="hlt">ultra-precision</span> voltage reference, produce <span class="hlt">highly</span> stable, <span class="hlt">precision</span> voltages. These are in turn selected by a low charge-injection multiplexer (MUX) chip, which are then used to set output currents via a linear current regulator. The controller is operated in conjunction with a power multiplexing unit, allowing one of three lasers to be driven by the controller while ensuring protection of controller and all lasersmore » during operation, standby and switching. Simple ASCII commands sent over a USB connection to a microprocessor located in the current controller operate both the controller (via the DACs and MUX chip) and the power multiplexer.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19770008348','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19770008348"><span>Solid state television camera (<span class="hlt">CCD</span>-buried channel)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1976-01-01</p> <p>The development of an all solid state television camera, which uses a buried channel charge coupled device (<span class="hlt">CCD</span>) as the image sensor, was undertaken. A 380 x 488 element <span class="hlt">CCD</span> array is utilized to ensure compatibility with 525 line transmission and display monitor equipment. Specific camera design approaches selected for study and analysis included (a) optional clocking modes for either fast (1/60 second) or normal (1/30 second) frame readout, (b) techniques for the elimination or suppression of <span class="hlt">CCD</span> blemish effects, and (c) automatic light control and video gain control (i.e., ALC and AGC) techniques to eliminate or minimize sensor overload due to bright objects in the scene. Preferred approaches were determined and integrated into a deliverable solid state TV camera which addressed the program requirements for a prototype qualifiable to space environment conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005SPIE10315E..0OM','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005SPIE10315E..0OM"><span>The ultrahigh <span class="hlt">precision</span> form measurement of small, steep-sided aspheric moulds, incorporating novel hardware and software developments; Technical Digest</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mills, M. W.; Hutchinson, Matthew J.</p> <p>2005-05-01</p> <p>A variety of consumer applications, eg cellphone camera lenses, optical storage devices, digital cameras, etc, are driving the demand for small, <span class="hlt">high</span> aspheric departure rotationally-symmetric moulded optics, manufactured both in polymer and glass materials. The mould tools for such components are manufactured by <span class="hlt">ultra-high</span> <span class="hlt">precision</span> techniques such as single point diamond turning and <span class="hlt">ultra-precision</span> grinding, and must be accurate to <1/10μm levels for form, and exhibit nanometric surface finish quality. The aspheric forms of such components' optical surfaces exhibit <span class="hlt">high</span> departure from best-fit sphere towards their outer edge, which renders this outer region especially critical for optical performance. The <span class="hlt">high</span> slope of these components at the clear aperture has caused some restrictions on the use of profilometry in the measurement of form across their full diameter. Taylor Hobson designs and manufactures a range of <span class="hlt">ultra-precision</span> profilometers for use in such industries as aspheric optics fabrication. In order to address the issues described, a new measurement system, Taylor Hobson Form Talysurf PGI 1250, has been developed, which contains new Aspheric Data Fusion Software, as well as Asphero-Diffractive Analysis Software, allowing the entire diametric profile to be analysed to the desired level of accuracy. This development removes the previous limitation of maximum slope for this type of measurement, thus enabling better quality control of <span class="hlt">high</span> slope, <span class="hlt">high</span> aspheric departure optics. Measurement data from the Form Talysurf PGI 1250 can be fed back directly to the machine tool, in order to optimize the form of the optical mould.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005SPIE.TD03...82M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005SPIE.TD03...82M"><span>The ultrahigh <span class="hlt">precision</span> form measurement of small, steep-sided aspheric moulds, incorporating novel hardware and software developments; Technical Digest</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mills, M. W.; Hutchinson, Matthew J.</p> <p>2005-05-01</p> <p>A variety of consumer applications, eg cellphone camera lenses, optical storage devices, digital cameras, etc, are driving the demand for small, <span class="hlt">high</span> aspheric departure rotationally-symmetric moulded optics, manufactured both in polymer and glass materials. The mould tools for such components are manufactured by <span class="hlt">ultra-high</span> <span class="hlt">precision</span> techniques such as single point diamond turning and <span class="hlt">ultra-precision</span> grinding, and must be accurate to <1/10μm levels for form, and exhibit nanometric surface finish quality. The aspheric forms of such components" optical surfaces exhibit <span class="hlt">high</span> departure from best-fit sphere towards their outer edge, which renders this outer region especially critical for optical performance. The <span class="hlt">high</span> slope of these components at the clear aperture has caused some restrictions on the use of profilometry in the measurement of form across their full diameter. Taylor Hobson designs and manufactures a range of <span class="hlt">ultra-precision</span> profilometers for use in such industries as aspheric optics fabrication. In order to address the issues described, a new measurement system, Taylor Hobson Form Talysurf PGI 1250, has been developed, which contains new Aspheric Data Fusion Software, as well as Asphero-Diffractive Analysis Software, allowing the entire diametric profile to be analysed to the desired level of accuracy. This development removes the previous limitation of maximum slope for this type of measurement, thus enabling better quality control of <span class="hlt">high</span> slope, <span class="hlt">high</span> aspheric departure optics. Measurement data from the Form Talysurf PGI 1250 can be fed back directly to the machine tool, in order to optimize the form of the optical mould.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.S13C2028M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.S13C2028M"><span>Concordia <span class="hlt">CCD</span> - A Geoscope station in continental Antarctica</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Maggi, A.; Lévêque, J.; Thoré, J.; Bes de Berc, M.; Bernard, A.; Danesi, S.; Morelli, A.; Delladio, A.; Sorrentino, D.; Stutzmann, E.; Geoscope Team</p> <p>2010-12-01</p> <p>Concordia (Dome C, Antarctica) has had a permanent seismic station since 2005. It is run by EOST and INGV in collaboration with the French and Italian polar institutes (IPEV and PNRA). It is installed in an ice-vault, at 12m depth, distant 1km from the permanent scientific base at Concordia. The temperature in the vault is a constant -55°C. The data quality at the station has improved continuously since its installation. In 2007, the station was declared at ISC as an open station with station code <span class="hlt">CCD</span> (ConCorDia), with data available upon request. It is only the second permanent station in the Antarctic continent, after South Pole. In 2010, <span class="hlt">CCD</span> was included in the Geoscope network. Data from <span class="hlt">CCD</span> starting in 2007 are now freely available from the Geoscope Data Center and IRIS. We present an analysis of the data quality at <span class="hlt">CCD</span>, and describe the technical difficulties of operating an observatory-quality seismic station in the extreme environmental conditons present in continental Antarctica.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5872998','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5872998"><span>Laser Induced Damage of Potassium Dihydrogen Phosphate (KDP) Optical Crystal Machined by Water Dissolution <span class="hlt">Ultra-Precision</span> Polishing Method</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gao, Hang; Wang, Xu; Guo, Dongming; Liu, Ziyuan</p> <p>2018-01-01</p> <p>Laser induced damage threshold (LIDT) is an important optical indicator for nonlinear Potassium Dihydrogen Phosphate (KDP) crystal used in <span class="hlt">high</span> power laser systems. In this study, KDP optical crystals are initially machined with single point diamond turning (SPDT), followed by water dissolution <span class="hlt">ultra-precision</span> polishing (WDUP) and then tested with 355 nm nanosecond pulsed-lasers. Power spectral density (PSD) analysis shows that WDUP process eliminates the laser-detrimental spatial frequencies band of micro-waviness on SPDT machined surface and consequently decreases its modulation effect on the laser beams. The laser test results show that LIDT of WDUP machined crystal improves and its stability has a significant increase by 72.1% compared with that of SPDT. Moreover, a subsequent ultrasonic assisted solvent cleaning process is suggested to have a positive effect on the laser performance of machined KDP crystal. Damage crater investigation indicates that the damage morphologies exhibit <span class="hlt">highly</span> thermal explosion features of melted cores and brittle fractures of periphery material, which can be described with the classic thermal explosion model. The comparison result demonstrates that damage mechanisms for SPDT and WDUP machined crystal are the same and WDUP process reveals the real bulk laser resistance of KDP optical crystal by removing the micro-waviness and subsurface damage on SPDT machined surface. This improvement of WDUP method makes the LIDT more accurate and will be beneficial to the laser performance of KDP crystal. PMID:29534032</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NaPho..12..324L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NaPho..12..324L"><span>Vacuum Bloch-Siegert shift in Landau polaritons with <span class="hlt">ultra-high</span> cooperativity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Xinwei; Bamba, Motoaki; Zhang, Qi; Fallahi, Saeed; Gardner, Geoff C.; Gao, Weilu; Lou, Minhan; Yoshioka, Katsumasa; Manfra, Michael J.; Kono, Junichiro</p> <p>2018-06-01</p> <p>A two-level system resonantly interacting with an a.c. magnetic or electric field constitutes the physical basis of diverse phenomena and technologies. However, Schrödinger's equation for this seemingly simple system can be solved exactly only under the rotating-wave approximation, which neglects the counter-rotating field component. When the a.c. field is sufficiently strong, this approximation fails, leading to a resonance-frequency shift known as the Bloch-Siegert shift. Here, we report the vacuum Bloch-Siegert shift, which is induced by the <span class="hlt">ultra</span>-strong coupling of matter with the counter-rotating component of the vacuum fluctuation field in a cavity. Specifically, an <span class="hlt">ultra-high</span>-mobility two-dimensional electron gas inside a <span class="hlt">high</span>-Q terahertz cavity in a quantizing magnetic field revealed <span class="hlt">ultra</span>-narrow Landau polaritons, which exhibited a vacuum Bloch-Siegert shift up to 40 GHz. This shift, clearly distinguishable from the photon-field self-interaction effect, represents a unique manifestation of a strong-field phenomenon without a strong field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/863953','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/863953"><span><span class="hlt">Ultra</span> <span class="hlt">high</span> vacuum seal arrangement</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Flaherty, Robert</p> <p>1981-01-01</p> <p>Arrangement for demountably sealing two concentric metallic tubes in an <span class="hlt">ultra</span> <span class="hlt">high</span> vacuum system which facilitates remote actuation. A tubular seal includes integral spaced lips which circumferentially engage the metallic tubes. The lips plastically deform the metallic tubes by mechanical forces resulting from a martensite to austenite transformation of the tubular seal upon application of a predetermined temperature. The sealing force is released upon application of another temperature which causes a transformation from the stronger austenite to the weaker martensite. Use of a dual acting sealing ring and driving ring circumferentially contacting the sealing ring is particularly applicable to sealing larger diameter concentric metallic members.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10448E..21H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10448E..21H"><span><span class="hlt">Precision</span> lens assembly with alignment turning system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ho, Cheng-Fang; Huang, Chien-Yao; Lin, Yi-Hao; Kuo, Hui-Jean; Kuo, Ching-Hsiang; Hsu, Wei-Yao; Chen, Fong-Zhi</p> <p>2017-10-01</p> <p>The poker chip assembly with <span class="hlt">high</span> <span class="hlt">precision</span> lens barrels is widely applied to <span class="hlt">ultra-high</span> performance optical system. ITRC applies the poker chip assembly technology to the <span class="hlt">high</span> numerical aperture objective lenses and lithography projection lenses because of its <span class="hlt">high</span> efficiency assembly process. In order to achieve <span class="hlt">high</span> <span class="hlt">precision</span> lens cell for poker chip assembly, an alignment turning system (ATS) is developed. The ATS includes measurement, alignment and turning modules. The measurement module is equipped with a non-contact displacement sensor (NCDS) and an autocollimator (ACM). The NCDS and ACM are used to measure centration errors of the top and the bottom surface of a lens respectively; then the amount of adjustment of displacement and tilt with respect to the rotational axis of the turning machine for the alignment module can be determined. After measurement, alignment and turning processes on the ATS, the centration error of a lens cell with 200 mm in diameter can be controlled within 10 arcsec. Furthermore, a poker chip assembly lens cell with three sub-cells is demonstrated, each sub-cells are measured and accomplished with alignment and turning processes. The lens assembly test for five times by each three technicians; the average transmission centration error of assembly lens is 12.45 arcsec. The results show that ATS can achieve <span class="hlt">high</span> assembly efficiency for <span class="hlt">precision</span> optical systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050215286','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050215286"><span>Design of <span class="hlt">Ultra-High</span>-Power-Density Machine Optimized for Future Aircraft</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Choi, Benjamin B.</p> <p>2004-01-01</p> <p>The NASA Glenn Research Center's Structural Mechanics and Dynamics Branch is developing a compact, nonpolluting, bearingless electric machine with electric power supplied by fuel cells for future "more-electric" aircraft with specific power in the projected range of 50 hp/lb, whereas conventional electric machines generate usually 0.2 hp/lb. The use of such electric drives for propulsive fans or propellers depends on the successful development of <span class="hlt">ultra-high</span>-power-density machines. One possible candidate for such <span class="hlt">ultra-high</span>-power-density machines, a round-rotor synchronous machine with an engineering current density as <span class="hlt">high</span> as 20,000 A/sq cm, was selected to investigate how much torque and power can be produced.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10562E..4KK','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10562E..4KK"><span>Early study on the application of Nexcera <span class="hlt">ultra</span> low thermal expansion ceramic to space telescopes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kamiya, Tomohiro; Sugawara, Jun; Mizutani, Tadahito; Yasuda, Susumu; Kitamoto, Kazuya</p> <p>2017-09-01</p> <p>Optical mirrors for space telescopes, which require <span class="hlt">high</span> <span class="hlt">precision</span> and <span class="hlt">high</span> thermal stability, have commonly been made of glass materials such as <span class="hlt">ultra</span> low expansion glass (e.g. ULE®) or extremely low expansion glassceramic (e.g. ZERODUR® or CLEARCERAM®). These materials have been well-known for their reliability due to their long history of achievements in many space applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA581191','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA581191"><span>Spatially-Resolved Characterization Techniques to Investigate Impact Damage in <span class="hlt">Ultra-High</span> Performance Concretes</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2013-04-01</p> <p>Concretes G eo te ch n ic al a n d S tr u ct u re s La b or at or y Robert D. Moser, Paul G. Allison, and Mei Q. Chandler April 2013 Approved...Impact Damage in <span class="hlt">Ultra-High</span> Performance Concretes Robert D. Moser, Paul G. Allison, and Mei Q. Chandler Geotechnical and Structures Laboratory US...Portland Cement concrete (OPC) and <span class="hlt">Ultra-High</span> Performance Concretes (UHPCs) under <span class="hlt">high</span>-strain impact and penetration loads at lower length scales</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006SPIE.6347E..0NK','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006SPIE.6347E..0NK"><span>New low noise <span class="hlt">CCD</span> cameras for Pi-of-the-Sky project</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kasprowicz, G.; Czyrkowski, H.; Dabrowski, R.; Dominik, W.; Mankiewicz, L.; Pozniak, K.; Romaniuk, R.; Sitek, P.; Sokolowski, M.; Sulej, R.; Uzycki, J.; Wrochna, G.</p> <p>2006-10-01</p> <p>Modern research trends require observation of fainter and fainter astronomical objects on large areas of the sky. This implies usage of systems with <span class="hlt">high</span> temporal and optical resolution with computer based data acquisition and processing. Therefore Charge Coupled Devices (<span class="hlt">CCD</span>) became so popular. They offer quick picture conversion with much better quality than film based technologies. This work is theoretical and practical study of the <span class="hlt">CCD</span> based picture acquisition system. The system was optimized for "Pi of The Sky" project. But it can be adapted to another professional astronomical researches. The work includes issue of picture conversion, signal acquisition, data transfer and mechanical construction of the device.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1082356','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1082356"><span><span class="hlt">Ultra-high</span> density diffraction grating</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Padmore, Howard A.; Voronov, Dmytro L.; Cambie, Rossana; Yashchuk, Valeriy V.; Gullikson, Eric M.</p> <p>2012-12-11</p> <p>A diffraction grating structure having <span class="hlt">ultra-high</span> density of grooves comprises an echellette substrate having periodically repeating recessed features, and a multi-layer stack of materials disposed on the echellette substrate. The surface of the diffraction grating is planarized, such that layers of the multi-layer stack form a plurality of lines disposed on the planarized surface of the structure in a periodical fashion, wherein lines having a first property alternate with lines having a dissimilar property on the surface of the substrate. For example, in one embodiment, lines comprising <span class="hlt">high</span>-Z and low-Z materials alternate on the planarized surface providing a structure that is suitable as a diffraction grating for EUV and soft X-rays. In some embodiments, line density of between about 10,000 lines/mm to about 100,000 lines/mm is provided.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999SPIE.3786..402G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999SPIE.3786..402G"><span>Adjustment of multi-<span class="hlt">CCD</span>-chip-color-camera heads</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guyenot, Volker; Tittelbach, Guenther; Palme, Martin</p> <p>1999-09-01</p> <p>The principle of beam-splitter-multi-chip cameras consists in splitting an image into differential multiple images of different spectral ranges and in distributing these onto separate black and white <span class="hlt">CCD</span>-sensors. The resulting electrical signals from the chips are recombined to produce a <span class="hlt">high</span> quality color picture on the monitor. Because this principle guarantees higher resolution and sensitivity in comparison to conventional single-chip camera heads, the greater effort is acceptable. Furthermore, multi-chip cameras obtain the compete spectral information for each individual object point while single-chip system must rely on interpolation. In a joint project, Fraunhofer IOF and STRACON GmbH and in future COBRA electronic GmbH develop methods for designing the optics and dichroitic mirror system of such prism color beam splitter devices. Additionally, techniques and equipment for the alignment and assembly of color beam splitter-multi-<span class="hlt">CCD</span>-devices on the basis of gluing with UV-curable adhesives have been developed, too.</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('https://www.ncbi.nlm.nih.gov/pubmed/29319915','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29319915"><span>Enantioselective <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid and supercritical fluid chromatography: The race to the shortest chromatogram.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ciogli, Alessia; Ismail, Omar H; Mazzoccanti, Giulia; Villani, Claudio; Gasparrini, Francesco</p> <p>2018-03-01</p> <p>The ever-increasing need for enantiomerically pure chiral compounds has greatly expanded the number of enantioselective separation methods available for the <span class="hlt">precise</span> and accurate measurements of the enantiomeric purity. The introduction of chiral stationary phases for liquid chromatography in the last decades has revolutionized the routine methods to determine enantiomeric purity of chiral drugs, agrochemicals, fragrances, and in general of organic and organometallic compounds. In recent years, additional efforts have been placed on faster, enantioselective analytical methods capable to fulfill the <span class="hlt">high</span> throughput requirements of modern screening procedures. Efforts in this field, capitalizing on improved chromatographic particle technology and dedicated instrumentation, have led to <span class="hlt">highly</span> efficient separations that are routinely completed on the seconds time scale. An overview of the recent achievements in the field of <span class="hlt">ultra-high</span>-resolution chromatography on column packed with chiral stationary phases, both based on sub-2 μm fully porous and sub-3 μm superficially porous particles, will be given, with an emphasis on very recent studies on ultrafast chiral separations. © 2018 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPS...383..102T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPS...383..102T"><span><span class="hlt">High</span>-energy green supercapacitor driven by ionic liquid electrolytes as an <span class="hlt">ultra-high</span> stable next-generation energy storage device</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thangavel, Ranjith; Kannan, Aravindaraj G.; Ponraj, Rubha; Thangavel, Vigneysh; Kim, Dong-Won; Lee, Yun-Sung</p> <p>2018-04-01</p> <p>Development of supercapacitors with <span class="hlt">high</span> energy density and long cycle life using sustainable materials for next-generation applications is of paramount importance. The ongoing challenge is to elevate the energy density of supercapacitors on par with batteries, while upholding the power and cyclability. In addition, attaining such superior performance with green and sustainable bio-mass derived compounds is very crucial to address the rising environmental concerns. Herein, we demonstrate the use of watermelon rind, a bio-waste from watermelons, towards <span class="hlt">high</span> energy, and <span class="hlt">ultra</span>-stable <span class="hlt">high</span> temperature green supercapacitors with a <span class="hlt">high</span>-voltage ionic liquid electrolyte. Supercapacitors assembled with <span class="hlt">ultra-high</span> surface area, hierarchically porous carbon exhibits a remarkable performance both at room temperature and at <span class="hlt">high</span> temperature (60 °C) with maximum energy densities of ∼174 Wh kg-1 (25 °C), and 177 Wh kg-1 (60 °C) - based on active mass of both electrodes. Furthermore, an <span class="hlt">ultra-high</span> specific power of ∼20 kW kg-1 along with an <span class="hlt">ultra</span>-stable cycling performance with 90% retention over 150,000 cycles has been achieved even at 60 °C, outperforming supercapacitors assembled with other carbon based materials. These results demonstrate the potential to develop <span class="hlt">high</span>-performing, green energy storage devices using eco-friendly materials for next generation electric vehicles and other advanced energy storage systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006SPIE.6031E..09G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006SPIE.6031E..09G"><span><span class="hlt">CCD</span> imaging system for the EUV solar telescope</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gong, Yan; Song, Qian; Ye, Bing-Xun</p> <p>2006-01-01</p> <p>In order to develop the detector adapted to the space solar telescope, we have built a <span class="hlt">CCD</span> camera system capable of working in the extra ultraviolet (EUV) band, which is composed of one phosphor screen, one intensified system using a photocathode/micro-channel plate(MCP)/ phosphor, one optical taper and one chip of front-illuminated (FI) <span class="hlt">CCD</span> without screen windows. All of them were stuck one by one with optical glue. The working principle of the camera system is presented; moreover we have employed the mesh experiment to calibrate and test the <span class="hlt">CCD</span> camera system in 15~24nm, the position resolution of about 19 μm is obtained at the wavelength of 17.1nm and 19.5nm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1026322','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1026322"><span>Link and Network Layers Design for <span class="hlt">Ultra-High</span>-Speed Terahertz-Band Communications Networks</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2017-01-01</p> <p>throughput, and identify the optimal parameter values for their design (Sec. 6.2.3). Moreover, we validate and test the scheme with experimental data obtained...LINK AND NETWORK LAYERS DESIGN FOR <span class="hlt">ULTRA-HIGH</span>- SPEED TERAHERTZ-BAND COMMUNICATIONS NETWORKS STATE UNIVERSITY OF NEW YORK (SUNY) AT BUFFALO JANUARY...TYPE FINAL TECHNICAL REPORT 3. DATES COVERED (From - To) FEB 2015 – SEP 2016 4. TITLE AND SUBTITLE LINK AND NETWORK LAYERS DESIGN FOR <span class="hlt">ULTRA-HIGH</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009SPIE.7439E..04L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009SPIE.7439E..04L"><span><span class="hlt">CCD</span> radiation damage in ESA Cosmic Visions missions: assessment and mitigation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lumb, David H.</p> <p>2009-08-01</p> <p>Charge Coupled Device (<span class="hlt">CCD</span>) imagers have been widely used in space-borne astronomical instruments. A frequent concern has been the radiation damage effects on the <span class="hlt">CCD</span> charge transfer properties. We review some methods for assessing the Charge Transfer Inefficiency (CTI) in CCDs. Techniques to minimise degradation using background charge injection and p-channel <span class="hlt">CCD</span> architectures are discussed. A critical review of the claims for p-channel architectures is presented. The performance advantage for p-channel <span class="hlt">CCD</span> performance is shown to be lower than claimed previously. Finally we present some projections for the performance in the context of some future ESA missions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JInst..12P4009S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JInst..12P4009S"><span>A new spectroscopic imager for X-rays from 0.5 keV to 150 keV combining a pn<span class="hlt">CCD</span> and a columnar CsI(Tl) scintillator</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schlosser, D. M.; Hartmann, R.; Kalok, D.; Bechteler, A.; Abboud, A.; Shokr, M.; Çonka, T.; Pietsch, U.; Strüder, L.</p> <p>2017-04-01</p> <p>By combining a low noise fully depleted pn<span class="hlt">CCD</span> detector with a columnar CsI(Tl) scintillator an energy dispersive spatial resolving detector can be realized with a <span class="hlt">high</span> quantum efficiency in the range from below 0.5 keV to above 150 keV. The used scintillator system increases the pulse height of gamma-rays converted in the CsI(Tl), due to focusing properties of the columnar scintillator structure by reducing the event size in indirect detection mode (conversion in the scintillator). In case of direct detection (conversion in the silicon of the pn<span class="hlt">CCD</span>) the relative energy resolution is 0.7% at 122 keV (FWHM = 850 eV) and the spatial resolution is less than 75 μm. In case of indirect detection the relative energy resolution, integrated over all event sizes is about 9% at 122 keV with an expected spatial <span class="hlt">precision</span> of below 75 μm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10379E..09B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10379E..09B"><span>Adaptive sensor-based <span class="hlt">ultra-high</span> accuracy solar concentrator tracker</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brinkley, Jordyn; Hassanzadeh, Ali</p> <p>2017-09-01</p> <p>Conventional solar trackers use information of the sun's position, either by direct sensing or by GPS. Our method uses the shading of the receiver. This, coupled with nonimaging optics design allows us to achieve <span class="hlt">ultra-high</span> concentration. Incorporating a sensor based shadow tracking method with a two stage concentration solar hybrid parabolic trough allows the system to maintain <span class="hlt">high</span> concentration with acute accuracy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19780023348&hterms=Memory+transfer&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DMemory%2Btransfer','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19780023348&hterms=Memory+transfer&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DMemory%2Btransfer"><span>A wide bandwidth <span class="hlt">CCD</span> buffer memory system</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Siemens, K.; Wallace, R. W.; Robinson, C. R.</p> <p>1978-01-01</p> <p>A prototype system was implemented to demonstrate that <span class="hlt">CCD</span>'s can be applied advantageously to the problem of low power digital storage and particularly to the problem of interfacing widely varying data rates. <span class="hlt">CCD</span> shift register memories (8K bit) were used to construct a feasibility model 128 K-bit buffer memory system. Serial data that can have rates between 150 kHz and 4.0 MHz can be stored in 4K-bit, randomly-accessible memory blocks. Peak power dissipation during a data transfer is less than 7 W, while idle power is approximately 5.4 W. The system features automatic data input synchronization with the recirculating <span class="hlt">CCD</span> memory block start address. System expansion to accommodate parallel inputs or a greater number of memory blocks can be performed in a modular fashion. Since the control logic does not increase proportionally to increase in memory capacity, the power requirements per bit of storage can be reduced significantly in a larger system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApPhL.112k3501G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApPhL.112k3501G"><span><span class="hlt">High</span>-efficiency water-loaded microwave antenna in <span class="hlt">ultra-high</span>-frequency band</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gong, Zilun; Bartone, Chris; Yang, Fuyi; Yao, Jie</p> <p>2018-03-01</p> <p><span class="hlt">High</span>-index dielectrics are widely used in microwave antennas to control the radiation characteristics. Liquid water, with a <span class="hlt">high</span> dielectric index at microwave frequency, is an interesting material to achieving tunable functionalities. Here, we demonstrate a water-loaded microwave antenna system that has <span class="hlt">high</span> loss-tolerance and wideband tunability enabled by fluidity. Our simulation and experimental results show that the resonance frequency can be effectively tuned by the size of loading water. Furthermore, the antenna systems with water loading can achieve <span class="hlt">high</span> radiation efficiency (>90%) in the <span class="hlt">ultra-high</span>-frequency (0.3-3 GHz) band. This work brings about opportunities in realistic tunable microwave antenna designs enabled by liquid.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997ASPC..125..385Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997ASPC..125..385Y"><span>CICADA, <span class="hlt">CCD</span> and Instrument Control Software</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Young, Peter J.; Brooks, Mick; Meatheringham, Stephen J.; Roberts, William H.</p> <p></p> <p>Computerised Instrument Control and Data Acquisition (CICADA) is a software system for control of telescope instruments in a distributed computing environment. It is designed using object-oriented techniques and built with standard computing tools such as RPC, SysV IPC, Posix threads, Tcl, and GUI builders. The system is readily extensible to new instruments and currently supports the Astromed 3200 <span class="hlt">CCD</span> controller and MSSSO's new tip-tilt system. Work is currently underway to provide support for the SDSU <span class="hlt">CCD</span> controller and MSSSO's Double Beam Spectrograph. A core set of processes handle common communication and control tasks, while specific instruments are ``bolted'' on using C++ inheritance techniques.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1212153-high-precision-arithmetic-mathematical-physics','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1212153-high-precision-arithmetic-mathematical-physics"><span><span class="hlt">High-precision</span> arithmetic in mathematical physics</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Bailey, David H.; Borwein, Jonathan M.</p> <p>2015-05-12</p> <p>For many scientific calculations, particularly those involving empirical data, IEEE 32-bit floating-point arithmetic produces results of sufficient accuracy, while for other applications IEEE 64-bit floating-point is more appropriate. But for some very demanding applications, even higher levels of <span class="hlt">precision</span> are often required. Furthermore, this article discusses the challenge of <span class="hlt">high-precision</span> computation, in the context of mathematical physics, and highlights what facilities are required to support future computation, in light of emerging developments in computer architecture.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25132205','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25132205"><span>Simultaneous determination of phenolic compounds in Equisetum palustre L. by <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography with tandem mass spectrometry combined with matrix solid-phase dispersion extraction.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wei, Zuofu; Pan, Youzhi; Li, Lu; Huang, Yuyang; Qi, Xiaolin; Luo, Meng; Zu, Yuangang; Fu, Yujie</p> <p>2014-11-01</p> <p>A method based on matrix solid-phase dispersion extraction followed by <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography with tandem mass spectrometry is presented for the extraction and determination of phenolic compounds in Equisetum palustre. This method combines the <span class="hlt">high</span> efficiency of matrix solid-phase dispersion extraction and the rapidity, sensitivity, and accuracy of <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography with tandem mass spectrometry. The influential parameters of the matrix solid-phase dispersion extraction were investigated and optimized. The optimized conditions were as follows: silica gel was selected as dispersing sorbent, the ratio of silica gel to sample was selected to be 2:1 (400/200 mg), and 8 mL of 80% methanol was used as elution solvent. Furthermore, a fast and sensitive <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography with tandem mass spectrometry method was developed for the determination of nine phenolic compounds in E. palustre. This method was carried out within <6 min, and exhibited satisfactory linearity, <span class="hlt">precision</span>, and recovery. Compared with ultrasound-assisted extraction, the proposed matrix solid-phase dispersion procedure possessed higher extraction efficiency, and was more convenient and time saving with reduced requirements on sample and solvent amounts. All these results suggest that the developed method represents an excellent alternative for the extraction and determination of active components in plant matrices. © 2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10177E..1AL','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10177E..1AL"><span><span class="hlt">Ultra</span>-compact <span class="hlt">high</span>-performance MCT MWIR engine</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lutz, H.; Breiter, R.; Eich, D.; Figgemeier, H.; Oelmaier, R.; Rutzinger, S.; Schenk, H.; Wendler, J.</p> <p>2017-02-01</p> <p>Size, weight and power (SWaP) reduction is <span class="hlt">highly</span> desired by applications such as sights for the dismounted soldier or small gimbals for UAVs. But why have <span class="hlt">high</span> performance and small size of IR systems inevitably exclude each other? Namely, recent development progress in the fields of miniature cryocoolers, short dewars and <span class="hlt">high</span> operating temperature (HOT) FPAs combined with pitch size reduction opens the door for very compact MWIR-modules while keeping <span class="hlt">high</span> electro-optical performance. Now, AIM has realized first prototypes of an <span class="hlt">ultra</span>-compact <span class="hlt">high</span>-performance MWIR engine in a total volume of only 18cl (60mm length x 60mm height x 50mm width). Impressive SWaP characteristics are completed by a total weight below 400g and a power consumption < 4W in basic imaging mode. The engine consists of a XGA-format (1024x768) MCT detector array with 10μm pitch and a low power consuming ROIC. It is cooled down to a typical operating temperature of 160K by the miniature linear cryocooler SX020. The dewar uses a short coldfinger and is designed to reduce the heat load as much as possible. The cooler drive electronics is implemented in the CCE layout in order to reduce the required space of the printed boards and to save power. Uncorrected 14bit video data is provided via Camera Link. Optionally, a small image processing board can be stacked on top of the CCE to gain access to basic functions such as BPR, 2- point NUC and dynamic reduction. This paper will present the design, functionalities and performance data of the <span class="hlt">ultra</span>-compact MCT MWIR engine operated at HOT.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23834497','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23834497"><span>Development and <span class="hlt">ultra</span>-structure of an <span class="hlt">ultra</span>-thin silicone epidermis of bioengineered alternative tissue.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wessels, Quenton; Pretorius, Etheresia</p> <p>2015-08-01</p> <p>Burn wound care today has a primary objective of temporary or permanent wound closure. Commercially available engineered alternative tissues have become a valuable adjunct to the treatment of burn injuries. Their constituents can be biological, alloplastic or a combination of both. Here the authors describe the aspects of the development of a siloxane epidermis for a collagen-glycosaminoglycan and for nylon-based artificial skin replacement products. A method to fabricate an <span class="hlt">ultra</span>-thin epidermal equivalent is described. Pores, to allow the escape of wound exudate, were punched and a tri-filament nylon mesh or collagen scaffold was imbedded and silicone polymerisation followed at 120°C for 5 minutes. The <span class="hlt">ultra</span>-structure of these bilaminates was assessed through scanning electron microscopy. An <span class="hlt">ultra</span>-thin biomedical grade siloxane film was reliably created through <span class="hlt">precision</span> coating on a pre-treated polyethylene terephthalate carrier. © 2013 The Authors. International Wound Journal © 2013 Medicalhelplines.com Inc and John Wiley & Sons Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA135988','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA135988"><span><span class="hlt">Precision</span> Machining Application and Technology: An Overview and Perspective.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1983-08-24</p> <p>diamond turning lathes are being used to produce computer discs. Bryant Symons, an English firm, has reported diamond turning an aluminum computer disk at...34 <span class="hlt">Precision</span> Engineering, Vol. 5(2), Guildford, Engl nd, July 1983. Watt, G., " Lathe for Generation of Spherical -arfaces of Revolution," given to Optical...<span class="hlt">Precision</span> CNC Diamond Turning Machine," Annuals of the CIRP, Vol. 31/1, p 409, 1982. 8. Bryant Simmons Product Brochur-, "<span class="hlt">Ultra</span> <span class="hlt">Precision</span> Oiamond Turning</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810013455','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810013455"><span>Development of a <span class="hlt">CCD</span> array as an imaging detector for advanced X-ray astrophysics facilities</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schwartz, D. A.</p> <p>1981-01-01</p> <p>The development of a charge coupled device (<span class="hlt">CCD</span>) X-ray imager for a large aperture, <span class="hlt">high</span> angular resolution X-ray telescope is discussed. Existing CCDs were surveyed and three candidate concepts were identified. An electronic camera control and computer interface, including software to drive a Fairchild 211 <span class="hlt">CCD</span>, is described. In addition a vacuum mounting and cooling system is discussed. Performance data for the various components are given.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4541858','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4541858"><span>A Real-Time Infrared <span class="hlt">Ultra</span>-Spectral Signature Classification Method via Spatial Pyramid Matching</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Mei, Xiaoguang; Ma, Yong; Li, Chang; Fan, Fan; Huang, Jun; Ma, Jiayi</p> <p>2015-01-01</p> <p>The state-of-the-art <span class="hlt">ultra</span>-spectral sensor technology brings new hope for <span class="hlt">high</span> <span class="hlt">precision</span> applications due to its <span class="hlt">high</span> spectral resolution. However, it also comes with new challenges, such as the <span class="hlt">high</span> data dimension and noise problems. In this paper, we propose a real-time method for infrared <span class="hlt">ultra</span>-spectral signature classification via spatial pyramid matching (SPM), which includes two aspects. First, we introduce an infrared <span class="hlt">ultra</span>-spectral signature similarity measure method via SPM, which is the foundation of the matching-based classification method. Second, we propose the classification method with reference spectral libraries, which utilizes the SPM-based similarity for the real-time infrared <span class="hlt">ultra</span>-spectral signature classification with robustness performance. Specifically, instead of matching with each spectrum in the spectral library, our method is based on feature matching, which includes a feature library-generating phase. We calculate the SPM-based similarity between the feature of the spectrum and that of each spectrum of the reference feature library, then take the class index of the corresponding spectrum having the maximum similarity as the final result. Experimental comparisons on two publicly-available datasets demonstrate that the proposed method effectively improves the real-time classification performance and robustness to noise. PMID:26205263</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1995PhDT........43C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1995PhDT........43C"><span>Application of the <span class="hlt">CCD</span> Fabry-Perot Annular Summing Technique to Thermospheric O(1)D.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Coakley, Monica Marie</p> <p>1995-01-01</p> <p>This work will detail the verification of the advantages of the Fabry-Perot charge coupled device (<span class="hlt">CCD</span>) annular summing technique, the development of the technique for analysis of daysky spectra, and the implications of the resulting spectra for neutral temperature and wind measurements in the daysky thermosphere. The daysky spectral feature of interest is the bright (1 kilo-Rayleigh) thermospheric (OI) emission at 6300 A which had been observed in the nightsky in order to determine winds and temperatures in the vicinity of the altitude of 250 km. In the daysky, the emission line sits on top of a bright Rayleigh scattered continuum background which significantly complicates the observation. With a triple etalon Fabry-Perot spectrometer, the continuum background can be reduced while maintaining <span class="hlt">high</span> throughput and <span class="hlt">high</span> resolution. The inclusion of a <span class="hlt">CCD</span> camera results in significant savings in integration time over the two more standard scanning photomultiplier systems that have made the same wind and temperature measurements in the past. A comparable <span class="hlt">CCD</span> system can experience an order of magnitude savings in integration time over a PMT system. Laboratory and field tests which address the advantages and limitations of both the Fabry-Perot <span class="hlt">CCD</span> annular summing technique and the daysky <span class="hlt">CCD</span> imaging are included in Chap. 2 and Chap. 3. With a sufficiently large throughput associated with the spectrometer and a <span class="hlt">CCD</span> detector, rapid observations (~4 minute integrations) can be made. Extraction of the line width and line center from the daysky near-continuum background is complicated compared to the nightsky case, but possible. Methods of fitting the line are included in Chap. 4. The daysky O ^1D temperatures are consistent with a lower average emission height than predicted by models. The data and models are discussed in Chap. 5. Although some discrepancies exist between resulting temperatures and models, the observations indicate the potential for other direct measurements</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/35739','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/35739"><span>Bond Behavior of Reinforcing Steel in <span class="hlt">Ultra-High</span> Performance Concrete</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2014-11-01</p> <p><span class="hlt">Ultra-high</span> performance concrete (UHPC) has garnered interest from the highway infrastructure community for its greatly enhanced mechanical and durability properties. The objective of this research is to extensively evaluate the factors that affect bo...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26415171','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26415171"><span>Layered compression for <span class="hlt">high-precision</span> depth data.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Miao, Dan; Fu, Jingjing; Lu, Yan; Li, Shipeng; Chen, Chang Wen</p> <p>2015-12-01</p> <p>With the development of depth data acquisition technologies, access to <span class="hlt">high-precision</span> depth with more than 8-b depths has become much easier and determining how to efficiently represent and compress <span class="hlt">high-precision</span> depth is essential for practical depth storage and transmission systems. In this paper, we propose a layered <span class="hlt">high-precision</span> depth compression framework based on an 8-b image/video encoder to achieve efficient compression with low complexity. Within this framework, considering the characteristics of the <span class="hlt">high-precision</span> depth, a depth map is partitioned into two layers: 1) the most significant bits (MSBs) layer and 2) the least significant bits (LSBs) layer. The MSBs layer provides rough depth value distribution, while the LSBs layer records the details of the depth value variation. For the MSBs layer, an error-controllable pixel domain encoding scheme is proposed to exploit the data correlation of the general depth information with sharp edges and to guarantee the data format of LSBs layer is 8 b after taking the quantization error from MSBs layer. For the LSBs layer, standard 8-b image/video codec is leveraged to perform the compression. The experimental results demonstrate that the proposed coding scheme can achieve real-time depth compression with satisfactory reconstruction quality. Moreover, the compressed depth data generated from this scheme can achieve better performance in view synthesis and gesture recognition applications compared with the conventional coding schemes because of the error control algorithm.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5918778-waste-heat-recovery-ultra-high-speed-turbomachinery','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5918778-waste-heat-recovery-ultra-high-speed-turbomachinery"><span>Waste heat recovery with <span class="hlt">ultra</span> <span class="hlt">high</span>-speed turbomachinery</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>Vakkilainen, E.; Larjola, J.; Lindgren, O.</p> <p>1984-08-01</p> <p>A new ORC heat recovery system which converts waste heat to electricity has been developed in Lappeenranta University of Technology with support from Department of Energy in Finnish Ministry of Trade and Industry. Use of <span class="hlt">ultra</span> <span class="hlt">high</span>-speed turbomachinery (10 000 rpm - 200 000 rpm) promises lower unit costs, higher efficiencies and fast amortization rate, 2,4 - 3,0 years.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA069536','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA069536"><span>Characterization of Electrically Active Defects in Si Using <span class="hlt">CCD</span> Image Sensors</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1978-02-01</p> <p>63 35 Dislocation Segments in <span class="hlt">CCD</span> Imager . . . . . . . . . . . . . 64 36 422 Reflection Topograph of Dislocation Loop ir... Loops . . . . . 3 39 422 Reflection Topograph of Scratch on <span class="hlt">CCD</span> Imager, . . . 69 40 Dark Current Display of a <span class="hlt">CCD</span> Imager with 32 ms integration Time...made of each slice using the elon -asoorbio aold developer described in Appendix D. The inagers were then thinned using the procedure at Appendix taor</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23211908B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23211908B"><span>Performance of the STIS <span class="hlt">CCD</span> Dark Rate Temperature Correction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Branton, Doug; STScI STIS Team</p> <p>2018-06-01</p> <p>Since July 2001, the Space Telescope Imaging Spectrograph (STIS) onboard Hubble has operated on its Side-2 electronics due to a failure in the primary Side-1 electronics. While nearly identical, Side-2 lacks a functioning temperature sensor for the <span class="hlt">CCD</span>, introducing a variability in the <span class="hlt">CCD</span> operating temperature. Previous analysis utilized the <span class="hlt">CCD</span> housing temperature telemetry to characterize the relationship between the housing temperature and the dark rate. It was found that a first-order 7%/°C uniform dark correction demonstrated a considerable improvement in the quality of dark subtraction on Side-2 era <span class="hlt">CCD</span> data, and that value has been used on all Side-2 <span class="hlt">CCD</span> darks since. In this report, we show how this temperature correction has performed historically. We compare the current 7%/°C value against the ideal first-order correction at a given time (which can vary between ~6%/°C and ~10%/°C) as well as against a more complex second-order correction that applies a unique slope to each pixel as a function of dark rate and time. At worst, the current correction has performed ~1% worse than the second-order correction. Additionally, we present initial evidence suggesting that the variability in pixel temperature-sensitivity is significant enough to warrant a temperature correction that considers pixels individually rather than correcting them uniformly.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26495722','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26495722"><span>[Reparative Osteogenesis and Angiogenesis in Low Intensity Electromagnetic Radiation of <span class="hlt">Ultra-High</span> Frequency].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Iryanov, Y M; Kiryanov, N A</p> <p>2015-01-01</p> <p>Non-drug correction of reparative bone tissue regeneration in different pathological states - one of the most actual problems of modern medicine. Our aim was to conduct morphological analysis of the influence of electromagnetic radiation of <span class="hlt">ultra-high</span> frequency and low intensity on reparative osteogenesis and angiogenesis in fracture treatment under transosseous osteosynthesis. A controlled nonrandomized study was carried out. In the experiment conducted on rats we modeled tibial fracture with reposition and fixation of the bone fragments both in control and experimental groups. In the animals of the experimental group the fracture zone was exposed to low intensity electromagnetic radiation of <span class="hlt">ultra-high</span> frequency. Exposure simulation was performed in the control group. The operated bones were examined using radiography, light and electronic microscopy, X-ray electronic probe microanalysis. It has been established that electromagnetic radiation of <span class="hlt">ultra-high</span> frequency sessions in fracture treatment stimulate secretory activity and degranulation of mast cells, produce microcirculatory bed vascular permeability increase, endotheliocyte migration phenotype expression, provide endovascular endothelial outgrowth formation, activate reparative osteogenesis and angiogenesis while fracture reparation becomes the one of the primary type. The full periosteal, intermediary and intraosteal bone union was defined in 28 days. Among the therapeutic benefits of electromagnetic radiation of <span class="hlt">ultra-high</span> frequency in fracture treatment we can detect mast cell secretorv activity stimulation and endovascular anziozenesis activation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/35953','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/35953"><span>Development of Non-Proprietary <span class="hlt">Ultra-High</span> Performance Concrete : Final Report</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2017-12-01</p> <p><span class="hlt">Ultra-high</span> performance concrete (UHPC) has mechanical and durability properties that far exceed those of conventional concrete. Particularly, UHPC has compressive and post-cracking tensile strengths of around 20 ksi and 0.72 ksi, respectively. Thus, ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10448E..0WD','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10448E..0WD"><span>Analysis of the application of poly-nanocrystalline diamond tools for <span class="hlt">ultra</span> <span class="hlt">precision</span> machining of steel with ultrasonic assistance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Doetz, M.; Dambon, O.; Klocke, F.; Bulla, B.; Schottka, K.; Robertson, D. J.</p> <p>2017-10-01</p> <p><span class="hlt">Ultra-precision</span> diamond turning enables the manufacturing of parts with mirror-like surfaces and highest form accuracies out of non-ferrous, a few crystalline and plastic materials. Furthermore, an ultrasonic assistance has the ability to push these boundaries and enables the machining of materials like steel, which is not possible in a conventional way due to the excessive tool wear caused by the affinity of carbon to iron. Usually monocrystalline diamonds tools are applied due to their unsurpassed cutting edge properties. New cutting tool material developments have shown that it is possible to produce tools made of nano-polycrystalline diamonds with cutting edges equivalent to monocrystalline diamonds. In nano-polycrystalline diamonds <span class="hlt">ultra</span>-fine grains of a few tens of nanometers are firmly and directly bonded together creating an unisotropic structure. The properties of this material are described to be isotropic, harder and tougher than those of the monocrystalline diamonds, which are unisotropic. This publication will present machining results from the newest investigations of the process potential of this new polycrystalline cutting material. In order to provide a baseline with which to characterize the cutting material cutting experiments on different conventional machinable materials like Cooper or Aluminum are performed. The results provide information on the roughness and the topography of the surface focusing on the comparison to the results while machining with monocrystalline diamond. Furthermore, the cutting material is tested in machining steel with ultrasonic assistance with a focus on tool life time and surface roughness. An outlook on the machinability of other materials will be given.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28517823','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28517823"><span>SU-E-T-161: SOBP Beam Analysis Using Light Output of Scintillation Plate Acquired by <span class="hlt">CCD</span> Camera.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cho, S; Lee, S; Shin, J; Min, B; Chung, K; Shin, D; Lim, Y; Park, S</p> <p>2012-06-01</p> <p>To analyze Bragg-peak beams in SOBP (spread-out Bragg-peak) beam using <span class="hlt">CCD</span> (charge-coupled device) camera - scintillation screen system. We separated each Bragg-peak beam using light output of <span class="hlt">high</span> sensitivity scintillation material acquired by <span class="hlt">CCD</span> camera and compared with Bragg-peak beams calculated by Monte Carlo simulation. In this study, <span class="hlt">CCD</span> camera - scintillation screen system was constructed with a <span class="hlt">high</span> sensitivity scintillation plate (Gd2O2S:Tb) and a right-angled prismatic PMMA phantom, and a Marlin F-201B, EEE-1394 <span class="hlt">CCD</span> camera. SOBP beam irradiated by the double scattering mode of a PROTEUS 235 proton therapy machine in NCC is 8 cm width, 13 g/cm 2 range. The gain, dose rate and current of this beam is 50, 2 Gy/min and 70 nA, respectively. Also, we simulated the light output of scintillation plate for SOBP beam using Geant4 toolkit. We evaluated the light output of <span class="hlt">high</span> sensitivity scintillation plate according to intergration time (0.1 - 1.0 sec). The images of <span class="hlt">CCD</span> camera during the shortest intergration time (0.1 sec) were acquired automatically and randomly, respectively. Bragg-peak beams in SOBP beam were analyzed by the acquired images. Then, the SOBP beam used in this study was calculated by Geant4 toolkit and Bragg-peak beams in SOBP beam were obtained by ROOT program. The SOBP beam consists of 13 Bragg-peak beams. The results of experiment were compared with that of simulation. We analyzed Bragg-peak beams in SOBP beam using light output of scintillation plate acquired by <span class="hlt">CCD</span> camera and compared with that of Geant4 simulation. We are going to study SOBP beam analysis using more effective the image acquisition technique. © 2012 American Association of Physicists in Medicine.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25084664','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25084664"><span>Inactivation of Bacillus spores inoculated in milk by <span class="hlt">Ultra</span> <span class="hlt">High</span> Pressure Homogenization.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Amador Espejo, Genaro Gustavo; Hernández-Herrero, M M; Juan, B; Trujillo, A J</p> <p>2014-12-01</p> <p><span class="hlt">Ultra</span> <span class="hlt">High</span>-Pressure Homogenization treatments at 300 MPa with inlet temperatures (Ti) of 55, 65, 75 and 85 °C were applied to commercial <span class="hlt">Ultra</span> <span class="hlt">High</span> Temperature treated whole milk inoculated with Bacillus cereus, Bacillus licheniformis, Bacillus sporothermodurans, Bacillus coagulans, Geobacillus stearothermophilus and Bacillus subtilis spores in order to evaluate the inactivation level achieved. <span class="hlt">Ultra</span> <span class="hlt">High</span>-Pressure Homogenization conditions at 300 MPa with Ti = 75 and 85 °C were capable of a spore inactivation of ∼5 log CFU/mL. Furthermore, under these processing conditions, commercial sterility (evaluated as the complete inactivation of the inoculated spores) was obtained in milk, with the exception of G. stearothermophilus and B. subtilis treated at 300 MPa with Ti = 75 °C. The results showed that G. stearothermophilus and B. subtilis have higher resistance to the <span class="hlt">Ultra</span> <span class="hlt">High</span>-Pressure Homogenization treatments applied than the other microorganisms inoculated and that a treatment performed at 300 MPa with Ti = 85 °C was necessary to completely inactivate these microorganisms at the spore level inoculated (∼1 × 10(6) CFU/mL). Besides, a change in the resistance of B. licheniformis, B. sporothermodurans, G. stearothermophilus and B. subtilis spores was observed as the inactivation obtained increased remarkably in treatments performed with Ti between 65 and 75 °C. This study provides important evidence of the suitability of UHPH technology for the inactivation of spores in <span class="hlt">high</span> numbers, leading to the possibility of obtaining commercially sterile milk. Copyright © 2014 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23802132','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23802132"><span>Ion profiling in an ambient drift tube-ion mobility spectrometer using a <span class="hlt">high</span> pixel density linear array detector Ion<span class="hlt">CCD</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Davila, Stephen J; Hadjar, Omar; Eiceman, Gary A</p> <p>2013-07-16</p> <p>A linear pixel-based detector array, the Ion<span class="hlt">CCD</span>, is characterized for use under ambient conditions with thermal (<1 eV) positive ions derived from purified air and a 10 mCi (63)Ni foil. The Ion<span class="hlt">CCD</span> combined with a drift tube-ion mobility spectrometer permitted the direct detection of gas phase ions at atmospheric pressure and confirmed a limit of detection of 3000 ions/pixel/frame established previously in both the keV (1-2 keV) and the hyper-thermal (10-40 eV) regimes. Results demonstrate the "broad-band" application of the Ion<span class="hlt">CCD</span> over 10(5) orders in ion energy and over 10(10) in operating pressure. The Faraday detector of a drift tube for an ion mobility spectrometer was replaced with the Ion<span class="hlt">CCD</span> providing images of ion profiles over the cross-section of the drift tube. Patterns in the ion profiles were developed in the drift tube cross-section by control of electric fields between wires of Bradbury Nielson and Tyndall Powell shutter designs at distances of 1-8 cm from the detector. Results showed that ion beams formed in wire sets, retained their shape with limited mixing by diffusion and Coulombic repulsion. Beam broadening determined as 95 μm/cm for hydrated protons in air with moisture of ~10 ppmv. These findings suggest a value of the Ion<span class="hlt">CCD</span> in further studies of ion motion and diffusion of thermalized ions, enhancing computational results from simulation programs, and in the design or operation of ion mobility spectrometers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhSen...8...97L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhSen...8...97L"><span>Sensor-Based Inspection of the Formation Accuracy in <span class="hlt">Ultra-Precision</span> Grinding (UPG) of Aspheric Surface Considering the Chatter Vibration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lei, Yao; Bai, Yue; Xu, Zhijun</p> <p>2018-06-01</p> <p>This paper proposes an experimental approach for monitoring and inspection of the formation accuracy in <span class="hlt">ultra-precision</span> grinding (UPG) with respect to the chatter vibration. Two factors related to the grinding progress, the grinding speed of grinding wheel and spindle, and the oil pressure of the hydrostatic bearing are taken into account to determining the accuracy. In the meantime, a mathematical model of the radius deviation caused by the micro vibration is also established and applied in the experiments. The results show that the accuracy is sensitive to the vibration and the forming accuracy is much improved with proper processing parameters. It is found that the accuracy of aspheric surface can be less than 4 μm when the grinding speed is 1400 r/min and the wheel speed is 100 r/min with the oil pressure being 1.1 MPa.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JAP...113p4306L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JAP...113p4306L"><span><span class="hlt">High</span> longitudinal relaxivity of <span class="hlt">ultra</span>-small gadolinium oxide prepared by microsecond laser ablation in diethylene glycol</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Luo, Ningqi; Tian, Xiumei; Xiao, Jun; Hu, Wenyong; Yang, Chuan; Li, Li; Chen, Dihu</p> <p>2013-04-01</p> <p><span class="hlt">Ultra</span>-small gadolinium oxide (Gd2O3) can be used as T1-weighted Magnetic Resonance Imaging (MRI) contrast agent own to its <span class="hlt">high</span> longitudinal relaxivity (r1) and has attracted intensive attention in these years. In this paper, <span class="hlt">ultra</span>-small Gd2O3 nanoparticles of 3.8 nm in diameter have been successfully synthesized by a microsecond laser ablating a gadolinium (Gd) target in diethylene glycol (DEG). The growth inhibition effect induced by the large viscosity of DEG makes it possible to synthesize <span class="hlt">ultra</span>-small Gd2O3 by laser ablation in DEG. The r1 value and T1-weighted MR images are measured by a 3.0 T MRI spectroscope. The results show these nanoparticles with a <span class="hlt">high</span> r1 value of 9.76 s-1 mM-1 to be good MRI contrast agents. We propose an explanation for the <span class="hlt">high</span> r1 value of <span class="hlt">ultra</span>-small Gd2O3 by considering the decreasing factor (surface to volume ratio of the nanoparticles, S/V) and the increasing factor (water hydration number of the Gd3+ on Gd2O3 surface, q), which offer a new look into the relaxivity studies of MRI contrast agents. Our research provides a new approach to preparing <span class="hlt">ultra</span>-small Gd2O3 of <span class="hlt">high</span> r1 value by laser ablation in DEG and develops the understanding of <span class="hlt">high</span> relaxivity of <span class="hlt">ultra</span>-small Gd2O3 MRI contrast agents.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008SPIE.6837E..04J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008SPIE.6837E..04J"><span>Digital image measurement of specimen deformation based on <span class="hlt">CCD</span> cameras and Image J software: an application to human pelvic biomechanics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jia, Yongwei; Cheng, Liming; Yu, Guangrong; Lou, Yongjian; Yu, Yan; Chen, Bo; Ding, Zuquan</p> <p>2008-03-01</p> <p> matched the clinical results. Digital image measurement of specimen deformation based on <span class="hlt">CCD</span> cameras and Image J software has good perspective for application in biomechanical research, which has the advantage of simple optical setup, no-contact, <span class="hlt">high</span> <span class="hlt">precision</span>, and no special requirement of test environment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004SPIE.5499..452W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004SPIE.5499..452W"><span>AAO2: a general purpose <span class="hlt">CCD</span> controller for the AAT</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Waller, Lew; Barton, John; Mayfield, Don; Griesbach, Jason</p> <p>2004-09-01</p> <p>The Anglo-Australian Observatory has developed a 2nd generation optical <span class="hlt">CCD</span> controller to replace an earlier controller used now for almost twenty years. The new AAO2 controller builds on the considerable experience gained with the first controller, the new technologies now available and the techniques developed and successfully implemented in AAO's IRIS2 detector controller. The AAO2 controller has been designed to operate a wide variety of detectors and to achieve as near to detector limited performance as possible. It is capable of reading out CCDs with one, two or four output amplifiers, each output having its own video processor and <span class="hlt">high</span> speed 16-bit ADC. The video processor is a correlated double sampler that may be switched between low noise dual slope integration or <span class="hlt">high</span> speed clamp and sample modes. Programmable features include low noise DAC biases, horizontal clocks with DAC controllable levels and slopes and vertical clocks with DAC controllable arbitrary waveshapes. The controller uses two DSPs; one for overall control and the other for clock signal generation, which is <span class="hlt">highly</span> programmable, with downloadable sequences of waveform patterns. The controller incorporates a <span class="hlt">precision</span> detector temperature controller and provides accurate exposure time control. Telemetry is provided of all DAC generated voltages, many derived voltages, power supply voltages, detector temperature and detector identification. A <span class="hlt">high</span> speed, full duplex fibre optic interface connects the controller to a host computer. The modular design uses six to ten circuit boards, plugged in to common backplanes. Two backplanes separate noisy digital signals from low noise analog signals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PASP..130f4504B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PASP..130f4504B"><span>A Binary Offset Effect in <span class="hlt">CCD</span> Readout and Its Impact on Astronomical Data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boone, K.; Aldering, G.; Copin, Y.; Dixon, S.; Domagalski, R. S.; Gangler, E.; Pecontal, E.; Perlmutter, S.</p> <p>2018-06-01</p> <p>We have discovered an anomalous behavior of <span class="hlt">CCD</span> readout electronics that affects their use in many astronomical applications. An offset in the digitization of the <span class="hlt">CCD</span> output voltage that depends on the binary encoding of one pixel is added to pixels that are read out one, two, and/or three pixels later. One result of this effect is the introduction of a differential offset in the background when comparing regions with and without flux from science targets. Conventional data reduction methods do not correct for this offset. We find this effect in 16 of 22 instruments investigated, covering a variety of telescopes and many different front-end electronics systems. The affected instruments include LRIS and DEIMOS on the Keck telescopes, WFC3 UVIS and STIS on HST, MegaCam on CFHT, SNIFS on the UH88 telescope, GMOS on the Gemini telescopes, HSC on Subaru, and FORS on VLT. The amplitude of the introduced offset is up to 4.5 ADU per pixel, and it is not directly proportional to the measured ADU level. We have developed a model that can be used to detect this “binary offset effect” in data, and correct for it. Understanding how data are affected and applying a correction for the effect is essential for <span class="hlt">precise</span> astronomical measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1087845','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1087845"><span><span class="hlt">Ultra-high</span> vacuum photoelectron linear accelerator</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Yu, David U.L.; Luo, Yan</p> <p>2013-07-16</p> <p>An rf linear accelerator for producing an electron beam. The outer wall of the rf cavity of said linear accelerator being perforated to allow gas inside said rf cavity to flow to a pressure chamber surrounding said rf cavity and having means of <span class="hlt">ultra</span> <span class="hlt">high</span> vacuum pumping of the cathode of said rf linear accelerator. Said rf linear accelerator is used to accelerate polarized or unpolarized electrons produced by a photocathode, or to accelerate thermally heated electrons produced by a thermionic cathode, or to accelerate rf heated field emission electrons produced by a field emission cathode.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28560266','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28560266"><span>The effect of cognitive remediation in individuals at <span class="hlt">ultra-high</span> risk for psychosis: a systematic review.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Glenthøj, Louise Birkedal; Hjorthøj, Carsten; Kristensen, Tina Dam; Davidson, Charlie Andrew; Nordentoft, Merete</p> <p>2017-01-01</p> <p>Cognitive deficits are prominent features of the <span class="hlt">ultra-high</span> risk state for psychosis that are known to impact functioning and course of illness. Cognitive remediation appears to be the most promising treatment approach to alleviate the cognitive deficits, which may translate into functional improvements. This study systematically reviewed the evidence on the effectiveness of cognitive remediation in the <span class="hlt">ultra-high</span> risk population. The electronic databases MEDLINE, PsycINFO, and Embase were searched using keywords related to cognitive remediation and the UHR state. Studies were included if they were peer-reviewed, written in English, and included a population meeting standardized <span class="hlt">ultra-high</span> risk criteria. Six original research articles were identified. All the studies provided computerized, bottom-up-based cognitive remediation, predominantly targeting neurocognitive function. Four out of five studies that reported a cognitive outcome found cognitive remediation to improve cognition in the domains of verbal memory, attention, and processing speed. Two out of four studies that reported on functional outcome found cognitive remediation to improve the functional outcome in the domains of social functioning and social adjustment. Zero out of the five studies that reported such an outcome found cognitive remediation to affect the magnitude of clinical symptoms. Research on the effect of cognitive remediation in the <span class="hlt">ultra-high</span> risk state is still scarce. The current state of evidence indicates an effect of cognitive remediation on cognition and functioning in <span class="hlt">ultra-high</span> risk individuals. More research on cognitive remediation in <span class="hlt">ultra-high</span> risk is needed, notably in large-scale trials assessing the effect of neurocognitive and/or social cognitive remediation on multiple outcomes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997SPIE.3115..323R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997SPIE.3115..323R"><span>Portal imaging with flat-panel detector and <span class="hlt">CCD</span> camera</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roehrig, Hans; Tang, Chuankun; Cheng, Chee-Wai; Dallas, William J.</p> <p>1997-07-01</p> <p>This paper provides a comparison of imaging parameters of two portal imaging systems at 6 MV: a flat panel detector and a <span class="hlt">CCD</span>-camera based portal imaging system. Measurements were made of the signal and noise and consequently of signal-to-noise per pixel as a function of the exposure. Both systems have a linear response with respect to exposure, and the noise is proportional to the square-root of the exposure, indicating photon-noise limitation. The flat-panel detector has a signal- to-noise ratio, which is higher than that observed wit the <span class="hlt">CCD</span>-camera based portal imaging system. This is expected because most portal imaging systems using optical coupling with a lens exhibit severe quantum-sinks. The paper also presents data on the screen's photon gain (the number of light-photons per interacting x-ray photon), as well as on the magnitude of the Swank-noise, (which describes fluctuation in the screen's photon gain). Images of a Las Vegas-type aluminum contrast detail phantom, located at the ISO-Center, were generated at an exposure of 1 MU. The <span class="hlt">CCD</span>-camera based system permits detection of aluminum-holes of 0.01194 cm diameter and 0.228 mm depth while the flat-panel detector permits detection of aluminum holes of 0.01194 cm diameter and 0.1626 mm depth, indicating a better signal-to-noise ratio. Rank order filtering was applied to the raw images from the <span class="hlt">CCD</span>-based system in order to remove the direct hits. These are camera responses to scattered x-ray photons which interact directly with the <span class="hlt">CCD</span> of the <span class="hlt">CCD</span>-camera and generate 'salt and pepper type noise,' which interferes severely with attempts to determine accurate estimates of the image noise.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930010047','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930010047"><span>Mosaic <span class="hlt">CCD</span> method: A new technique for observing dynamics of cometary magnetospheres</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Saito, T.; Takeuchi, H.; Kozuba, Y.; Okamura, S.; Konno, I.; Hamabe, M.; Aoki, T.; Minami, S.; Isobe, S.</p> <p>1992-01-01</p> <p>On April 29, 1990, the plasma tail of Comet Austin was observed with a <span class="hlt">CCD</span> camera on the 105-cm Schmidt telescope at the Kiso Observatory of the University of Tokyo. The area of the <span class="hlt">CCD</span> used in this observation is only about 1 sq cm. When this <span class="hlt">CCD</span> is used on the 105-cm Schmidt telescope at the Kiso Observatory, the area corresponds to a narrow square view of 12 ft x 12 ft. By comparison with the photograph of Comet Austin taken by Numazawa (personal communication) on the same night, we see that only a small part of the plasma tail can be photographed at one time with the <span class="hlt">CCD</span>. However, by shifting the view on the <span class="hlt">CCD</span> after each exposure, we succeeded in imaging the entire length of the cometary magnetosphere of 1.6 x 10(exp 6) km. This new technique is called 'the mosaic <span class="hlt">CCD</span> method'. In order to study the dynamics of cometary plasma tails, seven frames of the comet from the head to the tail region were twice imaged with the mosaic <span class="hlt">CCD</span> method and two sets of images were obtained. Six microstructures, including arcade structures, were identified in both the images. Sketches of the plasma tail including microstructures are included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JDSO...14..257H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JDSO...14..257H"><span>Measurements of 161 Double Stars With a <span class="hlt">High</span>-Speed <span class="hlt">CCD</span>: The Winter/Spring 2017 Observing Program at Brilliant Sky Observatory, Part 2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harshaw, Richard</p> <p>2018-04-01</p> <p>In the winter and spring of 2017, an aggressive observing program of measuring close double stars with speckle interferometry and <span class="hlt">CCD</span> imaging was undertaken at Brilliant Sky Observatory, my observing site in Cave Creek, Arizona. A total of 596 stars were observed, 8 of which were rejected for various reasons, leaving 588 pairs. Of these, 427 were observed and measured with speckle interferometry, while the remaining 161 were measured with a <span class="hlt">CCD</span>. This paper reports the results of the observations of the 161 <span class="hlt">CCD</span> cases. A separate paper in this issue will report the speckle measurements of the 427 other pairs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10110E..05I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10110E..05I"><span>All plastic <span class="hlt">ultra</span>-small size imaging lens unit fabrication and evaluation for endoscope</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ishii, Kenta; Okamoto, Dai; Ushio, Makoto; Tai, Hidetoshi; Nishihara, Atsuhiko; Tokuda, Kimio; Kawai, Shinsuke; Kitagawa, Seiichiro</p> <p>2017-02-01</p> <p>There is demand for small-size lens units for endoscope and industrial applications. Polished glass lenses with a diameter of 1 - 2mm exist, however plastic lenses similar in size are not commonplace. For low-cost, light-weight, and mass production, plastic lens fabrication is extremely beneficial. Especially, in the medical field, there is strong demand for disposable lens unit for endoscopes which prevent contamination due to reuse of the lens. Therefore, <span class="hlt">high</span> mass producible and low cost becomes increasingly important. This paper reports our findings on injection-molded <span class="hlt">ultra</span>-small size plastic lens units with a diameter of 1.3mm and total thickness of 1.4mm. We performed optical design, injection molding, and lens unit assembly for injection moldable, <span class="hlt">high</span> imaging performance <span class="hlt">ultra</span>-small sized lens units. We prioritize a robust product design, considering injection molding properties and lens unit assembly, with feedback from molding simulations reflected into the optical design. A mold capable of <span class="hlt">high</span> <span class="hlt">precision</span> lens positioning is used to fabricate the lenses and decrease the variability of the assembly. The geometric dimensions of the resulting lenses, are measured and used in the optical simulation to validate the optical performance, and a <span class="hlt">high</span> agreement is reported. The injection molding of the lens and the assembly of the lens unit is performed with <span class="hlt">high</span> <span class="hlt">precision</span>, and results in <span class="hlt">high</span> optical performance.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_17 --> <div id="page_18" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="341"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MMTB...48..983C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MMTB...48..983C"><span>Gas-Enhanced <span class="hlt">Ultra-High</span> Shear Mixing: A Concept and Applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Czerwinski, Frank; Birsan, Gabriel</p> <p>2017-04-01</p> <p>The processes of mixing, homogenizing, and deagglomeration are of paramount importance in many industries for modifying properties of liquids or liquid-based dispersions at room temperature and treatment of molten or semi-molten alloys at <span class="hlt">high</span> temperatures, prior to their solidification. To implement treatments, a variety of technologies based on mechanical, electromagnetic, and ultrasonic principles are used commercially or tested at the laboratory scale. In a large number of techniques, especially those tailored toward metallurgical applications, the vital role is played by cavitation, generation of gas bubbles, and their interaction with the melt. This paper describes a novel concept exploring an integration of gas injection into the shear zone with <span class="hlt">ultra-high</span> shear mixing. As revealed via experiments with a prototype of the cylindrical rotor-stator apparatus and transparent media, gases injected radially through the <span class="hlt">high</span>-speed rotor generate <span class="hlt">highly</span> refined bubbles of <span class="hlt">high</span> concentration directly in the shear zone of the mixer. It is believed that an interaction of large volume of fine gas bubbles with the liquid, superimposed on <span class="hlt">ultra-high</span> shear, will enhance mixing capabilities and cause superior refining and homogenizing of the liquids or solid-liquid slurries, thus allowing their effective property modification.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EntIS..11.1105W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EntIS..11.1105W"><span>Ontology-based coupled optimisation design method using state-space analysis for the spindle box system of large <span class="hlt">ultra-precision</span> optical grinding machine</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Qianren; Chen, Xing; Yin, Yuehong; Lu, Jian</p> <p>2017-08-01</p> <p>With the increasing complexity of mechatronic products, traditional empirical or step-by-step design methods are facing great challenges with various factors and different stages having become inevitably coupled during the design process. Management of massive information or big data, as well as the efficient operation of information flow, is deeply involved in the process of coupled design. Designers have to address increased sophisticated situations when coupled optimisation is also engaged. Aiming at overcoming these difficulties involved in conducting the design of the spindle box system of <span class="hlt">ultra-precision</span> optical grinding machine, this paper proposed a coupled optimisation design method based on state-space analysis, with the design knowledge represented by ontologies and their semantic networks. An electromechanical coupled model integrating mechanical structure, control system and driving system of the motor is established, mainly concerning the stiffness matrix of hydrostatic bearings, ball screw nut and rolling guide sliders. The effectiveness and <span class="hlt">precision</span> of the method are validated by the simulation results of the natural frequency and deformation of the spindle box when applying an impact force to the grinding wheel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NJPh...18j3049C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NJPh...18j3049C"><span>Probabilistic metrology or how some measurement outcomes render <span class="hlt">ultra-precise</span> estimates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Calsamiglia, J.; Gendra, B.; Muñoz-Tapia, R.; Bagan, E.</p> <p>2016-10-01</p> <p>We show on theoretical grounds that, even in the presence of noise, probabilistic measurement strategies (which have a certain probability of failure or abstention) can provide, upon a heralded successful outcome, estimates with a <span class="hlt">precision</span> that exceeds the deterministic bounds for the average <span class="hlt">precision</span>. This establishes a new ultimate bound on the phase estimation <span class="hlt">precision</span> of particular measurement outcomes (or sequence of outcomes). For probe systems subject to local dephasing, we quantify such <span class="hlt">precision</span> limit as a function of the probability of failure that can be tolerated. Our results show that the possibility of abstaining can set back the detrimental effects of noise.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24718166','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24718166"><span>Atmospheric correction of HJ-1 <span class="hlt">CCD</span> imagery over turbid lake waters.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Minwei; Tang, Junwu; Dong, Qing; Duan, Hongtao; Shen, Qian</p> <p>2014-04-07</p> <p>We have presented an atmospheric correction algorithm for HJ-1 <span class="hlt">CCD</span> imagery over Lakes Taihu and Chaohu with <span class="hlt">highly</span> turbid waters. The Rayleigh scattering radiance (Lr) is calculated using the hyperspectral Lr with a wavelength interval 1nm. The hyperspectral Lr is interpolated from Lr in the central wavelengths of MODIS bands, which are converted from the band response-averaged Lr calculated using the Rayleigh look up tables (LUTs) in SeaDAS6.1. The scattering radiance due to aerosol (La) is interpolated from La at MODIS band 869nm, which is derived from MODIS imagery using a shortwave infrared atmospheric correction scheme. The accuracy of the atmospheric correction algorithm is firstly evaluated by comparing the <span class="hlt">CCD</span> measured remote sensing reflectance (Rrs) with MODIS measurements, which are validated by the in situ data. The <span class="hlt">CCD</span> measured Rrs is further validated by the in situ data for a total of 30 observation stations within ± 1h time window of satellite overpass and field measurements. The validation shows the mean relative errors about 0.341, 0.259, 0.293 and 0.803 at blue, green, red and near infrared bands.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JPhCS.486a2002V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JPhCS.486a2002V"><span><span class="hlt">High</span> <span class="hlt">precision</span> spectroscopy and imaging in THz frequency range</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vaks, Vladimir L.</p> <p>2014-03-01</p> <p>Application of microwave methods for development of the THz frequency range has resulted in elaboration of <span class="hlt">high</span> <span class="hlt">precision</span> THz spectrometers based on nonstationary effects. The spectrometers characteristics (spectral resolution and sensitivity) meet the requirements for <span class="hlt">high</span> <span class="hlt">precision</span> analysis. The gas analyzers, based on the <span class="hlt">high</span> <span class="hlt">precision</span> spectrometers, have been successfully applied for analytical investigations of gas impurities in <span class="hlt">high</span> pure substances. These investigations can be carried out both in absorption cell and in reactor. The devices can be used for ecological monitoring, detecting the components of chemical weapons and explosive in the atmosphere. The great field of THz investigations is the medicine application. Using the THz spectrometers developed one can detect markers for some diseases in exhaled air.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1175684','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1175684"><span><span class="hlt">Ultra-high</span> speed vacuum pump system with first stage turbofan and second stage turbomolecular pump</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Jostlein, Hans</p> <p>2006-04-04</p> <p>An <span class="hlt">ultra-high</span> speed vacuum pump evacuation system includes a first stage <span class="hlt">ultra-high</span> speed turbofan and a second stage conventional turbomolecular pump. The turbofan is either connected in series to a chamber to be evacuated, or is optionally disposed entirely within the chamber. The turbofan employs large diameter rotor blades operating at <span class="hlt">high</span> linear blade velocity to impart an <span class="hlt">ultra-high</span> pumping speed to a fluid. The second stage turbomolecular pump is fluidly connected downstream from the first stage turbofan. In operation, the first stage turbofan operates in a pre-existing vacuum, with the fluid asserting only small axial forces upon the rotor blades. The turbofan imparts a velocity to fluid particles towards an outlet at a <span class="hlt">high</span> volume rate, but moderate compression ratio. The second stage conventional turbomolecular pump then compresses the fluid to pressures for evacuation by a roughing pump.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22308585-novel-femtosecond-gated-high-resolution-frequency-shifted-shearing-interferometry-technique-probing-pre-plasma-expansion-ultra-intense-laser-experiments','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22308585-novel-femtosecond-gated-high-resolution-frequency-shifted-shearing-interferometry-technique-probing-pre-plasma-expansion-ultra-intense-laser-experiments"><span>A novel femtosecond-gated, <span class="hlt">high</span>-resolution, frequency-shifted shearing interferometry technique for probing pre-plasma expansion in <span class="hlt">ultra</span>-intense laser experiments</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>Feister, S., E-mail: feister.7@osu.edu; Orban, C.; Innovative Scientific Solutions, Inc., Dayton, Ohio 45459</p> <p></p> <p><span class="hlt">Ultra</span>-intense laser-matter interaction experiments (>10{sup 18} W/cm{sup 2}) with dense targets are <span class="hlt">highly</span> sensitive to the effect of laser “noise” (in the form of pre-pulses) preceding the main <span class="hlt">ultra</span>-intense pulse. These system-dependent pre-pulses in the nanosecond and/or picosecond regimes are often intense enough to modify the target significantly by ionizing and forming a plasma layer in front of the target before the arrival of the main pulse. Time resolved interferometry offers a robust way to characterize the expanding plasma during this period. We have developed a novel pump-probe interferometry system for an <span class="hlt">ultra</span>-intense laser experiment that uses two short-pulse amplifiersmore » synchronized by one <span class="hlt">ultra</span>-fast seed oscillator to achieve 40-fs time resolution over hundreds of nanoseconds, using a variable delay line and other techniques. The first of these amplifiers acts as the pump and delivers maximal energy to the interaction region. The second amplifier is frequency shifted and then frequency doubled to generate the femtosecond probe pulse. After passing through the laser-target interaction region, the probe pulse is split and recombined in a laterally sheared Michelson interferometer. Importantly, the frequency shift in the probe allows strong plasma self-emission at the second harmonic of the pump to be filtered out, allowing plasma expansion near the critical surface and elsewhere to be clearly visible in the interferograms. To aid in the reconstruction of phase dependent imagery from fringe shifts, three separate 120° phase-shifted (temporally sheared) interferograms are acquired for each probe delay. Three-phase reconstructions of the electron densities are then inferred by Abel inversion. This interferometric system delivers <span class="hlt">precise</span> measurements of pre-plasma expansion that can identify the condition of the target at the moment that the <span class="hlt">ultra</span>-intense pulse arrives. Such measurements are indispensable for correlating laser pre</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009BaltA..18..219N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009BaltA..18..219N"><span>STARL -- a Program to Correct <span class="hlt">CCD</span> Image Defects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Narbutis, D.; Vanagas, R.; Vansevičius, V.</p> <p></p> <p>We present a program tool, STARL, designed for automatic detection and correction of various defects in <span class="hlt">CCD</span> images. It uses genetic algorithm for deblending and restoring of overlapping saturated stars in crowded stellar fields. Using Subaru Telescope Suprime-Cam images we demonstrate that the program can be implemented in the wide-field survey data processing pipelines for production of <span class="hlt">high</span> quality color mosaics. The source code and examples are available at the STARL website.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9296E..0AW','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9296E..0AW"><span>Design of multi-mode compatible image acquisition system for HD area array <span class="hlt">CCD</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Chen; Sui, Xiubao</p> <p>2014-11-01</p> <p>Combining with the current development trend in video surveillance-digitization and <span class="hlt">high</span>-definition, a multimode-compatible image acquisition system for HD area array <span class="hlt">CCD</span> is designed. The hardware and software designs of the color video capture system of HD area array <span class="hlt">CCD</span> KAI-02150 presented by Truesense Imaging company are analyzed, and the structure parameters of the HD area array <span class="hlt">CCD</span> and the color video gathering principle of the acquisition system are introduced. Then, the <span class="hlt">CCD</span> control sequence and the timing logic of the whole capture system are realized. The noises of the video signal (KTC noise and 1/f noise) are filtered by using the Correlated Double Sampling (CDS) technique to enhance the signal-to-noise ratio of the system. The compatible designs in both software and hardware for the two other image sensors of the same series: KAI-04050 and KAI-08050 are put forward; the effective pixels of these two HD image sensors are respectively as many as four million and eight million. A Field Programmable Gate Array (FPGA) is adopted as the key controller of the system to perform the modularization design from top to bottom, which realizes the hardware design by software and improves development efficiency. At last, the required time sequence driving is simulated accurately by the use of development platform of Quartus II 12.1 combining with VHDL. The result of the simulation indicates that the driving circuit is characterized by simple framework, low power consumption, and strong anti-interference ability, which meet the demand of miniaturization and <span class="hlt">high</span>-definition for the current tendency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26193140','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26193140"><span>Smear correction of <span class="hlt">highly</span> variable, frame-transfer <span class="hlt">CCD</span> images with application to polarimetry.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Iglesias, Francisco A; Feller, Alex; Nagaraju, Krishnappa</p> <p>2015-07-01</p> <p>Image smear, produced by the shutterless operation of frame-transfer <span class="hlt">CCD</span> detectors, can be detrimental for many imaging applications. Existing algorithms used to numerically remove smear do not contemplate cases where intensity levels change considerably between consecutive frame exposures. In this report, we reformulate the smearing model to include specific variations of the sensor illumination. The corresponding desmearing expression and its noise properties are also presented and demonstrated in the context of fast imaging polarimetry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JMOp...64..379Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JMOp...64..379Z"><span>Real-time tricolor phase measuring profilometry based on <span class="hlt">CCD</span> sensitivity calibration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Lin; Cao, Yiping; He, Dawu; Chen, Cheng</p> <p>2017-02-01</p> <p>A real-time tricolor phase measuring profilometry (RTPMP) based on charge coupled device (<span class="hlt">CCD</span>) sensitivity calibration is proposed. Only one colour fringe pattern whose red (R), green (G) and blue (B) components are, respectively, coded as three sinusoidal phase-shifting gratings with an equivalent shifting phase of 2π/3 is needed and sent to an appointed flash memory on a specialized digital light projector (SDLP). A specialized time-division multiplexing timing sequence actively controls the SDLP to project the fringe patterns in R, G and B channels sequentially onto the measured object in one over seventy-two of a second and meanwhile actively controls a <span class="hlt">high</span> frame rate monochrome <span class="hlt">CCD</span> camera to capture the corresponding deformed patterns synchronously with the SDLP. So the sufficient information for reconstructing the three-dimensional (3D) shape in one over twenty-four of a second is obtained. Due to the different spectral sensitivity of the <span class="hlt">CCD</span> camera to RGB lights, the captured deformed patterns from R, G and B channels cannot share the same peak and valley, which will lead to lower accuracy or even failing to reconstruct the 3D shape. So a deformed pattern amending method based on <span class="hlt">CCD</span> sensitivity calibration is developed to guarantee the accurate 3D reconstruction. The experimental results verify the feasibility of the proposed RTPMP method. The proposed RTPMP method can obtain the 3D shape at over the video frame rate of 24 frames per second, avoid the colour crosstalk completely and be effective for measuring real-time changing object.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4946631','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4946631"><span><span class="hlt">Ultra-high-precision</span> Nd-isotope measurements of geological materials by MC-ICPMS</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Saji, Nikitha Susan; Wielandt, Daniel; Paton, Chad; Bizzarro, Martin</p> <p>2016-01-01</p> <p>We report novel techniques allowing the measurement of Nd-isotope ratios with unprecedented accuracy and <span class="hlt">precision</span> by multi-collector inductively coupled plasma mass spectrometry. Using the new protocol, we have measured the Nd-isotopic composition of rock and synthetic Nd standards as well as that of the Allende carbonaceous chondrite. Analyses of BCR-2, BHVO-2 and GSP-2 rock standards yield mass-independent compositions identical to the JNdi-1 Nd-reference standard, with an external reproducibility of 2.4, 1.6, 1.6 and 3.5 ppm respectively, on μ142Nd, μ145Nd, μ146Nd and μ150Nd (μ representing the ppm-deviation of the ratios from JNdi-1) using 148Nd/144Nd for internal normalization. This represents an improvement in <span class="hlt">precision</span> by a factor of 2, 7 and 9 respectively for μ142Nd, μ145Nd and μ150Nd. Near-quantitative recovery from purification chemistry and sample-standard bracketing allow for the determination of mass-dependent Nd-isotopic composition of samples. Synthetic standards, namely La Jolla and AMES, record mass-dependent variability of up to 1.2 ε per atomic mass unit and mass-independent compositions resolvable by up to 3 ppm for μ142Nd and 8 ppm for μ150Nd, relative to JNdi-1. The mass-independent compositions are consistent with equilibrium mass fractionation during purification. The terrestrial rock standards define a uniform stable ε145Nd of −0.24 ± 0.19 (2SD) relative to JNdi-1, indistinguishable from the mean Allende ε145Nd of −0.19 ± 0.09. We consider this value to represent the mass-dependent Nd-isotope composition of Bulk Silicate Earth (BSE). The modest mass-dependent fractionation of JNdi-1 relative to BSE results in potential effects on mass-independent composition that cannot be resolved within the reproducibility of our analyses when correcting for natural and instrumental mass fractionation by kinetic law, making it a suitable reference standard for analysis of unknowns. Analysis of Allende (CV3) carbonaceous chondrite</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AIPC..969.1045B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AIPC..969.1045B"><span>Proposed <span class="hlt">Ultra-High</span> Sensitivity <span class="hlt">High</span>-Frequency Gravitational Wave Detector</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baker, Robert M. L.; Stephenson, Gary V.; Li, Fangyu</p> <p>2008-01-01</p> <p>The paper discusses the proposed improvement of a <span class="hlt">High</span>-Frequency Relic Gravitational Wave (HFRGW) detector designed by Li, Baker, Fang, Stephenson and Chen in order to greatly improve its sensitivity. The improved detector is inspired by the Laser Interferometer Gravitational Observatory or LIGO, but is sensitive to the <span class="hlt">high</span>-frequency end of the gravitational-wave spectrum. As described in prior papers it utilizes the Gertsenshtein effect, which introduces the conversion of gravitational waves to electromagnetic (EM) waves in the presence of a static magnetic field. Such a conversion, if it leads to photons moving in a direction perpendicular to the plane of the EM waves and the magnetic field, will allow for <span class="hlt">ultra-high</span> sensitivity HFRGW detection. The use of sensitive microwave, single photon detectors such as a circuit QED and/or the Rydberg Atom Cavity Detector, or off-the-shelf detectors, could lead to such detection. When the EM-detection photons are focused at the microwave detectors by fractal-membrane reflectors sensitivity is also improved. Noise sources external to the HFRGW detector will be eliminated by placing a tight mosaic of superconducting tiles (e.g., YBCO) and/or fractal membranes on the interior surface of the detector's cryogenic containment vessel in order to provide a perfect Faraday cage. Internal thermal noise will be eliminated by means of a microwave absorbing (or reflecting) interior enclosure shaped to conform to a <span class="hlt">high</span>-intensity continuous microwave Gaussian beam (GB), will reduce any background photon flux (BPF) noise radiated normal to the GB's axis. Such BPF will be further attenuated by a series of microwave absorbing baffles forming tunnels to the sensitive microwave detectors on each side of the GB and at right angles to the static magnetic field. A HFGW detector of bandwidth of 1 KHz to 10 KHz or less in the GHz band has been selected. It is concluded that the utilization of the new <span class="hlt">ultra-high</span>-sensitivity microwave detectors</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10463E..1ED','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10463E..1ED"><span><span class="hlt">High-precision</span> processing and detection of the <span class="hlt">high</span>-caliber off-axis aspheric mirror</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dai, Chen; Li, Ang; Xu, Lingdi; Zhang, Yingjie</p> <p>2017-10-01</p> <p>To achieve the efficient, controllable, digital processing and <span class="hlt">high-precision</span> detection of the <span class="hlt">high</span>-caliber off-axis aspheric mirror, meeting the <span class="hlt">high</span>-level development needs of the modern <span class="hlt">high</span>-resolution, large field of space optical remote sensing camera, we carried out the research on <span class="hlt">high</span> <span class="hlt">precision</span> machining and testing technology of off-axis aspheric mirror. First, we forming the off-axis aspheric sample with diameter of 574mm × 302mm by milling it with milling machine, and then the intelligent robot equipment was used for off-axis aspheric <span class="hlt">high</span> <span class="hlt">precision</span> polishing. Surface detection of the sample will be proceed with the off-axis aspheric contact contour detection technology and offaxis non-spherical surface interference detection technology after its fine polishing using ion beam equipment. The final surface accuracy RMS is 12nm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9684E..0SW','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9684E..0SW"><span>Study on <span class="hlt">high-precision</span> measurement of long radius of curvature</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, Dongcheng; Peng, Shijun; Gao, Songtao</p> <p>2016-09-01</p> <p>It is hard to get <span class="hlt">high-precision</span> measurement of the radius of curvature (ROC), because of many factors that affect the measurement accuracy. For the measurement of long radius of curvature, some factors take more important position than others'. So, at first this paper makes some research about which factor is related to the long measurement distance, and also analyse the uncertain of the measurement accuracy. At second this article also study the influence about the support status and the adjust error about the cat's eye and confocal position. At last, a 1055micrometer radius of curvature convex is measured in <span class="hlt">high-precision</span> laboratory. Experimental results show that the proper steady support (three-point support) can guarantee the <span class="hlt">high-precision</span> measurement of radius of curvature. Through calibrating the gain of cat's eye and confocal position, is useful to ensure the <span class="hlt">precise</span> position in order to increase the measurement accuracy. After finish all the above process, the <span class="hlt">high-precision</span> long ROC measurement is realized.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9915E..0YS','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9915E..0YS"><span>Development of low-noise <span class="hlt">CCD</span> drive electronics for the world space observatory ultraviolet spectrograph subsystem</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Salter, Mike; Clapp, Matthew; King, James; Morse, Tom; Mihalcea, Ionut; Waltham, Nick; Hayes-Thakore, Chris</p> <p>2016-07-01</p> <p>World Space Observatory Ultraviolet (WSO-UV) is a major Russian-led international collaboration to develop a large space-borne 1.7 m Ritchey-Chrétien telescope and instrumentation to study the universe at ultraviolet wavelengths between 115 nm and 320 nm, exceeding the current capabilities of ground-based instruments. The WSO Ultraviolet Spectrograph subsystem (WUVS) is led by the Institute of Astronomy of the Russian Academy of Sciences and consists of two <span class="hlt">high</span> resolution spectrographs covering the Far-UV range of 115-176 nm and the Near-UV range of 174-310 nm, and a long-slit spectrograph covering the wavelength range of 115-305 nm. The custom-designed <span class="hlt">CCD</span> sensors and cryostat assemblies are being provided by e2v technologies (UK). STFC RAL Space is providing the Camera Electronics Boxes (CEBs) which house the <span class="hlt">CCD</span> drive electronics for each of the three WUVS channels. This paper presents the results of the detailed characterisation of the WUVS <span class="hlt">CCD</span> drive electronics. The electronics include a novel <span class="hlt">high</span>-performance video channel design that utilises Digital Correlated Double Sampling (DCDS) to enable low-noise readout of the <span class="hlt">CCD</span> at a range of pixel frequencies, including a baseline requirement of less than 3 electrons rms readout noise for the combined <span class="hlt">CCD</span> and electronics system at a readout rate of 50 kpixels/s. These results illustrate the performance of this new video architecture as part of a wider electronics sub-system that is designed for use in the space environment. In addition to the DCDS video channels, the CEB provides all the bias voltages and clocking waveforms required to operate the <span class="hlt">CCD</span> and the system is fully programmable via a primary and redundant SpaceWire interface. The development of the CEB electronics design has undergone critical design review and the results presented were obtained using the engineering-grade electronics box. A variety of parameters and tests are included ranging from general system metrics, such as the power and mass</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA495056','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA495056"><span>Design of <span class="hlt">Ultra-High</span> Temperature Ceramics for Improved Performance</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2009-02-28</p> <p>e.g., grain boundary chemistry or change in impurity concentrations) or physical (e.g., residual stress) effects. 600 co 500 a. oi400 c CD i...SA037 Effects of oxygen content on the properties of supcr-<span class="hlt">high</span>-teiiiperature resistant Si-AI- C fibers D.f. Zhao (National University of Defense...of Technology, China) 15:05 S A034 Oxyacetylene ablation behavior of carbon fibers reinforced carbon matrix and <span class="hlt">ultra-high</span> temperature</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910014760','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910014760"><span><span class="hlt">High</span> <span class="hlt">precision</span> applications of the global positioning system</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lichten, Stephen M.</p> <p>1991-01-01</p> <p>The Global Positioning System (GPS) is a constellation of U.S. defense navigation satellites which can be used for military and civilian positioning applications. A wide variety of GPS scientific applications were identified and <span class="hlt">precise</span> positioning capabilities with GPS were already demonstrated with data available from the present partial satellite constellation. Expected applications include: measurements of Earth crustal motion, particularly in seismically active regions; measurements of the Earth's rotation rate and pole orientation; <span class="hlt">high-precision</span> Earth orbiter tracking; surveying; measurements of media propagation delays for calibration of deep space radiometric data in support of NASA planetary missions; determination of <span class="hlt">precise</span> ground station coordinates; and <span class="hlt">precise</span> time transfer worldwide.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24810850','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24810850"><span>mrsFAST-<span class="hlt">Ultra</span>: a compact, SNP-aware mapper for <span class="hlt">high</span> performance sequencing applications.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hach, Faraz; Sarrafi, Iman; Hormozdiari, Farhad; Alkan, Can; Eichler, Evan E; Sahinalp, S Cenk</p> <p>2014-07-01</p> <p><span class="hlt">High</span> throughput sequencing (HTS) platforms generate unprecedented amounts of data that introduce challenges for processing and downstream analysis. While tools that report the 'best' mapping location of each read provide a fast way to process HTS data, they are not suitable for many types of downstream analysis such as structural variation detection, where it is important to report multiple mapping loci for each read. For this purpose we introduce mrsFAST-<span class="hlt">Ultra</span>, a fast, cache oblivious, SNP-aware aligner that can handle the multi-mapping of HTS reads very efficiently. mrsFAST-<span class="hlt">Ultra</span> improves mrsFAST, our first cache oblivious read aligner capable of handling multi-mapping reads, through new and compact index structures that reduce not only the overall memory usage but also the number of CPU operations per alignment. In fact the size of the index generated by mrsFAST-<span class="hlt">Ultra</span> is 10 times smaller than that of mrsFAST. As importantly, mrsFAST-<span class="hlt">Ultra</span> introduces new features such as being able to (i) obtain the best mapping loci for each read, and (ii) return all reads that have at most n mapping loci (within an error threshold), together with these loci, for any user specified n. Furthermore, mrsFAST-<span class="hlt">Ultra</span> is SNP-aware, i.e. it can map reads to reference genome while discounting the mismatches that occur at common SNP locations provided by db-SNP; this significantly increases the number of reads that can be mapped to the reference genome. Notice that all of the above features are implemented within the index structure and are not simple post-processing steps and thus are performed <span class="hlt">highly</span> efficiently. Finally, mrsFAST-<span class="hlt">Ultra</span> utilizes multiple available cores and processors and can be tuned for various memory settings. Our results show that mrsFAST-<span class="hlt">Ultra</span> is roughly five times faster than its predecessor mrsFAST. In comparison to newly enhanced popular tools such as Bowtie2, it is more sensitive (it can report 10 times or more mappings per read) and much faster (six times or</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/31148','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/31148"><span>MDOT aims for lower-cost <span class="hlt">ultra-high</span> performance concrete : research spotlight.</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2016-08-01</p> <p>In recent years, several vendors have developed <span class="hlt">ultra-high</span> performance : concrete (UHPC) that surpasses traditional concrete mixes by offering : exceptional freeze-thaw resistance, reduced susceptibility to cracking : and far less reinforcement corro...</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('https://www.osti.gov/servlets/purl/1039706','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1039706"><span>Multilayer <span class="hlt">ultra-high</span>-temperature ceramic coatings</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Loehman, Ronald E [Albuquerque, NM; Corral, Erica L [Tucson, AZ</p> <p>2012-03-20</p> <p>A coated carbon-carbon composite material with multiple ceramic layers to provide oxidation protection from <span class="hlt">ultra-high</span>-temperatures, where if the carbon-carbon composite material is uninhibited with B.sub.4C particles, then the first layer on the composite material is selected from ZrB.sub.2 and HfB.sub.2, onto which is coated a layer of SiC coated and if the carbon-carbon composite material is inhibited with B.sub.4C particles, then protection can be achieved with a layer of SiC and a layer of either ZrB.sub.2 and HfB.sub.2 in any order.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JInst..12C1035G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JInst..12C1035G"><span>On-ground and in-orbit characterisation plan for the PLATO <span class="hlt">CCD</span> normal cameras</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gow, J. P. D.; Walton, D.; Smith, A.; Hailey, M.; Curry, P.; Kennedy, T.</p> <p>2017-11-01</p> <p>PLAnetary Transits and Ocillations (PLATO) is the third European Space Agency (ESA) medium class mission in ESA's cosmic vision programme due for launch in 2026. PLATO will carry out <span class="hlt">high</span> <span class="hlt">precision</span> un-interrupted photometric monitoring in the visible band of large samples of bright solar-type stars. The primary mission goal is to detect and characterise terrestrial exoplanets and their systems with emphasis on planets orbiting in the habitable zone, this will be achieved using light curves to detect planetary transits. PLATO uses a novel multi- instrument concept consisting of 26 small wide field cameras The 26 cameras are made up of a telescope optical unit, four Teledyne e2v <span class="hlt">CCD</span>270s mounted on a focal plane array and connected to a set of Front End Electronics (FEE) which provide <span class="hlt">CCD</span> control and readout. There are 2 fast cameras with <span class="hlt">high</span> read-out cadence (2.5 s) for magnitude ~ 4-8 stars, being developed by the German Aerospace Centre and 24 normal (N) cameras with a cadence of 25 s to monitor stars with a magnitude greater than 8. The N-FEEs are being developed at University College London's Mullard Space Science Laboratory (MSSL) and will be characterised along with the associated CCDs. The CCDs and N-FEEs will undergo rigorous on-ground characterisation and the performance of the CCDs will continue to be monitored in-orbit. This paper discusses the initial development of the experimental arrangement, test procedures and current status of the N-FEE. The parameters explored will include gain, quantum efficiency, pixel response non-uniformity, dark current and Charge Transfer Inefficiency (CTI). The current in-orbit characterisation plan is also discussed which will enable the performance of the CCDs and their associated N-FEE to be monitored during the mission, this will include measurements of CTI giving an indication of the impact of radiation damage in the CCDs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SPIE10539E..02K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SPIE10539E..02K"><span><span class="hlt">Ultra-high</span>-speed variable focus optics for novel applications in advanced imaging</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kang, S.; Dotsenko, E.; Amrhein, D.; Theriault, C.; Arnold, C. B.</p> <p>2018-02-01</p> <p>With the advancement of <span class="hlt">ultra</span>-fast manufacturing technologies, <span class="hlt">high</span> speed imaging with <span class="hlt">high</span> 3D resolution has become increasingly important. Here we show the use of an <span class="hlt">ultra-high</span>-speed variable focus optical element, the TAG Lens, to enable new ways to acquire 3D information from an object. The TAG Lens uses sound to adjust the index of refraction profile in a liquid and thereby can achieve focal scanning rates greater than 100 kHz. When combined with a <span class="hlt">high</span>-speed pulsed LED and a <span class="hlt">high</span>-speed camera, we can exploit this phenomenon to achieve <span class="hlt">high</span>-resolution imaging through large depths. By combining the image acquisition with digital image processing, we can extract relevant parameters such as tilt and angle information from objects in the image. Due to the <span class="hlt">high</span> speeds at which images can be collected and processed, we believe this technique can be used as an efficient method of industrial inspection and metrology for <span class="hlt">high</span> throughput applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22772833','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22772833"><span>Construction of a photochemical reactor combining a <span class="hlt">CCD</span> spectrophotometer and a LED radiation source.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gombár, Melinda; Józsa, Éva; Braun, Mihály; Ősz, Katalin</p> <p>2012-10-01</p> <p>An inexpensive photoreactor using LED light sources and a fibre-optic <span class="hlt">CCD</span> spectrophotometer as a detector was built by designing a special cell holder for standard 1.000 cm cuvettes. The use of this device was demonstrated by studying the aqueous photochemical reaction of 2,5-dichloro-1,4-benzoquinone. The developed method combines the <span class="hlt">highly</span> quantitative data collection of <span class="hlt">CCD</span> spectrophotometers with the possibility of illuminating the sample independently of the detecting light beam, which is a substantial improvement of the method using diode array spectrophotometers as photoreactors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005ITNS...52..519B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005ITNS...52..519B"><span>Anomalous Annealing of a <span class="hlt">High</span>-Resistivity <span class="hlt">CCD</span> Irradiated at Low Temperature</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bautz, M.; Prigozhin, G.; Kissel, S.; LaMarr, B.; Grant, C.; Brown, S.</p> <p>2005-04-01</p> <p>The front-illuminated charge-coupled device (<span class="hlt">CCD</span>) detectors in the Chandra X-ray Observatory's ACIS instrument suffered radiation damage from soft protons focused by the telescope mirror early in the mission. In the course of assessing this damage, the focal plane was temporarily warmed from its normal operating temperature (then -100/spl deg/C) to +30/spl deg/C. Following this "bakeout", the radiation-damaged CCDs exhibited significantly greater charge transfer inefficiency (CTI). We performed a laboratory experiment with a sibling of the flight detectors in an attempt to reproduce and better understand this phenomenon. The test <span class="hlt">CCD</span> was cooled to -100/spl deg/C, irradiated by 120 keV protons and then warmed to +30/spl deg/C for 8 hours. As expected, after the initial irradiation, but before detector warmup, a substantial CTI increase was observed. The subsequent warmup itself then produced an additional factor /spl ap/2.5 increase in CTI. Following smaller subsequent irradiations with the detector cold, a "bakeout" for 8 hours at -60/spl deg/C produced no observable increase in CTI. However, a subsequent bakeout to +30/spl deg/C for another 8 hours resulted in an additional increase in CTI of roughly 15%. The CTI changes produced by the room temperature bakeout are accompanied by dramatic changes in the de-trapping times of electron traps responsible for the CTI. The distributions of signal amplitudes in the pixels trailing X-ray events indicate that annealing at room temperature can cause large changes of the trap emission times, from which we infer that conversion of trapping defects takes place. The observed phenomena can be explained by the previously suggested mechanism of carbon-related defect transformation. Specifically, the room-temperature annealing may allow carbon interstitials to form metastable complexes with phosphorus and/or carbon substitutional atoms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090008382','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090008382"><span>NASA / Pratt and Whitney Collaborative Partnership Research in <span class="hlt">Ultra</span> <span class="hlt">High</span> Bypass Cycle Propulsion Concepts</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hughes, Chris; Lord, Wed</p> <p>2008-01-01</p> <p>Current collaborative research with Pratt & Whitney on <span class="hlt">Ultra</span> <span class="hlt">High</span> Bypass Engine Cycle noise, performance and emissions improvements as part of the Subsonic Fixed Wing Project <span class="hlt">Ultra</span> <span class="hlt">High</span> Bypass Engine Partnership Element is discussed. The Subsonic Fixed Wing Project goals are reviewed, as well as their relative technology level compared to previous NASA noise program goals. Progress toward achieving the Subsonic Fixed Wing Project goals over the 2008 fiscal year by the UHB Partnership in this area of research are reviewed. The current research activity in <span class="hlt">Ultra</span> <span class="hlt">High</span> Bypass Engine Cycle technology, specifically the Pratt & Whitney Geared Turbofan, at NASA and Pratt & Whitney are discussed including the contributions each entity bring toward the research project, and technical plans and objectives. Pratt & Whitney Geared Turbofan current and future technology and business plans are also discussed, including the role the NASA SFW UHB partnership plays toward achieving those goals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/869249','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/869249"><span>Portable <span class="hlt">high</span> <span class="hlt">precision</span> pressure transducer system</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Piper, Thomas C.; Morgan, John P.; Marchant, Norman J.; Bolton, Steven M.</p> <p>1994-01-01</p> <p>A <span class="hlt">high</span> <span class="hlt">precision</span> pressure transducer system for checking the reliability of a second pressure transducer system used to monitor the level of a fluid confined in a holding tank. Since the response of the pressure transducer is temperature sensitive, it is continually housed in an battery powered oven which is configured to provide a temperature stable environment at specified temperature for an extended period of time. Further, a <span class="hlt">high</span> <span class="hlt">precision</span> temperature stabilized oscillator and counter are coupled to a single board computer to accurately determine the pressure transducer oscillation frequency and convert it to an applied pressure. All of the components are powered by the batteries which during periods of availability of line power are charged by an on board battery charger. The pressure readings outputs are transmitted to a line printer and a vacuum florescent display.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5033709','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/5033709"><span>Portable <span class="hlt">high</span> <span class="hlt">precision</span> pressure transducer system</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Piper, T.C.; Morgan, J.P.; Marchant, N.J.; Bolton, S.M.</p> <p>1994-04-26</p> <p>A <span class="hlt">high</span> <span class="hlt">precision</span> pressure transducer system is described for checking the reliability of a second pressure transducer system used to monitor the level of a fluid confined in a holding tank. Since the response of the pressure transducer is temperature sensitive, it is continually housed in an battery powered oven which is configured to provide a temperature stable environment at specified temperature for an extended period of time. Further, a <span class="hlt">high</span> <span class="hlt">precision</span> temperature stabilized oscillator and counter are coupled to a single board computer to accurately determine the pressure transducer oscillation frequency and convert it to an applied pressure. All of the components are powered by the batteries which during periods of availability of line power are charged by an on board battery charger. The pressure readings outputs are transmitted to a line printer and a vacuum fluorescent display. 2 figures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MNRAS.469.4889E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MNRAS.469.4889E"><span><span class="hlt">Precision</span> of natural satellite ephemerides from observations of different types</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Emelyanov, N. V.</p> <p>2017-08-01</p> <p>Currently, various types of observations of natural planetary satellites are used to refine their ephemerides. A new type of measurement - determining the instants of apparent satellite encounters - has recently been proposed by Morgado and co-workers. The problem that arises is which type of measurement to choose in order to obtain an ephemeris <span class="hlt">precision</span> that is as <span class="hlt">high</span> as possible. The answer can be obtained only by modelling the entire process: observations, obtaining the measured values, refining the satellite motion parameters, and generating the ephemeris. The explicit dependence of the ephemeris <span class="hlt">precision</span> on observational accuracy as well as on the type of observations is unknown. In this paper, such a dependence is investigated using the Monte Carlo statistical method. The relationship between the ephemeris <span class="hlt">precision</span> for different types of observations is then assessed. The possibility of using the instants of apparent satellite encounters to obtain an ephemeris is investigated. A method is proposed that can be used to fit the satellite orbital parameters to this type of measurement. It is shown that, in the absence of systematic scale errors in the <span class="hlt">CCD</span> frame, the use of the instants of apparent encounters leads to less <span class="hlt">precise</span> ephemerides. However, in the presence of significant scale errors, which is often the case, this type of measurement becomes effective because the instants of apparent satellite encounters do not depend on scale errors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007JASS...24..349K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007JASS...24..349K"><span>Design and Development of Multi-Purpose <span class="hlt">CCD</span> Camera System with Thermoelectric Cooling: Hardware</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kang, Y.-W.; Byun, Y. I.; Rhee, J. H.; Oh, S. H.; Kim, D. K.</p> <p>2007-12-01</p> <p>We designed and developed a multi-purpose <span class="hlt">CCD</span> camera system for three kinds of CCDs; KAF-0401E(768×512), KAF-1602E(1536×1024), KAF-3200E(2184×1472) made by KODAK Co.. The system supports fast USB port as well as parallel port for data I/O and control signal. The packing is based on two stage circuit boards for size reduction and contains built-in filter wheel. Basic hardware components include clock pattern circuit, A/D conversion circuit, <span class="hlt">CCD</span> data flow control circuit, and <span class="hlt">CCD</span> temperature control unit. The <span class="hlt">CCD</span> temperature can be controlled with accuracy of approximately 0.4° C in the max. range of temperature, Δ 33° C. This <span class="hlt">CCD</span> camera system has with readout noise 6 e^{-}, and system gain 5 e^{-}/ADU. A total of 10 <span class="hlt">CCD</span> camera systems were produced and our tests show that all of them show passable performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMGP51A1364C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMGP51A1364C"><span><span class="hlt">Ultra</span>-low power <span class="hlt">high</span> <span class="hlt">precision</span> magnetotelluric receiver array based customized computer and wireless sensor network</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, R.; Xi, X.; Zhao, X.; He, L.; Yao, H.; Shen, R.</p> <p>2016-12-01</p> <p>Dense 3D magnetotelluric (MT) data acquisition owns the benefit of suppressing the static shift and topography effect, can achieve <span class="hlt">high</span> <span class="hlt">precision</span> and <span class="hlt">high</span> resolution inversion for underground structure. This method may play an important role in mineral exploration, geothermal resources exploration, and hydrocarbon exploration. It's necessary to reduce the power consumption greatly of a MT signal receiver for large-scale 3D MT data acquisition while using sensor network to monitor data quality of deployed MT receivers. We adopted a series of technologies to realized above goal. At first, we designed an low-power embedded computer which can couple with other parts of MT receiver tightly and support wireless sensor network. The power consumption of our embedded computer is less than 1 watt. Then we designed 4-channel data acquisition subsystem which supports 24-bit analog-digital conversion, GPS synchronization, and real-time digital signal processing. Furthermore, we developed the power supply and power management subsystem for MT receiver. At last, a series of software, which support data acquisition, calibration, wireless sensor network, and testing, were developed. The software which runs on personal computer can monitor and control over 100 MT receivers on the field for data acquisition and quality control. The total power consumption of the receiver is about 2 watts at full operation. The standby power consumption is less than 0.1 watt. Our testing showed that the MT receiver can acquire good quality data at ground with electrical dipole length as 3 m. Over 100 MT receivers were made and used for large-scale geothermal exploration in China with great success.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10567E..3QG','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10567E..3QG"><span>Advanced optical systems for <span class="hlt">ultra</span> <span class="hlt">high</span> energy cosmic rays detection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gambicorti, L.; Pace, E.; Mazzinghi, P.</p> <p>2017-11-01</p> <p>A new advanced optical system is proposed and analysed in this work with the purpose to improve the photons collection efficiency of Multi-AnodePhotoMultipliers (MAPMT) detectors, which will be used to cover large focal surface of instruments dedicated to the <span class="hlt">Ultra</span> <span class="hlt">High</span> Energy Cosmic Rays (UHECRs, above 1019eV) and <span class="hlt">Ultra</span> <span class="hlt">High</span> Energy Neutrino (UHEN) detection. The employment of the advanced optical system allows to focus all photons inside the sensitive area of detectors and to improve the signal-to-noise ratios in the wavelength range of interest (300-400nm), thus coupling imaging and filtering capability. Filter is realised with a multilayer coating to reach <span class="hlt">high</span> transparency in UV range and with a sharp cut-off outside. In this work the applications on different series of PMTs have been studied and results of simulations are shown. First prototypes have been realised. Finally, this paper proposes another class of adapters to be optically coupled on each pixel of MAPMT detector selected, consisting of non-imaging concentrators as Winston cones.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26698819','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26698819"><span>Examining the association between social cognition and functioning in individuals at <span class="hlt">ultra-high</span> risk for psychosis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cotter, Jack; Bartholomeusz, Cali; Papas, Alicia; Allott, Kelly; Nelson, Barnaby; Yung, Alison R; Thompson, Andrew</p> <p>2017-01-01</p> <p>Social and role functioning are compromised for the majority of individuals at <span class="hlt">ultra-high</span> risk of psychosis, and it is important to identify factors that contribute to this functional decline. This study aimed to investigate social cognitive abilities, which have previously been linked to functioning in schizophrenia, as potential factors that impact social, role and global functioning in <span class="hlt">ultra-high</span> risk patients. A total of 30 <span class="hlt">ultra-high</span> risk patients were recruited from an established at-risk clinical service in Melbourne, Australia, and completed a battery of social cognitive, neurocognitive, clinical and functioning measures. We examined the relationships between all four core domains of social cognition (emotion recognition, theory of mind, social perception and attributional style), neurocognitive, clinical and demographic variables with three measures of functioning (the Global Functioning Social and Role scales and the Social and Occupational Functioning Assessment Scale) using correlational and multiple regression analyses. Performance on a visual theory of mind task (visual jokes task) was significantly correlated with both concurrent role ( r = 0.425, p = 0.019) and global functioning ( r = 0.540, p = 0.002). In multivariate analyses, it also accounted for unique variance in global, but not role functioning after adjusting for negative symptoms and stress. Social functioning was not associated with performance on any of the social cognition tasks. Among specific social cognitive abilities, only a test of theory of mind was associated with functioning in our <span class="hlt">ultra-high</span> risk sample. Further longitudinal research is needed to examine the impact of social cognitive deficits on long-term functional outcome in the <span class="hlt">ultra-high</span> risk group. Identifying social cognitive abilities that significantly impact functioning is important to inform the development of targeted intervention programmes for <span class="hlt">ultra-high</span> risk individuals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22676086-influence-observatory-latitude-study-ultra-high-energy-cosmic-rays','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22676086-influence-observatory-latitude-study-ultra-high-energy-cosmic-rays"><span>The influence of the observatory latitude on the study of <span class="hlt">ultra</span> <span class="hlt">high</span> energy cosmic rays</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>Anjos, Rita C. dos; De Souza, Vitor; De Almeida, Rogerio M.</p> <p>2017-07-01</p> <p>Recent <span class="hlt">precision</span> measurements of the <span class="hlt">Ultra</span> <span class="hlt">High</span> Energy Cosmic Rays (UHECR) arrival directions, spectrum and parameters related to the mass of the primary particle have been done by the HiRes, Pierre Auger and Telescope Array (TA) Observatories. In this paper, distributions of arrival directions of events in the nearby Universe are assumed to correlate with sources in the 2MASS Redshift Survey (2MRS), IRAS 1.2 Jy Survey, Palermo Swift-BAT and Swift-BAT catalogs, and the effect of the latitude of the observatory on the measurement of the energy spectrum and on the capability of measuring anisotropy is studied. The differences between givenmore » latitudes on the northern and southern hemispheres are quantified. It is shown that the latitude of the observatory: a) has an influence on the total flux measured and b) imposes an important limitation on the capability of measuring an anisotropic sky.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25481418','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25481418"><span>Multidetection of antibiotics in liver tissue by <span class="hlt">ultra-high</span>-pressure-liquid-chromatography-tandem mass spectrometry.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Freitas, Andreia; Barbosa, Jorge; Ramos, Fernando</p> <p>2015-01-22</p> <p>A multiresidue quantitative screening method covering 39 antibiotics from 7 different families by <span class="hlt">ultra-high</span>-pressure-liquid-chromatography-tandem mass spectrometry (UHPLC-MS/MS) is described. Sulfonamides, trimethoprim, tetracyclines, macrolides, quinolones, penicillins and chloramphenicol are simultaneously detected in liver tissue. A simple sample treatment method consisting of extraction with a mixture of acetonitrile and ethylenediaminetetraacetic acid (EDTA) followed by solid-phase extraction (SPE) with a hydrophilic-lipophilic balanced (HLB) cartridge was developed. The methodology was validated, in accordance with Decision 2002/657/EC, by evaluating the following required parameters: decision limit (CCα), detection capability (CCβ), specificity, repeatability and reproducibility. The <span class="hlt">precision</span>, in terms of the relative standard deviation, was under 22% for all of the compounds, and the recoveries were between 80% and 110%. The CCα and CCβ were determined according to the maximum residue limit (MRL) or the minimum required performance limit (MRPL), when established. Copyright © 2014 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997SPIE.3200..183V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997SPIE.3200..183V"><span>UV-sensitive scientific <span class="hlt">CCD</span> image sensors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vishnevsky, Grigory I.; Kossov, Vladimir G.; Iblyaminova, A. F.; Lazovsky, Leonid Y.; Vydrevitch, Michail G.</p> <p>1997-06-01</p> <p>An investigation of probe laser irradiation interaction with substances containing in an environment has long since become a recognized technique for contamination detection and identification. For this purpose, a near and midrange-IR laser irradiation is traditionally used. However, as many works presented on last ecology monitoring conferences show, in addition to traditional systems, rapidly growing are systems with laser irradiation from near-UV range (250 - 500 nm). Use of <span class="hlt">CCD</span> imagers is one of the prerequisites for this allowing the development of a multi-channel computer-based spectral research system. To identify and analyze contaminating impurities on an environment, such methods as laser fluorescence analysis, UV absorption and differential spectroscopy, Raman scattering are commonly used. These methods are used to identify a large number of impurities (petrol, toluene, Xylene isomers, SO2, acetone, methanol), to detect and identify food pathogens in real time, to measure a concentration of NH3, SO2 and NO in combustion outbursts, to detect oil products in a water, to analyze contaminations in ground waters, to define ozone distribution in the atmosphere profile, to monitor various chemical processes including radioactive materials manufacturing, heterogeneous catalytic reactions, polymers production etc. Multi-element image sensor with enhanced UV sensitivity, low optical non-uniformity, low intrinsic noise and <span class="hlt">high</span> dynamic range is a key element of all above systems. Thus, so called Virtual Phase (VP) CCDs possessing all these features, seems promising for ecology monitoring spectral measuring systems. Presently, a family of VP CCDs with different architecture and number of pixels is developed and being manufactured. All CCDs from this family are supported with a <span class="hlt">precise</span> slow-scan digital image acquisition system that can be used in various image processing systems in astronomy, biology, medicine, ecology etc. An image is displayed directly on a PC</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20026749-high-performance-radial-amtec-cell-design-ultra-high-power-solar-amtec-systems','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20026749-high-performance-radial-amtec-cell-design-ultra-high-power-solar-amtec-systems"><span><span class="hlt">High</span>-performance radial AMTEC cell design for <span class="hlt">ultra-high</span>-power solar AMTEC 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>Hendricks, T.J.; Huang, C.</p> <p>1999-07-01</p> <p>Alkali Metal Thermal to Electric Conversion (AMTEC) technology is rapidly maturing for potential application in <span class="hlt">ultra-high</span>-power solar AMTEC systems required by potential future US Air Force (USAF) spacecraft missions in medium-earth and geosynchronous orbits (MEO and GEO). Solar thermal AMTEC power systems potentially have several important advantages over current solar photovoltaic power systems in <span class="hlt">ultra-high</span>-power spacecraft applications for USAF MEO and GEO missions. This work presents key aspects of radial AMTEC cell design to achieve <span class="hlt">high</span> cell performance in solar AMTEC systems delivering larger than 50 kW(e) to support <span class="hlt">high</span> power USAF missions. These missions typically require AMTEC cell conversionmore » efficiency larger than 25%. A sophisticated design parameter methodology is described and demonstrated which establishes optimum design parameters in any radial cell design to satisfy <span class="hlt">high</span>-power mission requirements. Specific relationships, which are distinct functions of cell temperatures and pressures, define critical dependencies between key cell design parameters, particularly the impact of parasitic thermal losses on Beta Alumina Solid Electrolyte (BASE) area requirements, voltage, number of BASE tubes, and system power production for both maximum power-per-BASE-area and optimum efficiency conditions. Finally, some <span class="hlt">high</span>-level system tradeoffs are demonstrated using the design parameter methodology to establish <span class="hlt">high</span>-power radial cell design requirements and philosophy. The discussion highlights how to incorporate this methodology with sophisticated SINDA/FLUINT AMTEC cell modeling capabilities to determine optimum radial AMTEC cell designs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19770018485','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19770018485"><span>Solid state television camera (<span class="hlt">CCD</span>-buried channel), revision 1</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1977-01-01</p> <p>An all solid state television camera was designed which uses a buried channel charge coupled device (<span class="hlt">CCD</span>) as the image sensor. A 380 x 488 element <span class="hlt">CCD</span> array is utilized to ensure compatibility with 525-line transmission and display monitor equipment. Specific camera design approaches selected for study and analysis included (1) optional clocking modes for either fast (1/60 second) or normal (1/30 second) frame readout, (2) techniques for the elimination or suppression of <span class="hlt">CCD</span> blemish effects, and (3) automatic light control and video gain control techniques to eliminate or minimize sensor overload due to bright objects in the scene. Preferred approaches were determined and integrated into a deliverable solid state TV camera which addressed the program requirements for a prototype qualifiable to space environment conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/35956','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/35956"><span>Development of Non-Proprietary <span class="hlt">Ultra-High</span> Performance Concrete : Project Summary Report</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2017-12-01</p> <p><span class="hlt">Ultra-high</span> performance concrete (UHPC) has mechanical and durability properties that far exceed those of conventional concrete. Thus, elements made with UHPC can be thinner/lighter than elements made with conventional concrete. The enhanced durabilit...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1034557','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1034557"><span>Design of a <span class="hlt">CCD</span> Camera for Space Surveillance</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2016-03-05</p> <p>Laboratory fabricated CCID-51M, a 2048x1024 pixel Charge Couple Device (<span class="hlt">CCD</span>) imager. [1] The mission objective is to observe and detect satellites in...phased to transfer the charge to the outputs. An electronic shutter is created by having an equal area of pixels covered by an opaque metal mask. The...Figure 4 CDS Timing Diagram By design the <span class="hlt">CCD</span> readout rate is 400 KHz. This rate was chosen so reading the 2E6 pixels from one output is less than</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('https://www.osti.gov/servlets/purl/874674','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/874674"><span>Device for wavefront correction in an <span class="hlt">ultra</span> <span class="hlt">high</span> power laser</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Ault, Earl R.; Comaskey, Brian J.; Kuklo, Thomas C.</p> <p>2002-01-01</p> <p>A system for wavefront correction in an <span class="hlt">ultra</span> <span class="hlt">high</span> power laser. As the laser medium flows past the optical excitation source and the fluid warms its index of refraction changes creating an optical wedge. A system is provided for correcting the thermally induced optical phase errors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22714317','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22714317"><span><span class="hlt">High</span>-power <span class="hlt">ultra</span>-broadband frequency comb from ultraviolet to infrared by <span class="hlt">high</span>-power fiber amplifiers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yang, Kangwen; Li, Wenxue; Yan, Ming; Shen, Xuling; Zhao, Jian; Zeng, Heping</p> <p>2012-06-04</p> <p>A <span class="hlt">high</span>-power <span class="hlt">ultra</span>-broadband frequency comb covering the spectral range from ultraviolet to infrared was generated directly by nonlinear frequency conversion of a multi-stage <span class="hlt">high</span>-power fiber comb amplifier. The 1030-nm infrared spectral fraction of a broadband Ti:sapphire femtosecond frequency comb was power-scaled up to 100 W average power by using a large-mode-area fiber chirped-pulse amplifier. We obtained a frequency-doubled green comb at 515 nm and frequency-quadrupled ultraviolet pulses at 258 nm with the average power of 12.8 and 1.62 W under the input infrared power of 42.2 W, respectively. The carrier envelope phase stabilization was accomplished with an <span class="hlt">ultra</span>-narrow line-width of 1.86 mHz and a quite low accumulated phase jitter of 0.41 rad, corresponding to a timing jitter of 143 as.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012APS..MAR.Y6012G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012APS..MAR.Y6012G"><span><span class="hlt">Ultra-high</span> density aligned Carbon-nanotube with controled nano-morphology for supercapacitors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ghaffari, Mehdi; Zhao, Ran; Liu, Yang; Zhou, Yue; Cheng, Jiping; Guzman de Villoria, Roberto; Wardle, B. L.; Zhang, Q. M.</p> <p>2012-02-01</p> <p>Recent advances in fabricating controlled-morphology vertically aligned carbon nanotubes (VA-CNTs) with ultrahigh volume fractioncreate unique opportunities for developing unconventional supercapacitors with <span class="hlt">ultra-high</span> energy density, power density, and long charge/discharge cycle life.Continuous paths through inter-VA-CNT channels allow fast ion transport, and <span class="hlt">high</span> electrical conduction of the aligned CNTs in the composite electrodes lead to fast discharge speed. We investigate the charge-discharge characteristics of VA-CNTs with >20 vol% of CNT and ionic liquids as electrolytes. By employing both the electric and electromechanical spectroscopes, as well as nanostructured materials characterization, the ion transport and storage behaviors in porous electrodes are studied. The results suggest pathways for optimizing the electrode morphology in supercapacitorsusing <span class="hlt">ultra-high</span> volume fraction VA-CNTs to further enhance performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/35889','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/35889"><span>Development of a Family of <span class="hlt">Ultra-High</span> Performance Concrete Pi-Girders</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2014-01-01</p> <p><span class="hlt">Ultra-high</span> performance concrete (UHPC) is an advanced cementitious composite material, which tends to exhibit superior properties such as exceptional durability, increased strength, and long-term stability. (See references 1-4.) The use of existing s...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/18193','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/18193"><span><span class="hlt">Ultra-high</span> performance concrete for Michigan bridges, material performance : phase I.</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2008-10-13</p> <p>One of the latest advancements in concrete technology is <span class="hlt">Ultra-High</span> Performance Concrete (UHPC). UHPC is : defined as concretes attaining compressive strengths exceeding 25 ksi (175 MPa). It is a fiber-reinforced, denselypacked : concrete material wh...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28688908','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28688908"><span><span class="hlt">Ultra</span>-wide-field imaging in diabetic retinopathy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ghasemi Falavarjani, Khalil; Tsui, Irena; Sadda, Srinivas R</p> <p>2017-10-01</p> <p>Since 1991, 7-field images captured with 30-50 degree cameras in the Early Treatment Diabetic Retinopathy Study were the gold standard for fundus imaging to study diabetic retinopathy. <span class="hlt">Ultra</span>-wide-field images cover significantly more area (up to 82%) of the fundus and with ocular steering can in many cases image 100% of the fundus ("panretinal"). Recent advances in image analysis of <span class="hlt">ultra</span>-wide-field imaging allow for <span class="hlt">precise</span> measurements of the peripheral retinal lesions. There is a growing consensus in the literature that <span class="hlt">ultra</span>-wide-field imaging improves detection of peripheral lesions in diabetic retinopathy and leads to more accurate classification of the disease. There is discordance among studies, however, on the correlation between peripheral diabetic lesions and diabetic macular edema and optimal management strategies to treat diabetic retinopathy. Copyright © 2017 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005NIMPA.542..148V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005NIMPA.542..148V"><span>Dynamic imaging with a triggered and intensified <span class="hlt">CCD</span> camera system in a <span class="hlt">high</span>-intensity neutron beam</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vontobel, P.; Frei, G.; Brunner, J.; Gildemeister, A. E.; Engelhardt, M.</p> <p>2005-04-01</p> <p>When time-dependent processes within metallic structures should be inspected and visualized, neutrons are well suited due to their <span class="hlt">high</span> penetration through Al, Ag, Ti or even steel. Then it becomes possible to inspect the propagation, distribution and evaporation of organic liquids as lubricants, fuel or water. The principle set-up of a suited real-time system was implemented and tested at the radiography facility NEUTRA of PSI. The highest beam intensity there is 2×107 cm s, which enables to observe sequences in a reasonable time and quality. The heart of the detection system is the MCP intensified <span class="hlt">CCD</span> camera PI-Max with a Peltier cooled chip (1300×1340 pixels). The intensifier was used for both gating and image enhancement, where as the information was accumulated over many single frames on the chip before readout. Although, a 16-bit dynamic range is advertised by the camera manufacturers, it must be less due to the inherent noise level from the intensifier. The obtained result should be seen as the starting point to go ahead to fit the different requirements of car producers in respect to fuel injection, lubricant distribution, mechanical stability and operation control. Similar inspections will be possible for all devices with repetitive operation principle. Here, we report about two measurements dealing with the lubricant distribution in a running motorcycle motor turning at 1200 rpm. We were monitoring the periodic stationary movements of piston, valves and camshaft with a micro-channel plate intensified <span class="hlt">CCD</span> camera system (PI-Max 1300RB, Princeton Instruments) triggered at exactly chosen time points.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PASP..130g4401B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PASP..130g4401B"><span>KPS-1b: The First Transiting Exoplanet Discovered Using an Amateur Astronomer's Wide-field <span class="hlt">CCD</span> Data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Burdanov, Artem; Benni, Paul; Sokov, Eugene; Krushinsky, Vadim; Popov, Alexander; Delrez, Laetitia; Gillon, Michael; Hébrard, Guillaume; Deleuil, Magali; Wilson, Paul A.; Demangeon, Olivier; Baştürk, Özgür; Pakštiene, Erika; Sokova, Iraida; Rusov, Sergei A.; Dyachenko, Vladimir V.; Rastegaev, Denis A.; Beskakotov, Anatoliy; Marchini, Alessandro; Bretton, Marc; Shadick, Stan; Ivanov, Kirill</p> <p>2018-07-01</p> <p>We report the discovery of the transiting hot Jupiter KPS-1b. This exoplanet orbits a V = 13.0 K1-type main-sequence star every 1.7 days, has a mass of {1.090}-0.087+0.086 M Jup and a radius of {1.03}-0.12+0.13 R Jup. The discovery was made by the prototype Kourovka Planet Search (KPS) project, which used wide-field <span class="hlt">CCD</span> data gathered by an amateur astronomer using readily available and relatively affordable equipment. Here we describe the equipment and observing technique used for the discovery of KPS-1b, its characterization with spectroscopic observations by the SOPHIE spectrograph and with <span class="hlt">high-precision</span> photometry obtained with 1 m class telescopes. We also outline the KPS project evolution into the Galactic Plane eXoplanet survey. The discovery of KPS-1b represents a new major step of the contribution of amateur astronomers to the burgeoning field of exoplanetology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012Cryo...52..505I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012Cryo...52..505I"><span>Integrated computational study of <span class="hlt">ultra-high</span> heat flux cooling using cryogenic micro-solid nitrogen spray</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ishimoto, Jun; Oh, U.; Tan, Daisuke</p> <p>2012-10-01</p> <p>A new type of <span class="hlt">ultra-high</span> heat flux cooling system using the atomized spray of cryogenic micro-solid nitrogen (SN2) particles produced by a superadiabatic two-fluid nozzle was developed and numerically investigated for application to next generation super computer processor thermal management. The fundamental characteristics of heat transfer and cooling performance of micro-solid nitrogen particulate spray impinging on a heated substrate were numerically investigated and experimentally measured by a new type of integrated computational-experimental technique. The employed Computational Fluid Dynamics (CFD) analysis based on the Euler-Lagrange model is focused on the cryogenic spray behavior of atomized particulate micro-solid nitrogen and also on its <span class="hlt">ultra-high</span> heat flux cooling characteristics. Based on the numerically predicted performance, a new type of cryogenic spray cooling technique for application to a <span class="hlt">ultra-high</span> heat power density device was developed. In the present integrated computation, it is clarified that the cryogenic micro-solid spray cooling characteristics are affected by several factors of the heat transfer process of micro-solid spray which impinges on heated surface as well as by atomization behavior of micro-solid particles. When micro-SN2 spraying cooling was used, an <span class="hlt">ultra-high</span> cooling heat flux level was achieved during operation, a better cooling performance than that with liquid nitrogen (LN2) spray cooling. As micro-SN2 cooling has the advantage of direct latent heat transport which avoids the film boiling state, the <span class="hlt">ultra</span>-short time scale heat transfer in a thin boundary layer is more possible than in LN2 spray. The present numerical prediction of the micro-SN2 spray cooling heat flux profile can reasonably reproduce the measurement results of cooling wall heat flux profiles. The application of micro-solid spray as a refrigerant for next generation computer processors is anticipated, and its <span class="hlt">ultra-high</span> heat flux technology is expected</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.ars.usda.gov/research/publications/publication/?seqNo115=244068','TEKTRAN'); return false;" href="http://www.ars.usda.gov/research/publications/publication/?seqNo115=244068"><span>Caveats when Analyzing <span class="hlt">Ultra-high</span> Molar Mass Polymers by SEC</span></a></p> <p><a target="_blank" href="https://www.ars.usda.gov/research/publications/find-a-publication/">USDA-ARS?s Scientific Manuscript database</a></p> <p></p> <p></p> <p>The analysis of <span class="hlt">ultra-high</span> molar mass (M > 1 million g/mol) polymers via size-exclusion chromatography (SEC) presents a number of non-trivial challenges. Dissolution and full solvation may take days, as is the case for cellulose dissolution in non-complexing non degrading solvents; very low concent...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1330273','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1330273"><span>Study of Volumetrically Heated <span class="hlt">Ultra-High</span> Energy Density 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>Rocca, Jorge J.</p> <p>2016-10-27</p> <p>Heating dense matter to millions of degrees is important for applications, but requires complex and expensive methods. The major goal of the project was to demonstrate using a compact laser the creation of a new <span class="hlt">ultra-high</span> energy density plasma regime characterized by simultaneous extremely <span class="hlt">high</span> temperature and <span class="hlt">high</span> density, and to study it combining experimental measurements and advanced simulations. We have demonstrated that trapping of intense femtosecond laser pulses deep within ordered nanowire arrays can heat near solid density matter into a new <span class="hlt">ultra</span> hot plasma regime. Extreme electron densities, and temperatures of several tens of million degrees were achievedmore » using laser pulses of only 0.5 J energy from a compact laser. Our x-ray spectra and simulations showed that extremely <span class="hlt">highly</span> ionized plasma volumes several micrometers in depth are generated by irradiation of gold and Nickel nanowire arrays with femtosecond laser pulses of relativistic intensities. We obtained extraordinarily <span class="hlt">high</span> degrees of ionization (e.g. we peeled 52 electrons from gold atoms, and up to 26 electrons from nickel atoms). In the process we generated Gigabar pressures only exceeded in the central hot spot of <span class="hlt">highly</span> compressed thermonuclear fusion plasmas.. The plasma created after the dissolved wires expand, collide, and thermalize, is computed to have a thermal energy density of 0.3 GJ cm -3 and a pressure of 1-2 Gigabar. These are pressures only exceeded in <span class="hlt">highly</span> compressed thermonuclear fusion plasmas. Scaling these results to higher laser intensities promises to create plasmas with temperatures and pressures exceeding those in the center of the sun.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5091470','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5091470"><span>Differential renal effects of candesartan at <span class="hlt">high</span> and <span class="hlt">ultra-high</span> doses in diabetic mice–potential role of the ACE2/AT2R/Mas axis</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Callera, Glaucia E.; Antunes, Tayze T.; Correa, Jose W.; Moorman, Danielle; Gutsol, Alexey; He, Ying; Cat, Aurelie Nguyen Dinh; Briones, Ana M.; Montezano, Augusto C.; Burns, Kevin D.; Touyz, Rhian M.</p> <p>2016-01-01</p> <p><span class="hlt">High</span> doses of Ang II receptor (AT1R) blockers (ARBs) are renoprotective in diabetes. Underlying mechanisms remain unclear. We evaluated whether <span class="hlt">high/ultra-high</span> doses of candesartan (ARB) up-regulate angiotensin-converting enzyme 2 (ACE2)/Ang II type 2 receptor (AT2R)/Mas receptor [protective axis of the of the renin–angiotensin system (RAS)] in diabetic mice. Systolic blood pressure (SBP), albuminuria and expression/activity of RAS components were assessed in diabetic db/db and control db/+ mice treated with increasing candesartan doses (intermediate, 1 mg/kg/d; <span class="hlt">high</span>, 5 mg/kg/d; <span class="hlt">ultra-high</span>, 25 and 75 mg/kg/d; 4 weeks). Lower doses candesartan did not influence SBP, but <span class="hlt">ultra-high</span> doses reduced SBP in both groups. Plasma glucose and albuminuria were increased in db/db compared with db/+ mice. In diabetic mice treated with intermediate dose candesartan, renal tubular damage and albuminuria were ameliorated and expression of ACE2, AT2R and Mas and activity of ACE2 were increased, effects associated with reduced ERK1/2 phosphorylation, decreased fibrosis and renal protection. <span class="hlt">Ultra-high</span> doses did not influence the ACE2/AT2R/Mas axis and promoted renal injury with increased renal ERK1/2 activation and exaggerated fibronectin expression in db/db mice. Our study demonstrates dose-related effects of candesartan in diabetic nephropathy: intermediate–<span class="hlt">high</span> dose candesartan is renoprotective, whereas <span class="hlt">ultra-high</span> dose candesartan induces renal damage. Molecular processes associated with these effects involve differential modulation of the ACE2/AT2R/Mas axis: intermediate–<span class="hlt">high</span> dose candesartan up-regulating RAS protective components and attenuating pro-fibrotic processes, and <span class="hlt">ultra-high</span> doses having opposite effects. These findings suggest novel mechanisms through the protective RAS axis, whereby candesartan may ameliorate diabetic nephropathy. Our findings also highlight potential injurious renal effects of <span class="hlt">ultra-high</span> dose candesartan in diabetes. PMID:27612496</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26406516','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26406516"><span>Noise analysis for <span class="hlt">CCD</span>-based ultraviolet and visible spectrophotometry.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Davenport, John J; Hodgkinson, Jane; Saffell, John R; Tatam, Ralph P</p> <p>2015-09-20</p> <p>We present the results of a detailed analysis of the noise behavior of two <span class="hlt">CCD</span> spectrometers in common use, an AvaSpec-3648 <span class="hlt">CCD</span> UV spectrometer and an Ocean Optics S2000 Vis spectrometer. Light sources used include a deuterium UV/Vis lamp and UV and visible LEDs. Common noise phenomena include source fluctuation noise, photoresponse nonuniformity, dark current noise, fixed pattern noise, and read noise. These were identified and characterized by varying light source, spectrometer settings, or temperature. A number of noise-limiting techniques are proposed, demonstrating a best-case spectroscopic noise equivalent absorbance of 3.5×10(-4)  AU for the AvaSpec-3648 and 5.6×10(-4)  AU for the Ocean Optics S2000 over a 30 s integration period. These techniques can be used on other <span class="hlt">CCD</span> spectrometers to optimize performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EPJWC..4713001D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EPJWC..4713001D"><span><span class="hlt">High-precision</span> ground-based photometry of exoplanets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Mooij, Ernst J. W.; Jayawardhana, Ray</p> <p>2013-04-01</p> <p><span class="hlt">High-precision</span> photometry of transiting exoplanet systems has contributed significantly to our understanding of the properties of their atmospheres. The best targets are the bright exoplanet systems, for which the <span class="hlt">high</span> number of photons allow very <span class="hlt">high</span> signal-to-noise ratios. Most of the current instruments are not optimised for these <span class="hlt">high-precision</span> measurements, either they have a large read-out overhead to reduce the readnoise and/or their field-of-view is limited, preventing simultaneous observations of both the target and a reference star. Recently we have proposed a new wide-field imager for the Observatoir de Mont-Megantic optimised for these bright systems (PI: Jayawardhana). The instruments has a dual beam design and a field-of-view of 17' by 17'. The cameras have a read-out time of 2 seconds, significantly reducing read-out overheads. Over the past years we have obtained significant experience with how to reach the <span class="hlt">high</span> <span class="hlt">precision</span> required for the characterisation of exoplanet atmospheres. Based on our experience we provide the following advice: <list list-type="order"> <list-item> Get the best calibrations possible. In the case of bad weather, characterise the instrument (e.g. non-linearity, dome flats, bias level), this is vital for better understanding of the science data. </list-item> <list-item> Observe the target for as long as possible, the out-of-transit baseline is as important as the transit/eclipse itself. A short baseline can lead to improperly corrected systematic and mis-estimation of the red-noise. </list-item> <list-item> Keep everything (e.g. position on detector, exposure time) as stable as possible. </list-item> <list-item> Take care that the defocus is not too strong. For a large defocus, the contribution of the total flux from the sky-background in the aperture could well exceed that of the target, resulting in very strict requirements on the <span class="hlt">precision</span> at which the background is measured. </list-item></list></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9684E..0YS','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9684E..0YS"><span>Test technology on divergence angle of laser range finder based on <span class="hlt">CCD</span> imaging fusion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shi, Sheng-bing; Chen, Zhen-xing; Lv, Yao</p> <p>2016-09-01</p> <p>Laser range finder has been equipped with all kinds of weapons, such as tank, ship, plane and so on, is important component of fire control system. Divergence angle is important performance and incarnation of horizontal resolving power for laser range finder, is necessary appraised test item in appraisal test. In this paper, based on <span class="hlt">high</span> accuracy test on divergence angle of laser range finder, divergence angle test system is designed based on <span class="hlt">CCD</span> imaging, divergence angle of laser range finder is acquired through fusion technology for different attenuation imaging, problem that <span class="hlt">CCD</span> characteristic influences divergence angle test is solved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMOS51B1156M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMOS51B1156M"><span>Intermittent carbonate sedimentation in the equatoral Indian Ocean: fluctuations of the Eocene <span class="hlt">CCD</span>?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mitchison, F.; Kachovich, S.; Backman, J.; Pike, J.</p> <p>2017-12-01</p> <p>IODP Expedition 362 recently drilled from the sea floor to oceanic basement in the eastern equatorial Indian Ocean at Site U1480G (3°N, 91°E, water depth 4148 m). Beneath the thick ( 1250 m) predominantly siliciclastic Nicobar Fan succession, a condensed ( 10 m) middle Eocene pelagic interval displayed striking decimetre-scale banding, alternating between calcareous oozes and darker clays. We investigate whether deposition of the calcareous sediments was associated with periodic global carbonate accumulation events previously documented in the Equatorial Pacific and Atlantic Oceans, linked to oscillations of the carbonate compensation depth (<span class="hlt">CCD</span>). We present <span class="hlt">high</span>-resolution geochemical records (carbonate, organic carbon, bulk carbonate stable isotopes) and scanning electron microscope micro-element maps through several of the calcareous to clay transitions, as well as microfossil assemblages and new biostratigraphic constraints for the interval. Our data will reveal whether the banded sediments represent fluctuations of the <span class="hlt">CCD</span>, and whether the <span class="hlt">CCD</span> was likely responding to global (e.g. changes in pCO2) or local (e.g. local changes in calcareous plankton productivity) processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28025130','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28025130"><span><span class="hlt">High</span> and <span class="hlt">ultra-high</span> resolution metabolite mapping of the human brain using 1H FID MRSI at 9.4T.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nassirpour, Sahar; Chang, Paul; Henning, Anke</p> <p>2018-03-01</p> <p>Magnetic resonance spectroscopic imaging (MRSI) is a promising technique for mapping the spatial distribution of multiple metabolites in the human brain. These metabolite maps can be used as a diagnostic tool to gain insight into several biochemical processes and diseases in the brain. In comparison to lower field strengths, MRSI at <span class="hlt">ultra-high</span> field strengths benefits from a higher signal to noise ratio (SNR) as well as higher chemical shift dispersion, and hence spectral resolution. This study combines the benefits of an <span class="hlt">ultra-high</span> field magnet with the advantages of an <span class="hlt">ultra</span>-short TE and TR single-slice FID-MRSI sequence (such as negligible J-evolution and loss of SNR due to T 2 relaxation effects) and presents the first metabolite maps acquired at 9.4T in the healthy human brain at both <span class="hlt">high</span> (voxel size of 97.6µL) and <span class="hlt">ultra-high</span> (voxel size of 24.4µL) spatial resolutions in a scan time of 11 and 46min respectively. In comparison to lower field strengths, more anatomically-detailed maps with higher SNR from a larger number of metabolites are shown. A total of 12 metabolites including glutamate (Glu), glutamine (Gln), N-acetyl-aspartyl-glutamate (NAAG), Gamma-aminobutyric acid (GABA) and glutathione (GSH) are reliably mapped. Comprehensive description of the methodology behind these maps is provided. Copyright © 2016 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070031956&hterms=Silicide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DSilicide','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070031956&hterms=Silicide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DSilicide"><span><span class="hlt">Ultra-High</span> Temperature Materials Characterization for Propulsion Applications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rogers, Jan; Hyers, Robert</p> <p>2007-01-01</p> <p>Propulsion system efficiency increases as operating temperatures are increased. Some very <span class="hlt">high</span>-temperature materials are being developed, including refractory metal alloys, carbides, borides, and silicides. System design requires data for materials properties at operating temperatures. Materials property data are not available for many materials of interest at the desired operating temperatures (up to approx. 3000 K). The objective of this work is to provide important physical property data at <span class="hlt">ultra-high</span> temperatures. The MSFC Electrostatic levitation (ESL) facility can provide measurements of thermophysical properties which include: creep strength, density and thermal expansion for materials being developed for propulsion applications. The ESL facility uses electrostatic fields to position samples between electrodes during processing and characterization studies. Because the samples float between the electrodes during studies, they are free from any contact with a container or test apparatus. This provides a <span class="hlt">high</span> purity environment for the study of <span class="hlt">high</span>-temperature, reactive materials. ESL can be used to process a wide variety of materials including metals, alloys, ceramics, glasses and semiconductors. The MSFC ESL has provided non-contact measurements of properties of materials up to 3400 C. Density and thermal expansion are measured by analyzing digital images of the sample at different temperatures. Our novel, non-contact method for measuring creep uses rapid rotation to deform the sample. Digital images of the deformed samples are analyzed to obtain the creep properties, which match those obtained using ASTM Standard E-139 for Nb at 1985 C. Data from selected ESL-based characterization studies will be presented. The ESL technique could support numerous propulsion technologies by advancing the knowledge base and the technology readiness level for <span class="hlt">ultra-high</span> temperature materials. Applications include non-eroding nozzle materials and lightweight, <span class="hlt">high</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23076877','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23076877"><span><span class="hlt">Ultra</span> <span class="hlt">high</span> spatial and temporal resolution breast imaging at 7T.</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 Bank, B L; Voogt, I J; Italiaander, M; Stehouwer, B L; Boer, V O; Luijten, P R; Klomp, D W J</p> <p>2013-04-01</p> <p>There is a need to obtain higher specificity in the detection of breast lesions using MRI. To address this need, Dynamic Contrast-Enhanced (DCE) MRI has been combined with other structural and functional MRI techniques. Unfortunately, owing to time constraints structural images at <span class="hlt">ultra-high</span> spatial resolution can generally not be obtained during contrast uptake, whereas the relatively low spatial resolution of functional imaging (e.g. diffusion and perfusion) limits the detection of small lesions. To be able to increase spatial as well as temporal resolution simultaneously, the sensitivity of MR detection needs to increase as well as the ability to effectively accelerate the acquisition. The required gain in signal-to-noise ratio (SNR) can be obtained at 7T, whereas acceleration can be obtained with <span class="hlt">high</span>-density receiver coil arrays. In this case, morphological imaging can be merged with DCE-MRI, and other functional techniques can be obtained at higher spatial resolution, and with less distortion [e.g. Diffusion Weighted Imaging (DWI)]. To test the feasibility of this concept, we developed a unilateral breast coil for 7T. It comprises a volume optimized dual-channel transmit coil combined with a 30-channel receive array coil. The <span class="hlt">high</span> density of small coil elements enabled efficient acceleration in any direction to acquire <span class="hlt">ultra</span> <span class="hlt">high</span> spatial resolution MRI of close to 0.6 mm isotropic detail within a temporal resolution of 69 s, <span class="hlt">high</span> spatial resolution MRI of 1.5 mm isotropic within an <span class="hlt">ultra</span> <span class="hlt">high</span> temporal resolution of 6.7 s and low distortion DWI at 7T, all validated in phantoms, healthy volunteers and a patient with a lesion in the right breast classified as Breast Imaging Reporting and Data System (BI-RADS) IV. Copyright © 2012 John Wiley & Sons, Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SPIE.7536E..03D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SPIE.7536E..03D"><span>Improved sensitivity <span class="hlt">high</span>-definition interline <span class="hlt">CCD</span> using the KODAK TRUESENSE color filter pattern</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>DiBella, James; Andreghetti, Marco; Enge, Amy; Chen, William; Stanka, Timothy; Kaser, Robert</p> <p>2010-01-01</p> <p>The KODAK TRUESENSE Color Filter Pattern has technology that for the first time is applied to a commercially available interline <span class="hlt">CCD</span>. This 2/3" true-HD sensor will be described along with its performance attributes, including sensitivity improvement as compared to the Bayer CFA version of the same sensor. In addition, an overview of the system developed for demonstration and evaluation will be provided. Examples of the benefits of the new technology in specific applications including surveillance and intelligent traffic systems will be 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_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('https://www.ncbi.nlm.nih.gov/pubmed/26480197','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26480197"><span><span class="hlt">Ultra</span>-wide-range measurements of thin-film filter optical density over the visible and near-infrared spectrum.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lequime, Michel; Liukaityte, Simona; Zerrad, Myriam; Amra, Claude</p> <p>2015-10-05</p> <p>We present the improved structure and operating principle of a spectrophotometric mean that allows us for the recording of the transmittance of a thin-film filter over an <span class="hlt">ultra</span>-wide range of optical densities (from 0 to 11) between 400 and 1000 nm. The operation of this apparatus is based on the combined use of a <span class="hlt">high</span> power supercontinuum laser source, a tunable volume hologram filter, a standard monochromator and a scientific grade <span class="hlt">CCD</span> camera. The experimentally recorded noise floor is in good accordance with the optical density values given by the theoretical approach. A demonstration of the sensitivity gain provided by this new set-up with respect to standard spectrophotometric means is performed via the characterization of various types of filters (band-pass, long-pass, short-pass, and notch).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29461018','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29461018"><span>Analysis of new psychoactive substances in human urine by <span class="hlt">ultra-high</span> performance supercritical fluid and liquid chromatography: Validation and comparison.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Borovcová, Lucie; Pauk, Volodymyr; Lemr, Karel</p> <p>2018-05-01</p> <p>New psychoactive substances represent serious social and health problem as tens of new compounds are detected in Europe annually. They often show structural proximity or even isomerism, which complicates their analysis. Two methods based on <span class="hlt">ultra</span> <span class="hlt">high</span> performance supercritical fluid chromatography and <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography with mass spectrometric detection were validated and compared. A simple dilute-filter-and-shoot protocol utilizing propan-2-ol or methanol for supercritical fluid or liquid chromatography, respectively, was proposed to detect and quantify 15 cathinones and phenethylamines in human urine. Both methods offered fast separation (<3 min) and short total analysis time. <span class="hlt">Precision</span> was well <15% with a few exceptions in liquid chromatography. Limits of detection in urine ranged from 0.01 to 2.3 ng/mL, except for cathinone (5 ng/mL) in supercritical fluid chromatography. Nevertheless, this technique distinguished all analytes including four pairs of isomers, while liquid chromatography was unable to resolve fluoromethcathinone regioisomers. Concerning matrix effects and recoveries, supercritical fluid chromatography produced more uniform results for different compounds and at different concentration levels. This work demonstrates the performance and reliability of supercritical fluid chromatography and corroborates its applicability as an alternative tool for analysis of new psychoactive substances in biological matrixes. © 2018 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010LPICo1538.5289V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010LPICo1538.5289V"><span>Structural Analysis of Titan's Tholins by <span class="hlt">Ultra-High</span> Resolution Mass Spectrometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vuitton, V.; Frisari, M.; Thissen, R.; Dutuit, O.; Bonnet, J.-Y.; Quirico, E.; Sciamma O'Brien, E.; Szopa, C.; Carrasco, N.; Somogyi, A.; Smith, M.; Hörst, S. M.; Yelle, R.</p> <p>2010-04-01</p> <p>We propose here a systematic <span class="hlt">ultra-high</span> resolution mass spectrometry and MS/MS study in order to provide a more coherent and complete characterization of the structure of the molecules making up the soluble fraction of the Titan tholins.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhCS.734c2097H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhCS.734c2097H"><span>The Bendability of <span class="hlt">Ultra</span> <span class="hlt">High</span> strength Steels</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hazra, S. K.; Efthymiadis, P.; Alamoudi, A.; Kumar, R. L. V.; Shollock, B.; Dashwood, R.</p> <p>2016-08-01</p> <p>Automotive manufacturers have been reducing the weight of their vehicles to meet increasingly stringent environmental legislation that reflects public demand. A strategy is to use higher strength materials for parts with reduced cross-sections. However, such materials are less formable than traditional grades. The frequent result is increased processing and piece costs. 3D roll forming is a novel and flexible process: it is estimated that a quarter of the structure of a vehicle can be made with a single set of tooling. Unlike stamping, this process requires material with low work hardening rates. In this paper, we present results of <span class="hlt">ultra</span> <span class="hlt">high</span> strength steels that have low elongation in a tension but display <span class="hlt">high</span> formability in bending through the suppression of the necking response.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20697439','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20697439"><span>Spatial resolution of a hard x-ray <span class="hlt">CCD</span> detector.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Seely, John F; Pereira, Nino R; Weber, Bruce V; Schumer, Joseph W; Apruzese, John P; Hudson, Lawrence T; Szabo, Csilla I; Boyer, Craig N; Skirlo, Scott</p> <p>2010-08-10</p> <p>The spatial resolution of an x-ray <span class="hlt">CCD</span> detector was determined from the widths of the tungsten x-ray lines in the spectrum formed by a crystal spectrometer in the 58 to 70 keV energy range. The detector had 20 microm pixel, 1700 by 1200 pixel format, and a CsI x-ray conversion scintillator. The spectral lines from a megavolt x-ray generator were focused on the spectrometer's Rowland circle by a curved transmission crystal. The line shapes were Lorentzian with an average width after removal of the natural and instrumental line widths of 95 microm (4.75 pixels). A <span class="hlt">high</span> spatial frequency background, primarily resulting from scattered gamma rays, was removed from the spectral image by Fourier analysis. The spectral lines, having low spatial frequency in the direction perpendicular to the dispersion, were enhanced by partially removing the Lorentzian line shape and by fitting Lorentzian curves to broad unresolved spectral features. This demonstrates the ability to improve the spectral resolution of hard x-ray spectra that are recorded by a <span class="hlt">CCD</span> detector with well-characterized intrinsic spatial resolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22687404','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22687404"><span>Development of a <span class="hlt">highly</span> sensitive methodology for quantitative determination of fexofenadine in a microdose study by multiple injection method using <span class="hlt">ultra-high</span> performance liquid chromatography with tandem mass spectrometry.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tanaka, Yukari; Yoshikawa, Yutaka; Yasui, Hiroyuki</p> <p>2012-01-01</p> <p>An <span class="hlt">ultra</span> <span class="hlt">high</span>-sensitivity method for quantifying fexofenadine concentration in rat plasma samples by multiple injection method (MIM) was developed for a microdose study. In this study, MIM involved continuous injections of multiple samples containing the single compound into a column of the <span class="hlt">ultra</span>-HPLC (UHPLC) system, and then, temporary trapping of the analyte at the column head. This was followed by elution of the compound from the column and detection by mass spectrometer. Fexofenadine, used as a model compound in this study, was extracted from the plasma samples by a protein precipitation method. Chromatographic separation was achieved on a reversed-phase C18 column by using a gradient method with 0.1% formic acid and 0.1% formic acid in acetonitrile as the mobile phase. The analyte was quantified in the positive-ion electrospray ionization mode using selected reaction monitoring. In this study, the analytical time per fexofenadine sample was approximately 2 min according to the UHPLC system. The method exhibited the linear dynamic ranges of 5-5000 pg/mL for fexofenadine in rat plasma. The intra-day <span class="hlt">precisions</span> were from 3.2 to 8.7% and the accuracy range was 95.2-99.3%. The inter-day <span class="hlt">precisions</span> and accuracies ranged from 3.5 to 8.4% and from 98.6 to 102.6%, respectively. The validated MIM was successfully applied to a microdose study in the rats that received oral administration of 100 µg/kg fexofenadine. We suggest that this method might be beneficial for the quantification of fexofenadine concentrations in a microdose clinical study.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29565775','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29565775"><span>The Natural-<span class="hlt">CCD</span> Algorithm, a Novel Method to Solve the Inverse Kinematics of Hyper-redundant and Soft Robots.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Martín, Andrés; Barrientos, Antonio; Del Cerro, Jaime</p> <p>2018-03-22</p> <p>This article presents a new method to solve the inverse kinematics problem of hyper-redundant and soft manipulators. From an engineering perspective, this kind of robots are underdetermined systems. Therefore, they exhibit an infinite number of solutions for the inverse kinematics problem, and to choose the best one can be a great challenge. A new algorithm based on the cyclic coordinate descent (<span class="hlt">CCD</span>) and named as natural-<span class="hlt">CCD</span> is proposed to solve this issue. It takes its name as a result of generating very harmonious robot movements and trajectories that also appear in nature, such as the golden spiral. In addition, it has been applied to perform continuous trajectories, to develop whole-body movements, to analyze motion planning in complex environments, and to study fault tolerance, even for both prismatic and rotational joints. The proposed algorithm is very simple, <span class="hlt">precise</span>, and computationally efficient. It works for robots either in two or three spatial dimensions and handles a large amount of degrees-of-freedom. Because of this, it is aimed to break down barriers between discrete hyper-redundant and continuum soft robots.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/35955','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/35955"><span>Development of Non-Proprietary <span class="hlt">Ultra-High</span> Performance Concrete : Research Topic Statement</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2014-05-29</p> <p><span class="hlt">Ultra-high</span> performance concrete became commercially available in the U.S. in 2000. Since then, UHPC has been actively promoted by the Federal Highway Administration. UHPC has mostly been used in the U.S. for field-cast connections of prefabricated br...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22591733-ionic-liquid-gating-atomic-layer-deposition-passivated-gan-ultra-high-electron-density-induced-high-drain-current-low-contact-resistance','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22591733-ionic-liquid-gating-atomic-layer-deposition-passivated-gan-ultra-high-electron-density-induced-high-drain-current-low-contact-resistance"><span>Ionic liquid gating on atomic layer deposition passivated GaN: <span class="hlt">Ultra-high</span> electron density induced <span class="hlt">high</span> drain current and low contact resistance</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>Zhou, Hong; Du, Yuchen; Ye, Peide D., E-mail: yep@purdue.edu</p> <p>2016-05-16</p> <p>Herein, we report on achieving <span class="hlt">ultra-high</span> electron density (exceeding 10{sup 14 }cm{sup −2}) in a GaN bulk material device by ionic liquid gating, through the application of atomic layer deposition (ALD) of Al{sub 2}O{sub 3} to passivate the GaN surface. Output characteristics demonstrate a maximum drain current of 1.47 A/mm, the highest reported among all bulk GaN field-effect transistors, with an on/off ratio of 10{sup 5} at room temperature. An <span class="hlt">ultra-high</span> electron density exceeding 10{sup 14 }cm{sup −2} accumulated at the surface is confirmed via Hall-effect measurement and transfer length measurement. In addition to the <span class="hlt">ultra-high</span> electron density, we also observe a reductionmore » of the contact resistance due to the narrowing of the Schottky barrier width on the contacts. Taking advantage of the ALD surface passivation and ionic liquid gating technique, this work provides a route to study the field-effect and carrier transport properties of conventional semiconductors in unprecedented <span class="hlt">ultra-high</span> charge density regions.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1176157','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1176157"><span><span class="hlt">High</span> <span class="hlt">precision</span>, rapid laser hole drilling</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Chang, Jim J.; Friedman, Herbert W.; Comaskey, Brian J.</p> <p>2007-03-20</p> <p>A laser system produces a first laser beam for rapidly removing the bulk of material in an area to form a ragged hole. The laser system produces a second laser beam for accurately cleaning up the ragged hole so that the final hole has dimensions of <span class="hlt">high</span> <span class="hlt">precision</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1175264','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1175264"><span><span class="hlt">High</span> <span class="hlt">precision</span>, rapid laser hole drilling</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Chang, Jim J.; Friedman, Herbert W.; Comaskey, Brian J.</p> <p>2005-03-08</p> <p>A laser system produces a first laser beam for rapidly removing the bulk of material in an area to form a ragged hole. The laser system produces a second laser beam for accurately cleaning up the ragged hole so that the final hole has dimensions of <span class="hlt">high</span> <span class="hlt">precision</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1083908','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1083908"><span><span class="hlt">High</span> <span class="hlt">precision</span>, rapid laser hole drilling</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Chang, Jim J.; Friedman, Herbert W.; Comaskey, Brian J.</p> <p>2013-04-02</p> <p>A laser system produces a first laser beam for rapidly removing the bulk of material in an area to form a ragged hole. The laser system produces a second laser beam for accurately cleaning up the ragged hole so that the final hole has dimensions of <span class="hlt">high</span> <span class="hlt">precision</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1992NuPhS..28..123Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1992NuPhS..28..123Y"><span>A swimming pool array for <span class="hlt">ultra</span> <span class="hlt">high</span> energy showers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yodh, Gaurang B.; Shoup, Anthony; Barwick, Steve; Goodman, Jordan A.</p> <p>1992-11-01</p> <p>A very preliminary design concept for an array using water Cherenkov counters, built out of commercially available backyard swimming pools, to sample the electromagnetic and muonic components of <span class="hlt">ultra</span> <span class="hlt">high</span> energy showers at large lateral distances is presented. The expected performance of the pools is estimated using the observed lateral distributions by scintillator and water Cherenkov arrays at energies above 1019 eV and simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017RScI...88b3702S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017RScI...88b3702S"><span>Development of X-ray <span class="hlt">CCD</span> camera based X-ray micro-CT system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sarkar, Partha S.; Ray, N. K.; Pal, Manoj K.; Baribaddala, Ravi; Agrawal, Ashish; Kashyap, Y.; Sinha, A.; Gadkari, S. C.</p> <p>2017-02-01</p> <p>Availability of microfocus X-ray sources and <span class="hlt">high</span> resolution X-ray area detectors has made it possible for <span class="hlt">high</span> resolution microtomography studies to be performed outside the purview of synchrotron. In this paper, we present the work towards the use of an external shutter on a <span class="hlt">high</span> resolution microtomography system using X-ray <span class="hlt">CCD</span> camera as a detector. During micro computed tomography experiments, the X-ray source is continuously ON and owing to the readout mechanism of the <span class="hlt">CCD</span> detector electronics, the detector registers photons reaching it during the read-out period too. This introduces a shadow like pattern in the image known as smear whose direction is defined by the vertical shift register. To resolve this issue, the developed system has been incorporated with a synchronized shutter just in front of the X-ray source. This is positioned in the X-ray beam path during the image readout period and out of the beam path during the image acquisition period. This technique has resulted in improved data quality and hence the same is reflected in the reconstructed images.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4232278','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4232278"><span>Generation of a large volume of clinically relevant nanometre-sized <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles for cell culture studies</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ingham, Eileen; Fisher, John; Tipper, Joanne L</p> <p>2014-01-01</p> <p>It has recently been shown that the wear of <span class="hlt">ultra-high</span>-molecular-weight polyethylene in hip and knee prostheses leads to the generation of nanometre-sized particles, in addition to micron-sized particles. The biological activity of nanometre-sized <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles has not, however, previously been studied due to difficulties in generating sufficient volumes of nanometre-sized <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles suitable for cell culture studies. In this study, wear simulation methods were investigated to generate a large volume of endotoxin-free clinically relevant nanometre-sized <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles. Both single-station and six-station multidirectional pin-on-plate wear simulators were used to generate <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles under sterile and non-sterile conditions. Microbial contamination and endotoxin levels in the lubricants were determined. The results indicated that microbial contamination was absent and endotoxin levels were low and within acceptable limits for the pharmaceutical industry, when a six-station pin-on-plate wear simulator was used to generate <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles in a non-sterile environment. Different pore-sized polycarbonate filters were investigated to isolate nanometre-sized <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles from the wear test lubricants. The use of the filter sequence of 10, 1, 0.1, 0.1 and 0.015 µm pore sizes allowed successful isolation of <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles with a size range of < 100 nm, which was suitable for cell culture studies. PMID:24658586</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24658586','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24658586"><span>Generation of a large volume of clinically relevant nanometre-sized <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles for cell culture studies.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Aiqin; Ingham, Eileen; Fisher, John; Tipper, Joanne L</p> <p>2014-04-01</p> <p>It has recently been shown that the wear of <span class="hlt">ultra-high</span>-molecular-weight polyethylene in hip and knee prostheses leads to the generation of nanometre-sized particles, in addition to micron-sized particles. The biological activity of nanometre-sized <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles has not, however, previously been studied due to difficulties in generating sufficient volumes of nanometre-sized <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles suitable for cell culture studies. In this study, wear simulation methods were investigated to generate a large volume of endotoxin-free clinically relevant nanometre-sized <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles. Both single-station and six-station multidirectional pin-on-plate wear simulators were used to generate <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles under sterile and non-sterile conditions. Microbial contamination and endotoxin levels in the lubricants were determined. The results indicated that microbial contamination was absent and endotoxin levels were low and within acceptable limits for the pharmaceutical industry, when a six-station pin-on-plate wear simulator was used to generate <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles in a non-sterile environment. Different pore-sized polycarbonate filters were investigated to isolate nanometre-sized <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles from the wear test lubricants. The use of the filter sequence of 10, 1, 0.1, 0.1 and 0.015 µm pore sizes allowed successful isolation of <span class="hlt">ultra-high</span>-molecular-weight polyethylene wear particles with a size range of < 100 nm, which was suitable for cell culture studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19760023333','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19760023333"><span>Solid state, <span class="hlt">CCD</span>-buried channel, television camera study and design</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hoagland, K. A.; Balopole, H.</p> <p>1976-01-01</p> <p>An investigation of an all solid state television camera design, which uses a buried channel charge-coupled device (<span class="hlt">CCD</span>) as the image sensor, was undertaken. A 380 x 488 element <span class="hlt">CCD</span> array was utilized to ensure compatibility with 525 line transmission and display monitor equipment. Specific camera design approaches selected for study and analysis included (a) optional clocking modes for either fast (1/60 second) or normal (1/30 second) frame readout, (b) techniques for the elimination or suppression of <span class="hlt">CCD</span> blemish effects, and (c) automatic light control and video gain control techniques to eliminate or minimize sensor overload due to bright objects in the scene. Preferred approaches were determined and integrated into a design which addresses the program requirements for a deliverable solid state TV camera.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9077E..08P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9077E..08P"><span>Design and performance of an <span class="hlt">ultra</span>-wideband stepped-frequency radar with <span class="hlt">precise</span> frequency control for landmine and IED detection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Phelan, Brian R.; Sherbondy, Kelly D.; Ranney, Kenneth I.; Narayanan, Ram M.</p> <p>2014-05-01</p> <p>The Army Research Laboratory (ARL) has developed an impulse-based vehicle-mounted forward-looking <span class="hlt">ultra</span>- wideband (UWB) radar for imaging buried landmines and improvised explosive devices (IEDs). However, there is no control of the radiated spectrum in this system. As part of ARL's Partnerships in Research Transition (PIRT) program, the above deficiency is addressed by the design of a Stepped-Frequency Radar (SFR) which allows for <span class="hlt">precise</span> control over the radiated spectrum, while still maintaining an effective <span class="hlt">ultra</span>-wide bandwidth. The SFR utilizes a frequency synthesizer which can be configured to excise prohibited and interfering frequency bands and also implement frequency-hopping capabilities. The SFR is designed to be a forward-looking ground- penetrating (FLGPR) Radar utilizing a uniform linear array of sixteen (16) Vivaldi notch receive antennas and two (2) Quad-ridge horn transmit antennas. While a preliminary SFR consisting of four (4) receive channels has been designed, this paper describes major improvements to the system, and an analysis of expected system performance. The 4-channel system will be used to validate the SFR design which will eventually be augmented in to the full 16-channel system. The SFR has an operating frequency band which ranges from 300 - 2000 MHz, and a minimum frequency step-size of 1 MHz. The radar system is capable of illuminating range swaths that have maximum extents of 30 to 150 meters (programmable). The transmitter has the ability to produce approximately -2 dBm/MHz average power over the entire operating frequency range. The SFR will be used to determine the practicality of detecting and classifying buried and concealed landmines and IEDs from safe stand-off distances.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014sptz.prop11016C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014sptz.prop11016C"><span>SMUVS: Spitzer Matching survey of the <span class="hlt">Ultra</span>VISTA <span class="hlt">ultra</span>-deep Stripes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Caputi, Karina; Ashby, Matthew; Fazio, Giovanni; Huang, Jiasheng; Dunlop, James; Franx, Marijn; Le Fevre, Olivier; Fynbo, Johan; McCracken, Henry; Milvang-Jensen, Bo; Muzzin, Adam; Ilbert, Olivier; Somerville, Rachel; Wechsler, Risa; Behroozi, Peter; Lu, Yu</p> <p>2014-12-01</p> <p>We request 2026.5 hours to homogenize the matching <span class="hlt">ultra</span>-deep IRAC data of the <span class="hlt">Ultra</span>VISTA <span class="hlt">ultra</span>-deep stripes, producing a final area of ~0.6 square degrees with the deepest near- and mid-IR coverage existing in any such large area of the sky (H, Ks, [3.6], [4.5] ~ 25.3-26.1 AB mag; 5 sigma). The <span class="hlt">Ultra</span>VISTA <span class="hlt">ultra</span>-deep stripes are contained within the larger COSMOS field, which has a rich collection of multi-wavelength, ancillary data, making it ideal to study different aspects of galaxy evolution with <span class="hlt">high</span> statistical significance and excellent redshift accuracy. The <span class="hlt">Ultra</span>VISTA <span class="hlt">ultra</span>-deep stripes are the region of the COSMOS field where these studies can be pushed to the highest redshifts, but securely identifying <span class="hlt">high</span>-z galaxies, and determining their stellar masses, will only be possible if <span class="hlt">ultra</span>-deep mid-IR data are available. Our IRAC observations will allow us to: 1) extend the galaxy stellar mass function at redshifts z=3 to z=5 to the intermediate mass regime (M~5x10^9-10^10 Msun), which is critical to constrain galaxy formation models; 2) gain a factor of six in the area where it is possible to effectively search for z>=6 galaxies and study their properties; 3) measure, for the first time, the large-scale structure traced by an unbiased galaxy sample at z=5 to z=7, and make the link to their host dark matter haloes. This cannot be done in any other field of the sky, as the <span class="hlt">Ultra</span>VISTA <span class="hlt">ultra</span>-deep stripes form a quasi-contiguous, regular-shape field, which has a unique combination of large area and photometric depth. 4) provide a unique resource for the selection of secure z>5 targets for JWST and ALMA follow up. Our observations will have an enormous legacy value which amply justifies this new observing-time investment in the COSMOS field. Spitzer cannot miss this unique opportunity to open up a large 0.6 square-degree window to the early Universe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.ars.usda.gov/research/publications/publication/?seqNo115=291048','TEKTRAN'); return false;" href="http://www.ars.usda.gov/research/publications/publication/?seqNo115=291048"><span>Case study: dairies utilizing <span class="hlt">ultra-high</span> stock density grazing in the Northeast</span></a></p> <p><a target="_blank" href="https://www.ars.usda.gov/research/publications/find-a-publication/">USDA-ARS?s Scientific Manuscript database</a></p> <p></p> <p></p> <p><span class="hlt">Ultra-high</span> stock density (UHSD) grazing has gained interest in the forage industry. However, little credible research exists to support anecdotal claims that forage and soil improvement occur through trampling <span class="hlt">high</span> proportions (75+%) of mature forage into the soil by grazing dense groups of cattle o...</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_21 --> <div id="page_22" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="421"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29092494','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29092494"><span><span class="hlt">High-precision</span> multi-node clock network distribution.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Xing; Cui, Yifan; Lu, Xing; Ci, Cheng; Zhang, Xuesong; Liu, Bo; Wu, Hong; Tang, Tingsong; Shi, Kebin; Zhang, Zhigang</p> <p>2017-10-01</p> <p>A <span class="hlt">high</span> <span class="hlt">precision</span> multi-node clock network for multiple users was built following the <span class="hlt">precise</span> frequency transmission and time synchronization of 120 km fiber. The network topology adopts a simple star-shaped network structure. The clock signal of a hydrogen maser (synchronized with UTC) was recovered from a 120 km telecommunication fiber link and then was distributed to 4 sub-stations. The fractional frequency instability of all substations is in the level of 10 -15 in a second and the clock offset instability is in sub-ps in root-mean-square average.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9915E..21B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9915E..21B"><span>ESA's <span class="hlt">CCD</span> test bench for the PLATO mission</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Beaufort, Thierry; Duvet, Ludovic; Bloemmaert, Sander; Lemmel, Frederic; Prod'homme, Thibaut; Verhoeve, Peter; Smit, Hans; Butler, Bart; van der Luijt, Cornelis; Heijnen, Jerko; Visser, Ivo</p> <p>2016-08-01</p> <p>PLATO { PLAnetary Transits and Oscillations of stars { is the third medium-class mission to be selected in the European Space Agency (ESA) Science and Robotic Exploration Cosmic Vision programme. Due for launch in 2025, the payload makes use of a large format (8 cm x 8 cm) Charge-Coupled Devices (CCDs), the e2v <span class="hlt">CCD</span>270 operated at 4 MHz and at -70 C. To de-risk the PLATO <span class="hlt">CCD</span> qualification programme initiated in 2014 and support the mission definition process, ESA's Payload Technology Validation section from the Future Missions Office has developed a dedicated test bench.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013mss..confEMG07H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013mss..confEMG07H"><span><span class="hlt">High</span> <span class="hlt">Precision</span> Spectroscopy of CH_5^+ Using Nice-Ohvms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hodges, James N.; Perry, Adam J.; McCall, Benjamin J.</p> <p>2013-06-01</p> <p>The elusive methonium ion, CH_5^+, is of great interest due to its <span class="hlt">highly</span> fluxional nature. The only published <span class="hlt">high</span>-resolution infrared spectrum remains completely unassigned to this date. The primary challenge in understanding the CH_5^+ spectrum is that traditional spectroscopic approaches rely on a molecule having only small (or even large) amplitude motions about a well-defined reference geometry, and this is not the case with CH_5^+. We are in the process of re-scanning Oka's spectrum, in the original Black Widow discharge cell, using the new technique of Noise Immune Cavity Enhanced Optical Heterodyne Velocity Modulation Spectroscopy (NICE-OHVMS). The <span class="hlt">high</span> <span class="hlt">precision</span> afforded by optical saturation in conjunction with a frequency comb allows transition line centers to be determined with sub-MHz accuracy and <span class="hlt">precision</span> -- a substantial improvement over the 90 MHz <span class="hlt">precision</span> of Oka's work. With a <span class="hlt">high-precision</span> linelist in hand, we plan to search for four line combination differences to directly determine the spacings between rotational energy levels. Such a search is currently infeasible due to the large number of false positives resulting from the relatively low <span class="hlt">precision</span> and <span class="hlt">high</span> spectral density of Oka's spectrum. The resulting combination differences, in conjunction with state-of-the-art theoretical calculations from Tucker Carrington, may provide the first insight into the rotational structure of this unique molecular system. E. T. White, J. Tang, T. Oka, Science (1999) 284, 135--137. B. M. Siller, et al. Opt. Express (2011), 19, 24822--24827. K. N. Crabtree, et al. Chem. Phys. Lett. (2012), 551, 1--6. X. Wang, T. Carrington, J. Chem. Phys., (2008), 129, 234102.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9685E..0LY','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9685E..0LY"><span><span class="hlt">High</span> <span class="hlt">precision</span> locating control system based on VCM for Talbot lithography</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yao, Jingwei; Zhao, Lixin; Deng, Qian; Hu, Song</p> <p>2016-10-01</p> <p>Aiming at the <span class="hlt">high</span> <span class="hlt">precision</span> and efficiency requirements of Z-direction locating in Talbot lithography, a control system based on Voice Coil Motor (VCM) was designed. In this paper, we built a math model of VCM and its moving characteristic was analyzed. A double-closed loop control strategy including position loop and current loop were accomplished. The current loop was implemented by driver, in order to achieve the rapid follow of the system current. The position loop was completed by the digital signal processor (DSP) and the position feedback was achieved by <span class="hlt">high</span> <span class="hlt">precision</span> linear scales. Feed forward control and position feedback Proportion Integration Differentiation (PID) control were applied in order to compensate for dynamic lag and improve the response speed of the system. And the <span class="hlt">high</span> <span class="hlt">precision</span> and efficiency of the system were verified by simulation and experiments. The results demonstrated that the performance of Z-direction gantry was obviously improved, having <span class="hlt">high</span> <span class="hlt">precision</span>, quick responses, strong real-time and easily to expend for higher <span class="hlt">precision</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110011696','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110011696"><span><span class="hlt">Precision</span> Continuum Receivers for Astrophysical Applications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wollack, Edward J.</p> <p>2011-01-01</p> <p>Cryogenically cooled HEMT (<span class="hlt">High</span> Electron Mobility Transistor) amplifiers find widespread use in radioastronomy receivers. In recent years, these devices have also been commonly employed in broadband receivers for <span class="hlt">precision</span> measurements of the Cosmic Microwave Background (CMB) radiation. In this setting, the combination of <span class="hlt">ultra</span>-low-noise and low-spectral-resolution observations reinforce the importance achieving suitable control over the device environment to achieve fundamentally limited receiver performance. The influence of the intrinsic amplifier stability at low frequencies on data quality (e.g., achievable noise and residual temporal correlations), observational and calibration strategies, as well as architectural mitigation approaches in this setting will be discussed. The implications of device level 1/f fluctuations reported in the literature on system performance will be reviewed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20174119','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20174119"><span>Controlled nanostructrures formation by <span class="hlt">ultra</span> fast laser pulses for color marking.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dusser, B; Sagan, Z; Soder, H; Faure, N; Colombier, J P; Jourlin, M; Audouard, E</p> <p>2010-02-01</p> <p><span class="hlt">Precise</span> nanostructuration of surface and the subsequent upgrades in material properties is a strong outcome of <span class="hlt">ultra</span> fast laser irradiations. Material characteristics can be designed on mesoscopic scales, carrying new optical properties. We demonstrate in this work, the possibility of achieving material modifications using <span class="hlt">ultra</span> short pulses, via polarization dependent structures generation, that can generate specific color patterns. These oriented nanostructures created on the metal surface, called ripples, are typically smaller than the laser wavelength and in the range of visible spectrum. In this way, a complex colorization process of the material, involving imprinting, calibration and reading, has been performed to associate a priori defined colors. This new method based on the control of the laser-driven nanostructure orientation allows cumulating <span class="hlt">high</span> quantity of information in a minimal surface, proposing new applications for laser marking and new types of identifying codes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008SPIE.7156E..1KZ','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008SPIE.7156E..1KZ"><span>Research of optical coherence tomography microscope based on <span class="hlt">CCD</span> detector</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Hua; Xu, Zhongbao; Zhang, Shuomo</p> <p>2008-12-01</p> <p>The reference wave phase was modulated with a sinusoidal vibrating mirror attached to a Piezoelectric Transducer (PZT), the integration was performed by a <span class="hlt">CCD</span>, and the charge storage period of the <span class="hlt">CCD</span> image sensor was one-quarter period of the sinusoidal phase modulation. With the frequency- synchronous detection technique, four images (four frames of interference pattern) were recorded during one period of the phase modulation. In order to obtain the optimum modulation parameter, the values of amplitude and phase of the sinusoidal phase modulation were determined by considering the measurement error caused by the additive noise contained in the detected values. The PZT oscillation was controlled by a closed loop control system based on PID controller. An ideal discrete digital sine function at 50Hz with adjustable amplitude was used to adjust the vibrating of PZT, and a digital phase shift techniques was used to adjust vibrating phase of PZT so that the phase of the modulation could reach their optimum values. The <span class="hlt">CCD</span> detector was triggered with software at 200Hz. Based on work above a small coherent signal masked by the preponderant incoherent background with a <span class="hlt">CCD</span> detector was obtained.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27003466','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27003466"><span><span class="hlt">Ultra</span>-flexible nanocarriers for enhanced topical delivery of a <span class="hlt">highly</span> lipophilic antioxidative molecule for skin cancer chemoprevention.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Boakye, Cedar H A; Patel, Ketan; Doddapaneni, Ravi; Bagde, Arvind; Behl, Gautam; Chowdhury, Nusrat; Safe, Stephen; Singh, Mandip</p> <p>2016-07-01</p> <p>In this study, we developed cationic <span class="hlt">ultra</span>-flexible nanocarriers (<span class="hlt">Ultra</span>FLEX-Nano) to surmount the skin barrier structure and to potentiate the topical delivery of a <span class="hlt">highly</span> lipophilic antioxidative diindolylmethane derivative (DIM-D) for the inhibition of UV-induced DNA damage and skin carcinogenesis. <span class="hlt">Ultra</span>FLEX-Nano was prepared with 1,2-dipalmitoyl-sn-glycero-3-phosphocholine, 1,2-dioleoyl-3-trimethylammonium-propane, cholesterol and tween-80 by ethanolic injection method; was characterized by Differential Scanning Calorimetric (DSC), Fourier Transform Infrared (FT-IR) and Atomic Force Microscopic (phase-imaging) analyses and permeation studies were performed in dermatomed human skin. The efficacy of DIM-D-<span class="hlt">Ultra</span>FLEX-Nano for skin cancer chemoprevention was evaluated in UVB-induced skin cancer model in vivo. DIM-D-<span class="hlt">Ultra</span>FLEX-Nano formed a stable mono-dispersion (110.50±0.71nm) with >90% encapsulation of DIM-D that was supported by HPLC, DSC, FT-IR and AFM phase imaging. The blank formulation was non-toxic to human embryonic kidney cells. <span class="hlt">Ultra</span>FLEX-Nano was vastly deformable and <span class="hlt">highly</span> permeable across the stratum corneum; there was significant (p<0.01) skin deposition of DIM-D for <span class="hlt">Ultra</span>FLEX-Nano that was superior to PEG solution (13.83-fold). DIM-D-<span class="hlt">Ultra</span>FLEX-Nano pretreatment delayed the onset of UVB-induced tumorigenesis (2 weeks) and reduced (p<0.05) the number of tumors observed in SKH-1 mice (3.33-fold), which was comparable to pretreatment with sunscreen (SPF30). Also, DIM-D-<span class="hlt">Ultra</span>FLEX-Nano caused decrease (p<0.05) in UV-induced DNA damage (8-hydroxydeoxyguanosine), skin inflammation (PCNA), epidermal hyperplasia (c-myc, CyclinD1), immunosuppression (IL10), cell survival (AKT), metastasis (Vimentin, MMP-9, TIMP1) but increase in apoptosis (p53 and p21). <span class="hlt">Ultra</span>FLEX-Nano was efficient in enhancing the topical delivery of DIM-D. DIM-D-<span class="hlt">Ultra</span>FLEX-Nano was efficacious in delaying skin tumor incidence and multiplicity in SKH mice comparable to sunscreen (SPF30</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997SPIE.3032..131S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997SPIE.3032..131S"><span>DQE analysis for <span class="hlt">CCD</span> imaging arrays</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shaw, Rodney</p> <p>1997-05-01</p> <p>By consideration of the statistical interaction between exposure quanta and the mechanisms of image detection, the signal-to-noise limitations of a variety of image acquisition technologies are now well understood. However in spite of the growing fields of application for <span class="hlt">CCD</span> imaging- arrays and the obvious advantages of their multi-level mode of quantum detection, only limited and largely empirical approaches have been made to quantify these advantages on an absolute basis. Here an extension is made of a previous model for noise-free sequential photon-counting to the more general case involving both count-noise and arbitrary separation functions between count levels. This allows a basic model to be developed for the DQE associated with devices which approximate to the <span class="hlt">CCD</span> mode of operation, and conclusions to be made concerning the roles of the separation-function and count-noise in defining the departure from the ideal photon counter.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27338408','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27338408"><span>Systematic Calibration for <span class="hlt">Ultra-High</span> Accuracy Inertial Measurement Units.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cai, Qingzhong; Yang, Gongliu; Song, Ningfang; Liu, Yiliang</p> <p>2016-06-22</p> <p>An inertial navigation system (INS) has been widely used in challenging GPS environments. With the rapid development of modern physics, an atomic gyroscope will come into use in the near future with a predicted accuracy of 5 × 10(-6)°/h or better. However, existing calibration methods and devices can not satisfy the accuracy requirements of future <span class="hlt">ultra-high</span> accuracy inertial sensors. In this paper, an improved calibration model is established by introducing gyro g-sensitivity errors, accelerometer cross-coupling errors and lever arm errors. A systematic calibration method is proposed based on a 51-state Kalman filter and smoother. Simulation results show that the proposed calibration method can realize the estimation of all the parameters using a common dual-axis turntable. Laboratory and sailing tests prove that the position accuracy in a five-day inertial navigation can be improved about 8% by the proposed calibration method. The accuracy can be improved at least 20% when the position accuracy of the atomic gyro INS can reach a level of 0.1 nautical miles/5 d. Compared with the existing calibration methods, the proposed method, with more error sources and <span class="hlt">high</span> order small error parameters calibrated for <span class="hlt">ultra-high</span> accuracy inertial measurement units (IMUs) using common turntables, has a great application potential in future atomic gyro INSs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ISPAr49B3..251J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ISPAr49B3..251J"><span>Classification of LIDAR Data for Generating a <span class="hlt">High-Precision</span> Roadway Map</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jeong, J.; Lee, I.</p> <p>2016-06-01</p> <p>Generating of a <span class="hlt">highly</span> <span class="hlt">precise</span> map grows up with development of autonomous driving vehicles. The <span class="hlt">highly</span> <span class="hlt">precise</span> map includes a <span class="hlt">precision</span> of centimetres level unlike an existing commercial map with the <span class="hlt">precision</span> of meters level. It is important to understand road environments and make a decision for autonomous driving since a robust localization is one of the critical challenges for the autonomous driving car. The one of source data is from a Lidar because it provides <span class="hlt">highly</span> dense point cloud data with three dimensional position, intensities and ranges from the sensor to target. In this paper, we focus on how to segment point cloud data from a Lidar on a vehicle and classify objects on the road for the <span class="hlt">highly</span> <span class="hlt">precise</span> map. In particular, we propose the combination with a feature descriptor and a classification algorithm in machine learning. Objects can be distinguish by geometrical features based on a surface normal of each point. To achieve correct classification using limited point cloud data sets, a Support Vector Machine algorithm in machine learning are used. Final step is to evaluate accuracies of obtained results by comparing them to reference data The results show sufficient accuracy and it will be utilized to generate a <span class="hlt">highly</span> <span class="hlt">precise</span> road map.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29271757','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29271757"><span>Gratings for synchrotron and FEL beamlines: a project for the manufacture of <span class="hlt">ultra-precise</span> gratings at Helmholtz Zentrum Berlin.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Siewert, F; Löchel, B; Buchheim, J; Eggenstein, F; Firsov, A; Gwalt, G; Kutz, O; Lemke, St; Nelles, B; Rudolph, I; Schäfers, F; Seliger, T; Senf, F; Sokolov, A; Waberski, Ch; Wolf, J; Zeschke, T; Zizak, I; Follath, R; Arnold, T; Frost, F; Pietag, F; Erko, A</p> <p>2018-01-01</p> <p>Blazed gratings are of dedicated interest for the monochromatization of synchrotron radiation when a <span class="hlt">high</span> photon flux is required, such as, for example, in resonant inelastic X-ray scattering experiments or when the use of laminar gratings is excluded due to too <span class="hlt">high</span> flux densities and expected damage, for example at free-electron laser beamlines. Their availability became a bottleneck since the decommissioning of the grating manufacture facility at Carl Zeiss in Oberkochen. To resolve this situation a new technological laboratory was established at the Helmholtz Zentrum Berlin, including instrumentation from Carl Zeiss. Besides the upgraded ZEISS equipment, an advanced grating production line has been developed, including a new <span class="hlt">ultra-precise</span> ruling machine, ion etching technology as well as laser interference lithography. While the old ZEISS ruling machine GTM-6 allows ruling for a grating length up to 170 mm, the new GTM-24 will have the capacity for 600 mm (24 inch) gratings with groove densities between 50 lines mm -1 and 1200 lines mm -1 . A new ion etching machine with a scanning radiofrequency excited ion beam (HF) source allows gratings to be etched into substrates of up to 500 mm length. For a final at-wavelength characterization, a new reflectometer at a new Optics beamline at the BESSY-II storage ring is under operation. This paper reports on the status of the grating fabrication, the measured quality of fabricated items by ex situ and in situ metrology, and future development goals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/970','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/970"><span>Simultaneous structural and environmental loading of an <span class="hlt">ultra-high</span> performance concrete component</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2010-07-01</p> <p><span class="hlt">Ultra-high</span> performance concrete (UHPC) is an advanced cementitious composite material which tends to exhibit superior properties such as increased durability, strength, and long-term stability. This experimental investigation focused on the flexural ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4750074','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4750074"><span><span class="hlt">Ultra-high</span>-throughput Production of III-V/Si Wafer for Electronic and Photonic Applications</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Geum, Dae-Myeong; Park, Min-Su; Lim, Ju Young; Yang, Hyun-Duk; Song, Jin Dong; Kim, Chang Zoo; Yoon, Euijoon; Kim, SangHyeon; Choi, Won Jun</p> <p>2016-01-01</p> <p>Si-based integrated circuits have been intensively developed over the past several decades through ultimate device scaling. However, the Si technology has reached the physical limitations of the scaling. These limitations have fuelled the search for alternative active materials (for transistors) and the introduction of optical interconnects (called “Si photonics”). A series of attempts to circumvent the Si technology limits are based on the use of III-V compound semiconductor due to their superior benefits, such as <span class="hlt">high</span> electron mobility and direct bandgap. To use their physical properties on a Si platform, the formation of <span class="hlt">high</span>-quality III-V films on the Si (III-V/Si) is the basic technology ; however, implementing this technology using a <span class="hlt">high</span>-throughput process is not easy. Here, we report new concepts for an <span class="hlt">ultra-high</span>-throughput heterogeneous integration of <span class="hlt">high</span>-quality III-V films on the Si using the wafer bonding and epitaxial lift off (ELO) technique. We describe the <span class="hlt">ultra</span>-fast ELO and also the re-use of the III-V donor wafer after III-V/Si formation. These approaches provide an <span class="hlt">ultra-high</span>-throughput fabrication of III-V/Si substrates with a <span class="hlt">high</span>-quality film, which leads to a dramatic cost reduction. As proof-of-concept devices, this paper demonstrates GaAs-based <span class="hlt">high</span> electron mobility transistors (HEMTs), solar cells, and hetero-junction phototransistors on Si substrates. PMID:26864968</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28042846','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28042846"><span><span class="hlt">High-Precision</span> Registration of Point Clouds Based on Sphere Feature Constraints.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Huang, Junhui; Wang, Zhao; Gao, Jianmin; Huang, Youping; Towers, David Peter</p> <p>2016-12-30</p> <p>Point cloud registration is a key process in multi-view 3D measurements. Its <span class="hlt">precision</span> affects the measurement <span class="hlt">precision</span> directly. However, in the case of the point clouds with non-overlapping areas or curvature invariant surface, it is difficult to achieve a <span class="hlt">high</span> <span class="hlt">precision</span>. A <span class="hlt">high</span> <span class="hlt">precision</span> registration method based on sphere feature constraint is presented to overcome the difficulty in the paper. Some known sphere features with constraints are used to construct virtual overlapping areas. The virtual overlapping areas provide more accurate corresponding point pairs and reduce the influence of noise. Then the transformation parameters between the registered point clouds are solved by an optimization method with weight function. In that case, the impact of large noise in point clouds can be reduced and a <span class="hlt">high</span> <span class="hlt">precision</span> registration is achieved. Simulation and experiments validate the proposed method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5298645','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5298645"><span><span class="hlt">High-Precision</span> Registration of Point Clouds Based on Sphere Feature Constraints</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Huang, Junhui; Wang, Zhao; Gao, Jianmin; Huang, Youping; Towers, David Peter</p> <p>2016-01-01</p> <p>Point cloud registration is a key process in multi-view 3D measurements. Its <span class="hlt">precision</span> affects the measurement <span class="hlt">precision</span> directly. However, in the case of the point clouds with non-overlapping areas or curvature invariant surface, it is difficult to achieve a <span class="hlt">high</span> <span class="hlt">precision</span>. A <span class="hlt">high</span> <span class="hlt">precision</span> registration method based on sphere feature constraint is presented to overcome the difficulty in the paper. Some known sphere features with constraints are used to construct virtual overlapping areas. The virtual overlapping areas provide more accurate corresponding point pairs and reduce the influence of noise. Then the transformation parameters between the registered point clouds are solved by an optimization method with weight function. In that case, the impact of large noise in point clouds can be reduced and a <span class="hlt">high</span> <span class="hlt">precision</span> registration is achieved. Simulation and experiments validate the proposed method. PMID:28042846</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/874596','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/874596"><span><span class="hlt">Ultra-high</span> resolution computed tomography imaging</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Paulus, Michael J.; Sari-Sarraf, Hamed; Tobin, Jr., Kenneth William; Gleason, Shaun S.; Thomas, Jr., Clarence E.</p> <p>2002-01-01</p> <p>A method for <span class="hlt">ultra-high</span> resolution computed tomography imaging, comprising the steps of: focusing a <span class="hlt">high</span> energy particle beam, for example x-rays or gamma-rays, onto a target object; acquiring a 2-dimensional projection data set representative of the target object; generating a corrected projection data set by applying a deconvolution algorithm, having an experimentally determined a transfer function, to the 2-dimensional data set; storing the corrected projection data set; incrementally rotating the target object through an angle of approximately 180.degree., and after each the incremental rotation, repeating the radiating, acquiring, generating and storing steps; and, after the rotating step, applying a cone-beam algorithm, for example a modified tomographic reconstruction algorithm, to the corrected projection data sets to generate a 3-dimensional image. The size of the spot focus of the beam is reduced to not greater than approximately 1 micron, and even to not greater than approximately 0.5 microns.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008SPIE.6813E..07D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008SPIE.6813E..07D"><span>Video-rate or <span class="hlt">high-precision</span>: a flexible range imaging camera</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dorrington, Adrian A.; Cree, Michael J.; Carnegie, Dale A.; Payne, Andrew D.; Conroy, Richard M.; Godbaz, John P.; Jongenelen, Adrian P. P.</p> <p>2008-02-01</p> <p>A range imaging camera produces an output similar to a digital photograph, but every pixel in the image contains distance information as well as intensity. This is useful for measuring the shape, size and location of objects in a scene, hence is well suited to certain machine vision applications. Previously we demonstrated a heterodyne range imaging system operating in a relatively <span class="hlt">high</span> resolution (512-by-512) pixels and <span class="hlt">high</span> <span class="hlt">precision</span> (0.4 mm best case) configuration, but with a slow measurement rate (one every 10 s). Although this <span class="hlt">high</span> <span class="hlt">precision</span> range imaging is useful for some applications, the low acquisition speed is limiting in many situations. The system's frame rate and length of acquisition is fully configurable in software, which means the measurement rate can be increased by compromising <span class="hlt">precision</span> and image resolution. In this paper we demonstrate the flexibility of our range imaging system by showing examples of <span class="hlt">high</span> <span class="hlt">precision</span> ranging at slow acquisition speeds and video-rate ranging with reduced ranging <span class="hlt">precision</span> and image resolution. We also show that the heterodyne approach and the use of more than four samples per beat cycle provides better linearity than the traditional homodyne quadrature detection approach. Finally, we comment on practical issues of frame rate and beat signal frequency selection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011ASPC..443..425B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011ASPC..443..425B"><span>A <span class="hlt">CCD</span> Spectrometer for One Dollar</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Beaver, J.; Robert, D.</p> <p>2011-09-01</p> <p>We describe preliminary tests on a very low-cost system for obtaining stellar spectra for instructional use in an introductory astronomy laboratory. <span class="hlt">CCD</span> imaging with small telescopes is now commonplace and relatively inexpensive. Giving students direct experience taking stellar spectra, however, is much more difficult, and the equipment can easily be out of reach for smaller institutions, especially if one wants to give the experience to large numbers of students. We have performed preliminary tests on an extremely low-cost (about $1.00) objective grating that can be coupled with an existing <span class="hlt">CCD</span> camera or commercial digital single-lens reflex (DSLR) camera and a small telescope typical of introductory astronomy labs. With this equipment we believe it is possible for introductory astronomy students to take stellar spectra that are of <span class="hlt">high</span> enough quality to distinguish between many MK spectral classes, or to determine standard B and V magnitudes. We present observational tests of this objective grating used on an 8" Schmidt-Cassegrain with a low-end, consumer DSLR camera. Some low-cost strategies for reducing the raw data are compared, with an eye toward projects ranging from individual undergraduate research projects to use by many students in a non-majors introductory astronomy lab. Toward this end we compare various trade offs between complexity of the observing and data reduction processes and the usefulness of the final results. We also describe some undergraduate astronomy education projects that this system could potentially be used for. Some of these projects could involve data-sharing collaborations between students at different institutions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26993530','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26993530"><span>Effects of the <span class="hlt">ultra-high</span> pressure on structure and α-glucosidase inhibition of polysaccharide from Astragalus.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhu, Zhen-Yuan; Luo, You; Dong, Guo-Ling; Ren, Yuan-Yuan; Chen, Li-Jing; Guo, Ming-Zhu; Wang, Xiao-Ting; Yang, Xue-Ying; Zhang, Yongmin</p> <p>2016-06-01</p> <p>A novel homogeneous polysaccharide fraction (APS) was extracted from Astragalus by hot water and purified by Sephadex G-100 and G-75 column. Its molecular weight was 693kDa. APS and APS with <span class="hlt">ultra-high</span> pressure treatment exhibited significant inhibitory abilities on a-glucosidase, inhibition rate from <span class="hlt">high</span> to low in order was 400MPa-APS, 300MPa-APS, 500MPa-APS and APS. The inhibition ​percentage of 400MPa-APS (1.5mg/mL) was 49% (max.). This suggested that the inhibitory activity of APS on a-glucosidase was improved by <span class="hlt">ultra-high</span> pressure treatment. FT-IR, SEM, CD spectra, atomic force microscope and Congo red test analysis of APS and 400MPa-APS showed <span class="hlt">ultra-high</span> pressure treatment didn't change the preliminary structure but had an effect on its advanced structure. Copyright © 2016 Elsevier B.V. All rights reserved.</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/2013SPIE.8905E..19W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013SPIE.8905E..19W"><span>Method of <span class="hlt">high</span> <span class="hlt">precision</span> interval measurement in pulse laser ranging system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Zhen; Lv, Xin-yuan; Mao, Jin-jin; Liu, Wei; Yang, Dong</p> <p>2013-09-01</p> <p>Laser ranging is suitable for laser system, for it has the advantage of <span class="hlt">high</span> measuring <span class="hlt">precision</span>, fast measuring speed,no cooperative targets and strong resistance to electromagnetic interference,the measuremen of laser ranging is the key paremeters affecting the performance of the whole system.The <span class="hlt">precision</span> of the pulsed laser ranging system was decided by the <span class="hlt">precision</span> of the time interval measurement, the principle structure of laser ranging system was introduced, and a method of <span class="hlt">high</span> <span class="hlt">precision</span> time interval measurement in pulse laser ranging system was established in this paper.Based on the analysis of the factors which affected the <span class="hlt">precision</span> of range measure,the pulse rising edges discriminator was adopted to produce timing mark for the start-stop time discrimination,and the TDC-GP2 <span class="hlt">high</span> <span class="hlt">precision</span> interval measurement system based on TMS320F2812 DSP was designed to improve the measurement <span class="hlt">precision</span>.Experimental results indicate that the time interval measurement method in this paper can obtain higher range accuracy. Compared with the traditional time interval measurement system,the method simplifies the system design and reduce the influence of bad weather conditions,furthermore,it satisfies the requirements of low costs and miniaturization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006JPhCS..56..195K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006JPhCS..56..195K"><span>Characterization of a parallel beam <span class="hlt">CCD</span> optical-CT apparatus for 3D radiation dosimetry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krstajić, Nikola; Doran, Simon J.</p> <p>2006-12-01</p> <p>This paper describes the initial steps we have taken in establishing <span class="hlt">CCD</span> based optical-CT as a viable alternative for 3-D radiation dosimetry. First, we compare the optical density (OD) measurements from a <span class="hlt">high</span> quality test target and variable neutral density filter (VNDF). A modulation transfer function (MTF) of individual projections is derived for three positions of the sinusoidal test target within the scanning tank. Our <span class="hlt">CCD</span> is then characterized in terms of its signal-to-noise ratio (SNR). Finally, a sample reconstruction of a scan of a PRESAGETM (registered trademark of Heuris Pharma, NJ, Skillman, USA.) dosimeter is given, demonstrating the capabilities of the apparatus.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820011592','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820011592"><span><span class="hlt">Ultra</span> <span class="hlt">high</span> speed image processing techniques. [electronic packaging techniques</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Anthony, T.; Hoeschele, D. F.; Connery, R.; Ehland, J.; Billings, J.</p> <p>1981-01-01</p> <p>Packaging techniques for <span class="hlt">ultra</span> <span class="hlt">high</span> speed image processing were developed. These techniques involve the development of a signal feedthrough technique through LSI/VLSI sapphire substrates. This allows the stacking of LSI/VLSI circuit substrates in a 3 dimensional package with greatly reduced length of interconnecting lines between the LSI/VLSI circuits. The reduced parasitic capacitances results in higher LSI/VLSI computational speeds at significantly reduced power consumption levels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080039564','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080039564"><span>The In-flight Spectroscopic Performance of the Swift XRT <span class="hlt">CCD</span> Camera During 2006-2007</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Godet, O.; Beardmore, A.P.; Abbey, A.F.; Osborne, J.P.; Page, K.L.; Evans, P.; Starling, R.; Wells, A.A.; Angelini, L.; Burrows, D.N.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20080039564'); toggleEditAbsImage('author_20080039564_show'); toggleEditAbsImage('author_20080039564_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20080039564_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20080039564_hide"></p> <p>2007-01-01</p> <p>The Swift X-ray Telescope focal plane camera is a front-illuminated MOS <span class="hlt">CCD</span>, providing a spectral response kernel of 135 eV FWHM at 5.9 keV as measured before launch. We describe the <span class="hlt">CCD</span> calibration program based on celestial and on-board calibration sources, relevant in-flight experiences, and developments in the <span class="hlt">CCD</span> response model. We illustrate how the revised response model describes the calibration sources well. Comparison of observed spectra with models folded through the instrument response produces negative residuals around and below the Oxygen edge. We discuss several possible causes for such residuals. Traps created by proton damage on the <span class="hlt">CCD</span> increase the charge transfer inefficiency (CTI) over time. We describe the evolution of the CTI since the launch and its effect on the <span class="hlt">CCD</span> spectral resolution and the gain.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27510737','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27510737"><span>Development and validation of an <span class="hlt">ultra</span>-performance convergence chromatography method for the quality control of Angelica gigas Nakai.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Hyo Seon; Chun, Jin Mi; Kwon, Bo-In; Lee, A-Reum; Kim, Ho Kyoung; Lee, A Yeong</p> <p>2016-10-01</p> <p><span class="hlt">Ultra</span>-performance convergence chromatography, which integrates the advantages of supercritical fluid chromatography and <span class="hlt">ultra</span> <span class="hlt">high</span> performance liquid chromatography technologies, is an environmentally friendly analytical method that uses dramatically reduced amounts of organic solvents. An <span class="hlt">ultra</span>-performance convergence chromatography method was developed and validated for the quantification of decursinol angelate and decursin in Angelica gigas using a CSH Fluoro-Phenyl column (2.1 mm × 150 mm, 1.7 μm) with a run time of 4 min. The method had an improved resolution and a shorter analysis time in comparison to the conventional <span class="hlt">high</span>-performance liquid chromatography method. This method was validated in terms of linearity, <span class="hlt">precision</span>, and accuracy. The limits of detection were 0.005 and 0.004 μg/mL for decursinol angelate and decursin, respectively, while the limits of quantitation were 0.014 and 0.012 μg/mL, respectively. The two components showed good regression (correlation coefficient (r 2 ) > 0.999), excellent <span class="hlt">precision</span> (RSD < 2.28%), and acceptable recoveries (99.75-102.62%). The proposed method can be used to efficiently separate, characterize, and quantify decursinol angelate and decursin in Angelica gigas and its related medicinal materials or preparations, with the advantages of a shorter analysis time, greater sensitivity, and better environmental compatibility. © 2016 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MeScR..18...65D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MeScR..18...65D"><span><span class="hlt">High</span> <span class="hlt">Precision</span> Edge Detection Algorithm for Mechanical Parts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Duan, Zhenyun; Wang, Ning; Fu, Jingshun; Zhao, Wenhui; Duan, Boqiang; Zhao, Jungui</p> <p>2018-04-01</p> <p><span class="hlt">High</span> <span class="hlt">precision</span> and <span class="hlt">high</span> efficiency measurement is becoming an imperative requirement for a lot of mechanical parts. So in this study, a subpixel-level edge detection algorithm based on the Gaussian integral model is proposed. For this purpose, the step edge normal section line Gaussian integral model of the backlight image is constructed, combined with the point spread function and the single step model. Then gray value of discrete points on the normal section line of pixel edge is calculated by surface interpolation, and the coordinate as well as gray information affected by noise is fitted in accordance with the Gaussian integral model. Therefore, a <span class="hlt">precise</span> location of a subpixel edge was determined by searching the mean point. Finally, a gear tooth was measured by M&M3525 gear measurement center to verify the proposed algorithm. The theoretical analysis and experimental results show that the local edge fluctuation is reduced effectively by the proposed method in comparison with the existing subpixel edge detection algorithms. The subpixel edge location accuracy and computation speed are improved. And the maximum error of gear tooth profile total deviation is 1.9 μm compared with measurement result with gear measurement center. It indicates that the method has <span class="hlt">high</span> reliability to meet the requirement of <span class="hlt">high</span> <span class="hlt">precision</span> measurement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24364867','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24364867"><span>A customized protocol to assess bone quality in the metacarpal head, metacarpal shaft and distal radius: a <span class="hlt">high</span> resolution peripheral quantitative computed tomography <span class="hlt">precision</span> study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Feehan, Lynne; Buie, Helen; Li, Linda; McKay, Heather</p> <p>2013-12-24</p> <p><span class="hlt">High</span> Resolution-Peripheral Quantitative Computed Tomography (HR-pQCT) is an emerging technology for evaluation of bone quality in Rheumatoid Arthritis (RA). However, there are limitations with standard HR-pQCT imaging protocols for examination of regions of bone commonly affected in RA. We developed a customized protocol for evaluation of volumetric bone mineral density (vBMD) and microstructure at the metacarpal head (MH), metacarpal shaft (MS) and <span class="hlt">ultra-ultra</span>-distal (UUD) radius; three sites commonly affected in RA. The purpose was to evaluate short-term measurement <span class="hlt">precision</span> for bone density and microstructure at these sites. 12 non-RA participants, individuals likely to have no pre-existing bone damage, consented to participate [8 females, aged 23 to 71 y [median (IQR): 44 (28) y]. The custom protocol includes more comfortable/stable positioning and adapted cortical segmentation and direct transformation analysis methods. Dominant arm MH, MS and UUD radius scans were completed on day one; repeated twice (with repositioning) three to seven days later. Short-term <span class="hlt">precision</span> for repeated measures was explored using intraclass correlational coefficient (ICC), mean coefficient of variation (CV%), root mean square coefficient of variation (RMSCV%) and least significant change (LSC%95). Bone density and microstructure <span class="hlt">precision</span> was excellent: ICCs varied from 0.88 (MH2 trabecular number) to .99 (MS3 polar moment of inertia); CV% varied from < 1 (MS2 vBMD) to 6 (MS3 marrow space diameter); RMSCV% varied from < 1 (MH2 full bone vBMD) to 7 (MS3 marrow space diameter); and LSC%95 varied from 2 (MS2 full bone vBMD to 21 (MS3 marrow space diameter). Cortical porosity measures were the exception; RMSCV% varying from 19 (MS3) to 42 (UUD). No scans were stopped for discomfort. 5% (5/104) were repeated due to motion during imaging. 8% (8/104) of final images had motion artifact graded > 3 on 5 point scale. In our facility, this custom protocol extends the potential for in vivo</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AAS...21840604K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AAS...21840604K"><span>Fiber Scrambling for <span class="hlt">High</span> <span class="hlt">Precision</span> Spectrographs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kaplan, Zachary; Spronck, J. F. P.; Fischer, D.</p> <p>2011-05-01</p> <p>The detection of Earth-like exoplanets with the radial velocity method requires extreme Doppler <span class="hlt">precision</span> and long-term stability in order to measure tiny reflex velocities in the host star. Recent planet searches have led to the detection of so called "super-Earths” (up to a few Earth masses) that induce radial velocity changes of about 1 m/s. However, the detection of true Earth analogs requires a <span class="hlt">precision</span> of 10 cm/s. One of the largest factors limiting Doppler <span class="hlt">precision</span> is variation in the Point Spread Function (PSF) from observation to observation due to changes in the illumination of the slit and spectrograph optics. Thus, this stability has become a focus of current instrumentation work. Fiber optics have been used since the 1980's to couple telescopes to <span class="hlt">high-precision</span> spectrographs, initially for simpler mechanical design and control. However, fiber optics are also naturally efficient scramblers. Scrambling refers to a fiber's ability to produce an output beam independent of input. Our research is focused on characterizing the scrambling properties of several types of fibers, including circular, square and octagonal fibers. By measuring the intensity distribution after the fiber as a function of input beam position, we can simulate guiding errors that occur at an observatory. Through this, we can determine which fibers produce the most uniform outputs for the severest guiding errors, improving the PSF and allowing sub-m/s <span class="hlt">precision</span>. However, extensive testing of fibers of supposedly identical core diameter, length and shape from the same manufacturer has revealed the "personality” of individual fibers. Personality describes differing intensity patterns for supposedly duplicate fibers illuminated identically. Here, we present our results on scrambling characterization as a function of fiber type, while studying individual fiber personality.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28854262','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28854262"><span>Accurate measurement of chest compression depth using impulse-radio <span class="hlt">ultra</span>-wideband sensor on a mattress.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yu, Byung Gyu; Oh, Je Hyeok; Kim, Yeomyung; Kim, Tae Wook</p> <p>2017-01-01</p> <p>We developed a new chest compression depth (<span class="hlt">CCD</span>) measuring technology using radar and impulse-radio <span class="hlt">ultra</span>-wideband (IR-UWB) sensor. This study was performed to determine its accuracy on a soft surface. Four trials, trial 1: chest compressions on the floor using an accelerometer device; trial 2: chest compressions on the floor using an IR-UWB sensor; trial 3: chest compressions on a foam mattress using an accelerometer device; trial 4: chest compressions on a foam mattress using an IR-UWB sensor, were performed in a random order. In all the trials, a cardiopulmonary resuscitation provider delivered 50 uninterrupted chest compressions to a manikin. The <span class="hlt">CCD</span> measured by the manikin and the device were as follows: 57.42 ± 2.23 and 53.92 ± 2.92 mm, respectively in trial 1 (p < 0.001); 56.29 ± 1.96 and 54.16 ± 3.90 mm, respectively in trial 2 (p < 0.001); 55.61 ± 1.57 and 103.48 ± 10.48 mm, respectively in trial 3 (p < 0.001); 57.14 ± 3.99 and 55.51 ± 3.39 mm, respectively in trial 4 (p = 0.012). The gaps between the <span class="hlt">CCD</span> measured by the manikin and the devices (accelerometer device vs. IR-UWB sensor) on the floor were not different (3.50 ± 2.08 mm vs. 3.15 ± 2.27 mm, respectively, p = 0.136). However, the gaps were significantly different on the foam mattress (48.53 ± 5.65 mm vs. 4.10 ± 2.47 mm, p < 0.001). The IR-UWB sensor could measure the <span class="hlt">CCD</span> accurately both on the floor and on the foam mattress.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27501011','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27501011"><span>The Cross-Cultural Dementia Screening (<span class="hlt">CCD</span>): A new neuropsychological screening instrument for dementia in elderly immigrants.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Goudsmit, Miriam; Uysal-Bozkir, Özgül; Parlevliet, Juliette L; van Campen, Jos P C M; de Rooij, Sophia E; Schmand, Ben</p> <p>2017-03-01</p> <p>Currently, approximately 3.9% of the European population are non-EU citizens, and a large part of these people are from "non-Western" societies, such as Turkey and Morocco. For various reasons, the incidence of dementia in this group is expected to increase. However, cognitive testing is challenging due to language barriers and low education and/or illiteracy. The newly developed Cross-Cultural Dementia Screening (<span class="hlt">CCD</span>) can be administered without an interpreter. It contains three subtests that assess memory, mental speed, and executive function. We hypothesized the <span class="hlt">CCD</span> to be a culture-fair test that could discriminate between demented patients and cognitively healthy controls. To test this hypothesis, 54 patients who had probable dementia were recruited via memory clinics. Controls (N = 1625) were recruited via their general practitioners. All patients and controls were aged 55 years and older and of six different self-defined ethnicities (Dutch, Turkish, Moroccan-Arabic, Moroccan-Berber, Surinamese-Creole, and Surinamese-Hindustani). Exclusion criteria included current or previous conditions that affect cognitive functioning. There were performance differences between the ethnic groups, but these disappeared after correcting for age and education differences between the groups, which supports our central hypothesis that the <span class="hlt">CCD</span> is a culture-fair test. Receiver-operating characteristic (ROC) and logistic regression analyses showed that the <span class="hlt">CCD</span> has <span class="hlt">high</span> predictive validity for dementia (sensitivity: 85%; specificity: 89%). The <span class="hlt">CCD</span> is a sensitive and culture-fair neuropsychological instrument for dementia screening in low-educated immigrant populations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EPJWC..5306008T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EPJWC..5306008T"><span>A strategy to unveil transient sources of <span class="hlt">ultra-high</span>-energy cosmic rays</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Takami, Hajime</p> <p>2013-06-01</p> <p>Transient generation of <span class="hlt">ultra-high</span>-energy cosmic rays (UHECRs) has been motivated from promising candidates of UHECR sources such as gamma-ray bursts, flares of active galactic nuclei, and newly born neutron stars and magnetars. Here we propose a strategy to unveil transient sources of UHECRs from UHECR experiments. We demonstrate that the rate of UHECR bursts and/or flares is related to the apparent number density of UHECR sources, which is the number density estimated on the assumption of steady sources, and the time-profile spread of the bursts produced by cosmic magnetic fields. The apparent number density strongly depends on UHECR energies under a given rate of the bursts, which becomes observational evidence of transient sources. It is saturated at the number density of host galaxies of UHECR sources. We also derive constraints on the UHECR burst rate and/or energy budget of UHECRs per source as a function of the apparent source number density by using models of cosmic magnetic fields. In order to obtain a <span class="hlt">precise</span> constraint of the UHECR burst rate, <span class="hlt">high</span> event statistics above ˜ 1020 eV for evaluating the apparent source number density at the highest energies and better knowledge on cosmic magnetic fields by future observations and/or simulations to better estimate the time-profile spread of UHECR bursts are required. The estimated rate allows us to constrain transient UHECR sources by being compared with the occurrence rates of known energetic transient phenomena.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29631045','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29631045"><span>Microstructure of <span class="hlt">ultra</span> <span class="hlt">high</span> performance concrete containing lithium slag.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>He, Zhi-Hai; Du, Shi-Gui; Chen, Deng</p> <p>2018-04-03</p> <p>Lithium slag (LS) is discharged as a byproduct in the process of the lithium carbonate, and it is very urgent to explore an efficient way to recycle LS in order to protect the environments and save resources. Many available supplementary cementitious materials for partial replacement of cement and/or silica fume (SF) can be used to prepare <span class="hlt">ultra</span> <span class="hlt">high</span> performance concrete (UHPC). The effect of LS to replace SF partially by weight used as a supplementary cementitious material (0%, 5%, 10% and 15% of binder) on the compressive strengths and microstructure evolution of UHPC has experimentally been studied by multi-techniques including mercury intrusion porosimetry, scanning electron microscope and nanoindentation technique. The results show that the use of LS degrades the microstructure of UHPC at early ages, and however, the use of LS with the appropriate content improves microstructure of UHPC at later ages. The hydration products of UHPC are mainly dominated by <span class="hlt">ultra-high</span> density calcium-silicate-hydrate (UHD C-S-H) and interfacial transition zone (ITZ) in UHPC has similar compact microstructure with the matrix. The use of LS improves the hydration degree of UHPC and increases the elastic modulus of ITZ in UHPC. LS is a promising substitute for SF for preparation UHPC. Copyright © 2018 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/35954','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/35954"><span>Development of Non-Proprietary <span class="hlt">Ultra</span> <span class="hlt">High</span> Performance Concrete : Final Presentation : November, 2017</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2017-11-01</p> <p><span class="hlt">Ultra-high</span> performance concrete (UHPC) has mechanical and durability properties that far exceed those of conventional concrete. Particularly, UHPC has compressive and post-cracking tensile strengths of around 20 ksi and 0.72 ksi, respectively. Thus, ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26041248','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26041248"><span>The simple determination method for anthocyanidin aglycones in fruits using <span class="hlt">ultra-high</span>-performance liquid chromatography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shim, You-Shin; Yoon, Won-Jin; Kim, Dong-Man; Watanabe, Masaki; Park, Hyun-Jin; Jang, Hae Won; Lee, Jangho; Ha, Jaeho</p> <p>2015-01-01</p> <p>The simple determination method for anthocyanidin aglycones in fruits using <span class="hlt">ultra-high</span>-performance liquid chromatography (UHPLC) coupled with the heating-block acidic hydrolysis method was validated through the <span class="hlt">precision</span>, accuracy and linearity. The UHPLC separation was performed on a reversed-phase C18 column (particle size 2 μm, i.d. 2 mm, length 100 mm) with a photodiode-array detector. The limits of detection and quantification of the UHPLC analyses were 0.09 and 0.29 mg/kg for delphinidin, 0.08 and 0.24 mg/kg for cyanidin, 0.09 and 0.26 mg/kg for petunidin, 0.14 and 0.42 mg/kg for pelargonidin, 0.16 and 0.48 mg/kg for peonidin and 0.30 and 0.91 mg/kg for malvidin, respectively. The intra- and inter-day <span class="hlt">precisions</span> of individual anthocyanidin aglycones were <10.3%. All calibration curves exhibited good linearity (r = 0.999) within the tested ranges. The total run time of UHPLC was 8 min. The simple preparation method with UHPLC detection in this study presented herein significantly improved the speed and the simplicity for preparation step of delphinidin, cyanidin, petunidin, pelargonidin, peonidin and malvidin in fruits. Especially, the UHPLC detection exhibited good resolution in spite of shorter run time about four times than conventional HPLC detection. © The Author 2015. Published by Oxford University Press. All rights reserved. For Permissions, please email: journals.permissions@oup.com.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/32592','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/32592"><span><span class="hlt">Ultra-high</span> performance fiber-reinforced concrete (UHPFRC) for infrastructure rehabilitation Volume II : behavior of <span class="hlt">ultra-high</span> strength concrete bridge deck panels compared to conventional stay-in-place deck panels</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2017-08-01</p> <p>The remarkable features of <span class="hlt">ultra-high</span> performance concrete (UHPC) have been reported. Its application in bridge construction has been an active research area in recent years, attributed to its higher compressive strength, higher ductility and reduced...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22399066-long-range-surface-plasmon-resonance-ultra-high-penetration-depth-self-referenced-sensing-ultra-low-detection-limit-using-diverging-beam-approach','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22399066-long-range-surface-plasmon-resonance-ultra-high-penetration-depth-self-referenced-sensing-ultra-low-detection-limit-using-diverging-beam-approach"><span>Long range surface plasmon resonance with <span class="hlt">ultra-high</span> penetration depth for self-referenced sensing and <span class="hlt">ultra</span>-low detection limit using diverging beam approach</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>Isaacs, Sivan, E-mail: sivan.isaacs@gmail.com; Abdulhalim, Ibrahim; NEW CREATE Programme, School of Materials Science and Engineering, 1 CREATE Way, Research Wing, #02-06/08, Singapore 138602</p> <p>2015-05-11</p> <p>Using an insulator-metal-insulator structure with dielectric having refractive index (RI) larger than the analyte, long range surface plasmon (SP) resonance exhibiting <span class="hlt">ultra-high</span> penetration depth is demonstrated for sensing applications of large bioentities at wavelengths in the visible range. Based on the diverging beam approach in Kretschmann-Raether configuration, one of the SP resonances is shown to shift in response to changes in the analyte RI while the other is fixed; thus, it can be used as a built in reference. The combination of the <span class="hlt">high</span> sensitivity, <span class="hlt">high</span> penetration depth and self-reference using the diverging beam approach in which a dark linemore » is detected of the <span class="hlt">high</span> sensitivity, <span class="hlt">high</span> penetration depth, self-reference, and the diverging beam approach in which a dark line is detected using large number of camera pixels with a smart algorithm for sub-pixel resolution, a sensor with <span class="hlt">ultra</span>-low detection limit is demonstrated suitable for large bioentities.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20707182','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20707182"><span>[Techniques for pixel response nonuniformity correction of <span class="hlt">CCD</span> in interferential imaging spectrometer].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yao, Tao; Yin, Shi-Min; Xiangli, Bin; Lü, Qun-Bo</p> <p>2010-06-01</p> <p>Based on in-depth analysis of the relative radiation scaling theorem and acquired scaling data of pixel response nonuniformity correction of <span class="hlt">CCD</span> (charge-coupled device) in spaceborne visible interferential imaging spectrometer, a pixel response nonuniformity correction method of <span class="hlt">CCD</span> adapted to visible and infrared interferential imaging spectrometer system was studied out, and it availably resolved the engineering technical problem of nonuniformity correction in detector arrays for interferential imaging spectrometer system. The quantitative impact of <span class="hlt">CCD</span> nonuniformity on interferogram correction and recovery spectrum accuracy was given simultaneously. Furthermore, an improved method with calibration and nonuniformity correction done after the instrument is successfully assembled was proposed. The method can save time and manpower. It can correct nonuniformity caused by other reasons in spectrometer system besides <span class="hlt">CCD</span> itself's nonuniformity, can acquire recalibration data when working environment is changed, and can also more effectively improve the nonuniformity calibration accuracy of interferential imaging</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26707085','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26707085"><span>Comparison of <span class="hlt">ultra-high</span> performance supercritical fluid chromatography and <span class="hlt">ultra-high</span> performance liquid chromatography for the separation of spirostanol saponins.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhu, Ling-Ling; Zhao, Yang; Xu, Yong-Wei; Sun, Qing-Long; Sun, Xin-Guang; Kang, Li-Ping; Yan, Ren-Yi; Zhang, Jie; Liu, Chao; Ma, Bai-Ping</p> <p>2016-02-20</p> <p>Spirostanol saponins are important active components of some herb medicines, and their isolation and purification are crucial for the research and development of traditional Chinese medicines. We aimed to compare the separation of spirostanol saponins by <span class="hlt">ultra-high</span> performance supercritical fluid chromatography (UHPSFC) and <span class="hlt">ultra-high</span> performance liquid chromatography (UHPLC). Four groups of spirostanol saponins were separated respectively by UHPSFC and UHPLC. After optimization, UHPSFC was performed with a HSS C18 SB column or a Diol column and with methanol as the co-solvent. A BEH C18 column and mobile phase containing water (with 0.1% formic acid) and acetonitrile were used in UHPLC. We found that UHPSFC could be performed automatically and quickly. It is effective in separating the spirostanol saponins which share the same aglycone and vary in sugar chains, and is very sensitive to the number and the position of hydroxyl groups in aglycones. However, the resolution of spirostanol saponins with different aglycones and the same sugar moiety by UHPSFC was not ideal and could be resolved by UHPLC instead. UHPLC is good at differentiating the variation in aglycones, and is influenced by double bonds in aglycones. Therefore, UHPLC and UHPSFC are complementary in separating spirostanol saponins. Considering the naturally produced spirostanol saponins in herb medicines are different both in aglycones and in sugar chains, a better separation can be achieved by combination of UHPLC and UHPSFC. UHPSFC is a powerful technique for improving the resolution when UHPLC cannot resolve a mixture of spirostanol saponins and vice versa. Copyright © 2015 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ApPhL.101k3702S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ApPhL.101k3702S"><span><span class="hlt">Ultra-high</span> cooling rate utilizing thin film evaporation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Su, Fengmin; Ma, Hongbin; Han, Xu; Chen, Hsiu-hung; Tian, Bohan</p> <p>2012-09-01</p> <p>This research introduces a cell cryopreservation method, which utilizes thin film evaporation and provides an <span class="hlt">ultra-high</span> cooling rate. The microstructured surface forming the thin film evaporation was fabricated from copper microparticles with an average diameter of 50 μm. Experimental results showed that a cooling rate of approximately 5×104 °C/min was achieved in a temperature range from 10 °C to -187 °C. The current investigation will give birth to a cell cryopreservation method through vitrification with relatively low concentrations of cryoprotectants.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ExA....41..351C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ExA....41..351C"><span><span class="hlt">High</span> <span class="hlt">precision</span> radial velocities with GIANO spectra</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carleo, I.; Sanna, N.; Gratton, R.; Benatti, S.; Bonavita, M.; Oliva, E.; Origlia, L.; Desidera, S.; Claudi, R.; Sissa, E.</p> <p>2016-06-01</p> <p>Radial velocities (RV) measured from near-infrared (NIR) spectra are a potentially excellent tool to search for extrasolar planets around cool or active stars. <span class="hlt">High</span> resolution infrared (IR) spectrographs now available are reaching the <span class="hlt">high</span> <span class="hlt">precision</span> of visible instruments, with a constant improvement over time. GIANO is an infrared echelle spectrograph at the Telescopio Nazionale Galileo (TNG) and it is a powerful tool to provide <span class="hlt">high</span> resolution spectra for accurate RV measurements of exoplanets and for chemical and dynamical studies of stellar or extragalactic objects. No other <span class="hlt">high</span> spectral resolution IR instrument has GIANO's capability to cover the entire NIR wavelength range (0.95-2.45 μm) in a single exposure. In this paper we describe the ensemble of procedures that we have developed to measure <span class="hlt">high</span> <span class="hlt">precision</span> RVs on GIANO spectra acquired during the Science Verification (SV) run, using the telluric lines as wavelength reference. We used the Cross Correlation Function (CCF) method to determine the velocity for both the star and the telluric lines. For this purpose, we constructed two suitable digital masks that include about 2000 stellar lines, and a similar number of telluric lines. The method is applied to various targets with different spectral type, from K2V to M8 stars. We reached different <span class="hlt">precisions</span> mainly depending on the H-magnitudes: for H ˜ 5 we obtain an rms scatter of ˜ 10 m s-1, while for H ˜ 9 the standard deviation increases to ˜ 50 ÷ 80 m s-1. The corresponding theoretical error expectations are ˜ 4 m s-1 and 30 m s-1, respectively. Finally we provide the RVs measured with our procedure for the targets observed during GIANO Science Verification.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_23 --> <div id="page_24" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="461"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/14738125','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/14738125"><span><span class="hlt">Precision</span> ablation of dental enamel using a subpicosecond pulsed laser.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rode, A V; Gamaly, E G; Luther-Davies, B; Taylor, B T; Graessel, M; Dawes, J M; Chan, A; Lowe, R M; Hannaford, P</p> <p>2003-12-01</p> <p>In this study we report the use of <span class="hlt">ultra</span>-short-pulsed near-infrared lasers for <span class="hlt">precision</span> laser ablation of freshly extracted human teeth. The laser wavelength was approximately 800nm, with pulsewidths of 95 and 150fs, and pulse repetition rates of 1kHz. The laser beam was focused to an approximate diameter of 50microm and was scanned over the tooth surface. The rise in the intrapulpal temperature was monitored by embedded thermocouples, and was shown to remain below 5 degrees C when the tooth was air-cooled during laser treatment. The surface preparation of the ablated teeth, observed by optical and electron microscopy, showed no apparent cracking or heat effects, and the hardness and Raman spectra of the laser-treated enamel were not distinguishable from those of native enamel. This study indicates the potential for <span class="hlt">ultra</span>-short-pulsed lasers to effect <span class="hlt">precision</span> ablation of dental enamel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5245168','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5245168"><span>Rapid brain MRI acquisition techniques at <span class="hlt">ultra-high</span> fields</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Setsompop, Kawin; Feinberg, David A.; Polimeni, Jonathan R.</p> <p>2017-01-01</p> <p><span class="hlt">Ultra-high</span>-field MRI provides large increases in signal-to-noise ratio as well as enhancement of several contrast mechanisms in both structural and functional imaging. Combined, these gains result in a substantial boost in contrast-to-noise ratio that can be exploited for higher spatial resolution imaging to extract finer-scale information about the brain. With increased spatial resolution, however, is a concurrent increased image encoding burden that can cause unacceptably long scan times for structural imaging and slow temporal sampling of the hemodynamic response in functional MRI—particularly when whole-brain imaging is desired. To address this issue, new directions of imaging technology development—such as the move from conventional 2D slice-by-slice imaging to more efficient Simultaneous MultiSlice (SMS) or MultiBand imaging (which can be viewed as “pseudo-3D” encoding) as well as full 3D imaging—have provided dramatic improvements in acquisition speed. Such imaging paradigms provide higher SNR efficiency as well as improved encoding efficiency. Moreover, SMS and 3D imaging can make better use of coil sensitivity information in multi-channel receiver arrays used for parallel imaging acquisitions through controlled aliasing in multiple spatial directions. This has enabled unprecedented acceleration factors of an order of magnitude or higher in these imaging acquisition schemes, with low image artifact levels and <span class="hlt">high</span> SNR. Here we review the latest developments of SMS and 3D imaging methods and related technologies at <span class="hlt">ultra-high</span> field for rapid <span class="hlt">high</span>-resolution functional and structural imaging of the brain. PMID:26835884</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25840734','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25840734"><span>Modified Mostardi approach with <span class="hlt">ultra-high</span>-molecular-weight polyethylene tape for total hip arthroplasty provides a good rate of union of osteotomized fragments.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kuroda, Yutaka; Akiyama, Haruhiko; Nankaku, Manabu; So, Kazutaka; Matsuda, Shuichi</p> <p>2015-07-01</p> <p>A lateral approach is common in total hip arthroplasty because of the good exposure it provides and its low complication rates. However, a drawback of the procedure is that the abductor mechanism is damaged when the tendinous insertion of the abductor muscle is split. Here, we describe a wafer technique using <span class="hlt">ultra-high</span>-molecular-weight polyethylene tape for promising reattachment of the abductor mechanism. We retrospectively evaluated 120 consecutive primary total hip arthroplasties performed using a modified Mostardi approach, which involved reattaching the trochanter using either a braided polyester suture (polyester suture group, n = 60) or <span class="hlt">ultra-high</span>-molecular-weight polyethylene tape (UHMWPE tape group, n = 60). The osteotomized fragment was reattached by inducing bone-to-bone contact using 3-mm-wide tapes that were <span class="hlt">precisely</span> tied with a double-loop sliding knot in conjunction with a cable gun tensioner. The abductor strength and radiographic union rate were postoperatively assessed at 4 weeks and 6 months, respectively. A statistically significant lower incidence of nonunion and cutout was observed in the UHMWPE group (0 and 5.0 %, respectively) compared to the polyester suture group (8.3 and 15 %, respectively). No differences in abductor strength either preoperatively or at 4 weeks postoperatively were observed between the groups. In radiographically healed patients, abductor strength at 4 weeks post-surgery exceeded preoperative strength. The recovery rate of hip abductor strength was 109.9 ± 34.3 % in union patients and 92.9 ± 23.3 % in nonunion patients, which was statistically significant. The mean Japanese Orthopedic Association hip scores improved from 48.6 to 86.8 in union patients and from 50.3 to 85.9 in nonunion patients at 1 year postoperatively; however, this difference was not significant. The modified Mostardi approach using <span class="hlt">ultra-high</span> molecular weight polyethylene tape can promote successful union of the osteotomized fragment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28994811','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28994811"><span><span class="hlt">Precise</span>, <span class="hlt">High</span>-throughput Analysis of Bacterial Growth.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kurokawa, Masaomi; Ying, Bei-Wen</p> <p>2017-09-19</p> <p>Bacterial growth is a central concept in the development of modern microbial physiology, as well as in the investigation of cellular dynamics at the systems level. Recent studies have reported correlations between bacterial growth and genome-wide events, such as genome reduction and transcriptome reorganization. Correctly analyzing bacterial growth is crucial for understanding the growth-dependent coordination of gene functions and cellular components. Accordingly, the <span class="hlt">precise</span> quantitative evaluation of bacterial growth in a <span class="hlt">high</span>-throughput manner is required. Emerging technological developments offer new experimental tools that allow updates of the methods used for studying bacterial growth. The protocol introduced here employs a microplate reader with a <span class="hlt">highly</span> optimized experimental procedure for the reproducible and <span class="hlt">precise</span> evaluation of bacterial growth. This protocol was used to evaluate the growth of several previously described Escherichia coli strains. The main steps of the protocol are as follows: the preparation of a large number of cell stocks in small vials for repeated tests with reproducible results, the use of 96-well plates for <span class="hlt">high</span>-throughput growth evaluation, and the manual calculation of two major parameters (i.e., maximal growth rate and population density) representing the growth dynamics. In comparison to the traditional colony-forming unit (CFU) assay, which counts the cells that are cultured in glass tubes over time on agar plates, the present method is more efficient and provides more detailed temporal records of growth changes, but has a stricter detection limit at low population densities. In summary, the described method is advantageous for the <span class="hlt">precise</span> and reproducible <span class="hlt">high</span>-throughput analysis of bacterial growth, which can be used to draw conceptual conclusions or to make theoretical observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Nanos...8..536F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Nanos...8..536F"><span>Graphene stabilized <span class="hlt">ultra</span>-small CuNi nanocomposite with <span class="hlt">high</span> activity and recyclability toward catalysing the reduction of aromatic nitro-compounds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fang, Hao; Wen, Ming; Chen, Hanxing; Wu, Qingsheng; Li, Weiying</p> <p>2015-12-01</p> <p>Nowadays, it is of great significance and a challenge to design a noble-metal-free catalyst with <span class="hlt">high</span> activity and a long lifetime for the reduction of aromatic nitro-compounds. Here, a 2D structured nanocomposite catalyst with graphene supported CuNi alloy nanoparticles (NPs) is prepared, and is promising for meeting the requirements of green chemistry. In this graphene/CuNi nanocomposite, the <span class="hlt">ultra</span>-small CuNi nanoparticles (~2 nm) are evenly anchored on graphene sheets, which is not only a breakthrough in the structures, but also brings about an outstanding performance in activity and stability. Combined with a <span class="hlt">precise</span> optimization of the alloy ratios, the reaction rate constant of graphene/Cu61Ni39 reached a <span class="hlt">high</span> level of 0.13685 s-1, with a desirable selectivity as <span class="hlt">high</span> as 99% for various aromatic nitro-compounds. What's more, the catalyst exhibited a unprecedented long lifetime because it could be recycled over 25 times without obvious performance decay or even a morphology change. This work showed the promise and great potential of noble-metal-free catalysts in green chemistry.Nowadays, it is of great significance and a challenge to design a noble-metal-free catalyst with <span class="hlt">high</span> activity and a long lifetime for the reduction of aromatic nitro-compounds. Here, a 2D structured nanocomposite catalyst with graphene supported CuNi alloy nanoparticles (NPs) is prepared, and is promising for meeting the requirements of green chemistry. In this graphene/CuNi nanocomposite, the <span class="hlt">ultra</span>-small CuNi nanoparticles (~2 nm) are evenly anchored on graphene sheets, which is not only a breakthrough in the structures, but also brings about an outstanding performance in activity and stability. Combined with a <span class="hlt">precise</span> optimization of the alloy ratios, the reaction rate constant of graphene/Cu61Ni39 reached a <span class="hlt">high</span> level of 0.13685 s-1, with a desirable selectivity as <span class="hlt">high</span> as 99% for various aromatic nitro-compounds. What's more, the catalyst exhibited a unprecedented long lifetime</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004eso..pres...16.','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004eso..pres...16."><span>Weighing <span class="hlt">Ultra</span>-Cool Stars</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p></p> <p>2004-05-01</p> <p>Large Ground-Based Telescopes and Hubble Team-Up to Perform First Direct Brown Dwarf Mass Measurement [1] Summary Using ESO's Very Large Telescope at Paranal and a suite of ground- and space-based telescopes in a four-year long study, an international team of astronomers has measured for the first time the mass of an <span class="hlt">ultra</span>-cool star and its companion brown dwarf. The two stars form a binary system and orbit each other in about 10 years. The team obtained <span class="hlt">high</span>-resolution near-infrared images; on the ground, they defeated the blurring effect of the terrestrial atmosphere by means of adaptive optics techniques. By <span class="hlt">precisely</span> determining the orbit projected on the sky, the astronomers were able to measure the total mass of the stars. Additional data and comparison with stellar models then yield the mass of each of the components. The heavier of the two stars has a mass around 8.5% of the mass of the Sun and its brown dwarf companion is even lighter, only 6% of the solar mass. Both objects are relatively young with an age of about 500-1,000 million years. These observations represent a decisive step towards the still missing calibration of stellar evolution models for very-low mass stars. PR Photo 19a/04: Orbit of the <span class="hlt">ultra</span>-cool stars in 2MASSW J0746425+2000321. PR Photo 19b/04: Animated Gif of the orbital motion. Telephone number star Even though astronomers have found several hundreds of very low mass stars and brown dwarfs, the fundamental properties of these extreme objects, such as masses and surface temperatures, are still not well known. Within the cosmic zoo, these <span class="hlt">ultra</span>-cool stars represent a class of "intermediate" objects between giant planets - like Jupiter - and "normal" stars less massive than our Sun, and to understand them well is therefore crucial to the field of stellar astrophysics. The problem with these <span class="hlt">ultra</span>-cool stars is that contrary to normal stars that burn hydrogen in their central core, no unique relation exists between the luminosity of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012SPIE.8442E..47K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012SPIE.8442E..47K"><span>Nano-JASMINE: cosmic radiation degradation of <span class="hlt">CCD</span> performance and centroid detection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kobayashi, Yukiyasu; Shimura, Yuki; Niwa, Yoshito; Yano, Taihei; Gouda, Naoteru; Yamada, Yoshiyuki</p> <p>2012-09-01</p> <p>Nano-JASMINE (NJ) is a very small astrometry satellite project led by the National Astronomical Observatory of Japan. The satellite is ready for launch, and the launch is currently scheduled for late 2013 or early 2014. The satellite is equipped with a fully depleted <span class="hlt">CCD</span> and is expected to perform astrometry observations for stars brighter than 9 mag in the zw-band (0.6 µm-1.0 µm). Distances of stars located within 100 pc of the Sun can be determined by using annual parallax measurements. The targeted accuracy for the position determination of stars brighter than 7.5 mag is 3 mas, which is equivalent to measuring the positions of stars with an accuracy of less than one five-hundredth of the <span class="hlt">CCD</span> pixel size. The position measurements of stars are performed by centroiding the stellar images taken by the <span class="hlt">CCD</span> that operates in the time and delay integration mode. The degradation of charge transfer performance due to cosmic radiation damage in orbit is proved experimentally. A method is then required to compensate for the effects of performance degradation. One of the most effective ways of achieving this is to simulate observed stellar outputs, including the effect of <span class="hlt">CCD</span> degradation, and then formulate our centroiding algorithm and evaluate the accuracies of the measurements. We report here the planned procedure to simulate the outputs of the NJ observations. We also developed a <span class="hlt">CCD</span> performance-measuring system and present preliminary results obtained using the system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170012428','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170012428"><span>Live <span class="hlt">Ultra-High</span> Definition from the International Space Station</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Grubbs, Rodney; George, Sandy</p> <p>2017-01-01</p> <p>The first ever live downlink of <span class="hlt">Ultra-High</span> Definition (UHD) video from the International Space Station (ISS) was the highlight of a 'Super Session' at the National Association of Broadcasters (NAB) in April 2017. The <span class="hlt">Ultra-High</span> Definition video downlink from the ISS all the way to the Las Vegas Convention Center required considerable planning, pushed the limits of conventional video distribution from a space-craft, and was the first use of <span class="hlt">High</span> Efficiency Video Coding (HEVC) from a space-craft. The live event at NAB will serve as a pathfinder for more routine downlinks of UHD as well as use of HEVC for conventional HD downlinks to save bandwidth. HEVC may also enable live Virtual Reality video downlinks from the ISS. This paper will describe the overall work flow and routing of the UHD video, how audio was synchronized even though the video and audio were received many seconds apart from each other, and how the demonstration paves the way for not only more efficient video distribution from the ISS, but also serves as a pathfinder for more complex video distribution from deep space. The paper will also describe how a 'live' event was staged when the UHD coming from the ISS had a latency of 10+ seconds. Finally, the paper will discuss how NASA is leveraging commercial technologies for use on-orbit vs. creating technology as was required during the Apollo Moon Program and early space age.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003AAS...202.0808M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003AAS...202.0808M"><span>The First <span class="hlt">Precision</span> <span class="hlt">CCD</span> Observations of the Near Contact Binary, UY Muscae</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McKenzie, R.; Stoddard, M. L.; Samec, R. G.; Faulkner, D. R.</p> <p>2003-05-01</p> <p>As a part of our study of solar type stars with gas streams we observed UY Muscae [Star "y" (Oosterhoff, BAIN #148, 1928) GSC 8987 392, α (2000) = 12h 30m 47s , δ (2000) = -66° 01' 52.8"]. The observations were taken at CTIO in Chili with the 0.9-m reflector on 18, 19, 20, 23 May 2001, by RGS and DRF. The CFIM T2K <span class="hlt">CCD</span> camera with standard UBVRcIc filters in quad mode were used. More than 200 observations were taken in each pass band. The stars (GSC 8987 1279 α (2000) = 12h30m43.7s, δ (2000) = -65°59 '45") and (GSC 8987 1884, α (2000) = 12h30m45.7s, δ (2000) = -66°01 '5") were used as comparison and check stars, respectively. Two mean epochs of minimum light were determined from primary and secondary eclipses, HJD = 2452047.6239(0.0017) and 2452049.5918(0.0005) . Standard errors are given in parentheses. We calculated the following ephemeris from our data: HJD Tmin I = 2452047.6240(0.0003) + 0.562273(0.000151)d*E . A UBVRI synthetic light curve solution was calculated using the Wilson Code. It indicates the primary (more massive) component is under-filling its Roche lobe [fill-out = 94.4(0.001) critical lobe. This is similar to an Algol system. The final parameters include a mass ratio, m2/m1 = 0.551(0.001) , and a temperature difference T1-T2 = 1280(3)K. Two spots were modeled: a stream spot with a temperature factor of 1.060(0.002) very near the L1 point of the primary component and a solar type dark spot of radius 25.2(0.3)° with a T factor of 0.970( 0.001). Large night to night variations in the light curve lead us to believe that the components are saturated with magnetic activity. It is possible that the system was previously in contact and is undergoing TRO oscillations. Our model indicates that the components are currently separating. Further results of this study will be presented. We wish to thank CTIO for their allocation of observing time, and a small research grant from the American Astronomical Society which supported this run.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE10157E..03Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE10157E..03Z"><span>Design and algorithm research of <span class="hlt">high</span> <span class="hlt">precision</span> airborne infrared touch screen</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Xiao-Bing; Wang, Shuang-Jie; Fu, Yan; Chen, Zhao-Quan</p> <p>2016-10-01</p> <p>There are shortcomings of low <span class="hlt">precision</span>, touch shaking, and sharp decrease of touch <span class="hlt">precision</span> when emitting and receiving tubes are failure in the infrared touch screen. A <span class="hlt">high</span> <span class="hlt">precision</span> positioning algorithm based on extended axis is proposed to solve these problems. First, the unimpeded state of the beam between emitting and receiving tubes is recorded as 0, while the impeded state is recorded as 1. Then, the method of oblique scan is used, in which the light of one emitting tube is used for five receiving tubes. The impeded information of all emitting and receiving tubes is collected as matrix. Finally, according to the method of arithmetic average, the position of the touch object is calculated. The extended axis positioning algorithm is characteristic of <span class="hlt">high</span> <span class="hlt">precision</span> in case of failure of individual infrared tube and affects slightly the <span class="hlt">precision</span>. The experimental result shows that the 90% display area of the touch error is less than 0.25D, where D is the distance between adjacent emitting tubes. The conclusion is gained that the algorithm based on extended axis has advantages of <span class="hlt">high</span> <span class="hlt">precision</span>, little impact when individual infrared tube is failure, and using easily.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27216291','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27216291"><span>An <span class="hlt">ultra</span>-thin, un-doped NiO hole transporting layer of <span class="hlt">highly</span> efficient (16.4%) organic-inorganic hybrid perovskite solar cells.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Seo, Seongrok; Park, Ik Jae; Kim, Myungjun; Lee, Seonhee; Bae, Changdeuck; Jung, Hyun Suk; Park, Nam-Gyu; Kim, Jin Young; Shin, Hyunjung</p> <p>2016-06-02</p> <p>NiO is a wide band gap p-type oxide semiconductor and has potential for applications in solar energy conversion as a hole-transporting layer (HTL). It also has good optical transparency and <span class="hlt">high</span> chemical stability, and the capability of aligning the band edges to the perovskite (CH3NH3PbI3) layers. <span class="hlt">Ultra</span>-thin and un-doped NiO films with much less absorption loss were prepared by atomic layer deposition (ALD) with <span class="hlt">highly</span> <span class="hlt">precise</span> control over thickness without any pinholes. Thin enough (5-7.5 nm in thickness) NiO films with the thickness of few time the Debye length (LD = 1-2 nm for NiO) show enough conductivities achieved by overlapping space charge regions. The inverted planar perovskite solar cells with NiO films as HTLs exhibited the highest energy conversion efficiency of 16.40% with <span class="hlt">high</span> open circuit voltage (1.04 V) and fill factor (0.72) with negligible current-voltage hysteresis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PhST..156a4022K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PhST..156a4022K"><span><span class="hlt">High-precision</span> x-ray spectroscopy of <span class="hlt">highly</span> charged ions with microcalorimeters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kraft-Bermuth, S.; Andrianov, V.; Bleile, A.; Echler, A.; Egelhof, P.; Grabitz, P.; Ilieva, S.; Kilbourne, C.; Kiselev, O.; McCammon, D.; Meier, J.</p> <p>2013-09-01</p> <p>The <span class="hlt">precise</span> determination of the energy of the Lyman α1 and α2 lines in hydrogen-like heavy ions provides a sensitive test of quantum electrodynamics in very strong Coulomb fields. To improve the experimental <span class="hlt">precision</span>, the new detector concept of microcalorimeters is now exploited for such measurements. Such detectors consist of compensated-doped silicon thermistors and Pb or Sn absorbers to obtain <span class="hlt">high</span> quantum efficiency in the energy range of 40-70 keV, where the Doppler-shifted Lyman lines are located. For the first time, a microcalorimeter was applied in an experiment to <span class="hlt">precisely</span> determine the transition energy of the Lyman lines of lead ions at the experimental storage ring at GSI. The energy of the Ly α1 line E(Ly-α1, 207Pb81+) = (77937 ± 12stat ± 25syst) eV agrees within error bars with theoretical predictions. To improve the experimental <span class="hlt">precision</span>, a new detector array with more pixels and better energy resolution was equipped and successfully applied in an experiment to determine the Lyman-α lines of gold ions 197Au78+.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10123E..1NP','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10123E..1NP"><span>Heat dissipation schemes in QCLs monitored by <span class="hlt">CCD</span> thermoreflectance (Conference Presentation)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pierscinski, Kamil; Pierścińska, Dorota; Morawiec, Magdalena; Gutowski, Piotr; Karbownik, Piotr; Serebrennikova, Olga; Bugajski, Maciej</p> <p>2017-02-01</p> <p>In this paper we present the development of the instrumentation for accurate evaluation of the thermal characteristics of quantum cascade lasers based on <span class="hlt">CCD</span> thermoreflectance (<span class="hlt">CCD</span> TR). This method allows rapid thermal characterization of QCLs, as the registration of <span class="hlt">high</span>-resolution map of the whole device facet lasts only several seconds. The capabilities of the <span class="hlt">CCD</span> TR are used to study temperature dissipation schemes in different designs of QCLs. We report on the investigation of thermal performance of QCLs developed at the Institute of Electron Technology, with an emphasis on the influence of different material system, processing technology and device designs. We investigate and compare AlInAs/InGaAs/InP QCLs (lattice matched and strain compensated) of different architectures, i.e., double trench and buried heterostructure (BH) in terms of thermal management. Experimental results are in very good agreement with numerical predictions of heat dissipation in various device constructions. Numerical model is based on FEM model solved by commercial software package. The model assumes anisotropic thermal conductivity in the AR layers as well as the temperature dependence of thermal conductivities of all materials in the project. We have observed experimentally improvement of thermal properties of devices based on InP materials, especially for buried heterostructure type. The use of buried heterostructure enhanced the lateral heat dissipation from the active region of QCLs. The BH structure and epilayer-down bonding help dissipate the heat generated from active core of the QCL.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3658068','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3658068"><span>A validated <span class="hlt">ultra</span> <span class="hlt">high</span>-pressure liquid chromatography method for separation of candesartan cilexetil impurities and its degradents in drug product</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kumar, Namala Durga Atchuta; Babu, K. Sudhakar; Gosada, Ullas; Sharma, Nitish</p> <p>2012-01-01</p> <p>Introduction: A selective, specific, and sensitive “<span class="hlt">Ultra</span> <span class="hlt">High</span>-Pressure Liquid Chromatography” (UPLC) method was developed for determination of candesartan cilexetil impurities as well asits degradent in tablet formulation. Materials and Methods: The chromatographic separation was performed on Waters Acquity UPLC system and BEH Shield RP18 column using gradient elution of mobile phase A and B. 0.01 M phosphate buffer adjusted pH 3.0 with Orthophosphoric acid was used as mobile phase A and 95% acetonitrile with 5% Milli Q Water was used as mobile phase B. Ultraviolet (UV) detection was performed at 254 nm and 210 nm, where (CDS-6), (CDS-5), (CDS-7), (Ethyl Candesartan), (Desethyl CCX), (N-Ethyl), (CCX-1), (1 N Ethyl Oxo CCX), (2 N Ethyl Oxo CCX), (2 N Ethyl) and any unknown impurity were monitored at 254 nm wavelength, and two process-related impurities, trityl alcohol and MTE impurity, were estimated at 210 nm. Candesartan cilexetil andimpurities were chromatographed with a total run time of 20 min. Results: Calibration showed that the response of impurity was a linear function of concentration over the range limit of quantification to 2 μg/mL (r2≥0.999) and the method was validated over this range for <span class="hlt">precision</span>, intermediate <span class="hlt">precision</span>, accuracy, linearity, and specificity. For the <span class="hlt">precision</span> study, percentage relative standard deviation of each impurity was <15% (n=6). Conclusion: The method was found to be <span class="hlt">precise</span>, accurate, linear, and specific. The proposed method was successfully employed for estimation of candesartan cilexetil impurities in pharmaceutical preparations. PMID:23781475</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20060047798','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20060047798"><span>Correcting STIS <span class="hlt">CCD</span> Point-Source Spectra for CTE Loss</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Goudfrooij, Paul; Bohlin, Ralph C.; Maiz-Apellaniz, Jesus</p> <p>2006-01-01</p> <p>We review the on-orbit spectroscopic observations that are being used to characterize the Charge Transfer Efficiency (CTE) of the STIS <span class="hlt">CCD</span> in spectroscopic mode. We parameterize the CTE-related loss for spectrophotometry of point sources in terms of dependencies on the brightness of the source, the background level, the signal in the PSF outside the standard extraction box, and the time of observation. Primary constraints on our correction algorithm are provided by measurements of the CTE loss rates for simulated spectra (images of a tungsten lamp taken through slits oriented along the dispersion axis) combined with estimates of CTE losses for actual spectra of spectrophotometric standard stars in the first order <span class="hlt">CCD</span> modes. For point-source spectra at the standard reference position at the <span class="hlt">CCD</span> center, CTE losses as large as 30% are corrected to within approx.1% RMS after application of the algorithm presented here, rendering the Poisson noise associated with the source detection itself to be the dominant contributor to the total flux calibration uncertainty.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004JPhCS...3..240D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004JPhCS...3..240D"><span>Optical CT scanning of PRESAGETM polyurethane samples with a <span class="hlt">CCD</span>-based readout system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Doran, S. J.; Krstajic, N.; Adamovics, J.; Jenneson, P. M.</p> <p>2004-01-01</p> <p>This article demonstrates the resolution capabilities of the <span class="hlt">CCD</span> scanner under ideal circumstances and describes the first <span class="hlt">CCD</span>-based optical CT experiments on a new class of dosimeter, known as PRESAGETM (Heuris Pharma, Skillman, NJ).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AAS...20511101F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AAS...20511101F"><span><span class="hlt">High-Precision</span> Timing of Several Millisecond Pulsars</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ferdman, R. D.; Stairs, I. H.; Backer, D. C.; Ramachandran, R.; Demorest, P.; Nice, D. J.; Lyne, A. G.; Kramer, M.; Lorimer, D.; McLaughlin, M.; Manchester, D.; Camilo, F.; D'Amico, N.; Possenti, A.; Burgay, M.; Joshi, B. C.; Freire, P. C.</p> <p>2004-12-01</p> <p>The highest <span class="hlt">precision</span> pulsar timing is achieved by reproducing as accurately as possible the pulse profile as emitted by the pulsar, in <span class="hlt">high</span> signal-to-noise observations. The best profile reconstruction can be accomplished with several-bit voltage sampling and coherent removal of the dispersion suffered by pulsar signals as they traverse the interstellar medium. The Arecibo Signal Processor (ASP) and its counterpart the Green Bank Astronomical Signal Processor (GASP) are flexible, state-of-the-art wide-bandwidth observing systems, built primarily for <span class="hlt">high-precision</span> long-term timing of millisecond and binary pulsars. ASP and GASP are in use at the 300-m Arecibo telescope in Puerto Rico and the 100-m Green Bank Telescope in Green Bank, West Virginia, respectively, taking advantage of the enormous sensitivities of these telescopes. These instruments result in <span class="hlt">high-precision</span> science through 4 and 8-bit sampling and perform coherent dedispersion on the incoming data stream in real or near-real time. This is done using a network of personal computers, over an observing bandwidth of 64 to 128 MHz, in each of two polarizations. We present preliminary results of timing and polarimetric observations with ASP/GASP for several pulsars, including the recently-discovered relativistic double-pulsar binary J0737-3039. These data are compared to simultaneous observations with other pulsar instruments, such as the new "spigot card" spectrometer on the GBT and the Princeton Mark IV instrument at Arecibo, the precursor timing system to ASP. We also briefly discuss several upcoming observations with ASP/GASP.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AN....330..419M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AN....330..419M"><span>CTK: A new <span class="hlt">CCD</span> Camera at the University Observatory Jena</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mugrauer, M.</p> <p>2009-05-01</p> <p>The Cassegrain-Teleskop-Kamera (CTK) is a new <span class="hlt">CCD</span> imager which is operated at the University Observatory Jena since begin of 2006. This article describes the main characteristics of the new camera. The properties of the <span class="hlt">CCD</span> detector, the CTK image quality, as well as its detection limits for all filters are presented. Based on observations obtained with telescopes of the University Observatory Jena, which is operated by the Astrophysical Institute of the Friedrich-Schiller-University.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10322E..32P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10322E..32P"><span>Design and control of a <span class="hlt">high</span> <span class="hlt">precision</span> drive mechanism</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pan, Bo; He, Yongqiang; Wang, Haowei; Zhang, Shuyang; Zhang, Donghua; Wei, Xiaorong; Jiang, Zhihong</p> <p>2017-01-01</p> <p>This paper summarizes the development of a <span class="hlt">high</span> <span class="hlt">precision</span> drive mechanism (HPDM) for space application, such as the directional antenna, the laser communication device, the mobile camera and other pointing mechanisms. In view of the great practical significance of <span class="hlt">high</span> <span class="hlt">precision</span> drive system, control technology for permanent magnet synchronous motor (PMSM) servo system is also studied and a PMSM servo controller is designed in this paper. And the software alignment was applied to the controller to eliminate the steady error of the optical encoder, which helps to realize the 1 arcsec (1σ) control <span class="hlt">precision</span>. To assess its capabilities, the qualification environment testing including the thermal vacuum cycling testing, and the sinusoidal and random vibration were carried out. The testing results show that the performance of the HPDM is almost the same between the former and the end of each testing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1986sao..reptR....N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1986sao..reptR....N"><span>Development of a <span class="hlt">CCD</span> based solar speckle imaging system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nisenson, Peter; Stachnik, Robert V.; Noyes, Robert W.</p> <p>1986-02-01</p> <p>A program to develop software and hardware for the purpose of obtaining <span class="hlt">high</span> angular resolution images of the solar surface is described. The program included the procurement of a Charge Coupled Devices imaging system; an extensive laboratory and remote site testing of the camera system; the development of a software package for speckle image reconstruction which was eventually installed and tested at the Sacramento Peak Observatory; and experiments of the <span class="hlt">CCD</span> system (coupled to an image intensifier) for low light level, narrow spectral band solar imaging.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999ASPC..172..183B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999ASPC..172..183B"><span>A Pipeline Tool for <span class="hlt">CCD</span> Image Processing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bell, Jon F.; Young, Peter J.; Roberts, William H.; Sebo, Kim M.</p> <p></p> <p>MSSSO is part of a collaboration developing a wide field imaging <span class="hlt">CCD</span> mosaic (WFI). As part of this project, we have developed a GUI based pipeline tool that is an integrated part of MSSSO's CICADA data acquisition environment and processes <span class="hlt">CCD</span> FITS images as they are acquired. The tool is also designed to run as a stand alone program to process previously acquired data. IRAF tasks are used as the central engine, including the new NOAO mscred package for processing multi-extension FITS files. The STScI OPUS pipeline environment may be used to manage data and process scheduling. The Motif GUI was developed using SUN Visual Workshop. C++ classes were written to facilitate launching of IRAF and OPUS tasks. While this first version implements calibration processing up to and including flat field corrections, there is scope to extend it to other processing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1990SPIE.1235..413S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1990SPIE.1235..413S"><span>The CTIO Acquisition <span class="hlt">CCD</span>-TV camera design</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schmidt, Ricardo E.</p> <p>1990-07-01</p> <p>A <span class="hlt">CCD</span>-based Acquisition TV Camera has been developed at CTIO to replace the existing ISIT units. In a 60 second exposure, the new Camera shows a sixfold improvement in sensitivity over an ISIT used with a Leaky Memory. Integration times can be varied over a 0.5 to 64 second range. The <span class="hlt">CCD</span>, contained in an evacuated enclosure, is operated at -45 C. Only the image section, an area of 8.5 mm x 6.4 mm, gets exposed to light. Pixel size is 22 microns and either no binning or 2 x 2 binning can be selected. The typical readout rates used vary between 3.5 and 9 microseconds/pixel. Images are stored in a PC/XT/AT, which generates RS-170 video. The contrast in the RS-170 frames is automatically enhanced by the software.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018uhec.confa1021C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018uhec.confa1021C"><span>A Novel Study Connecting <span class="hlt">Ultra-High</span> Energy Cosmic Rays, Neutrinos, and Gamma-Rays</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Coenders, Stefan; Resconi, Elisa; Padovani, Paolo; Giommi, Paolo; Caccianiga, Lorenzo</p> <p></p> <p>We present a novel study connecting <span class="hlt">ultra-high</span> energy cosmic rays, neutrinos, and gamma-rays with the objective to identify common counterparts of the three astrophysical messengers. In the test presented here, we first identify potential hadronic sources by filtering gamma-ray emitters that are in spatial coincidence with IceCube neutrinos. Subsequently, these objects are correlated against <span class="hlt">ultra-high</span> energy cosmic rays detected by the Pierre Auger Observatory and the Telescope Array, scanning in gamma-ray flux and angular separation between sources and cosmic rays. A maximal excess of 80 cosmic rays (41.9 expected) is observed for the second catalog of hard Fermi-LAT objects of blazars of the <span class="hlt">high</span> synchrotron peak type. This corresponds to a deviation from the null-hypothesis of 2.94σ . No excess is observed for objects not in spatial connection with neutrinos. The gamma-ray sources that make up the excess are blazars of the <span class="hlt">high</span> synchrotron peak type.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007NIMPA.582..175L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007NIMPA.582..175L"><span><span class="hlt">CCD</span> detector development projects by the Beamline Technical Support Group at the Advanced Photon Source</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, John H.; Fernandez, Patricia; Madden, Tim; Molitsky, Michael; Weizeorick, John</p> <p>2007-11-01</p> <p>This paper will describe two ongoing detector projects being developed by the Beamline Technical Support Group at the Advanced Photon Source (APS) at Argonne National Laboratory (ANL). The first project is the design and construction of two detectors: a single-<span class="hlt">CCD</span> system and a two-by-two Mosaic <span class="hlt">CCD</span> camera for Small-Angle X-ray Scattering (SAXS). Both of these systems utilize the Kodak KAF-4320E <span class="hlt">CCD</span> coupled to fiber optic tapers, custom mechanical hardware, electronics, and software developed at ANL. The second project is a Fast-<span class="hlt">CCD</span> (FCCD) detector being developed in a collaboration between ANL and Lawrence Berkeley National Laboratory (LBNL). This detector will use ANL-designed readout electronics and a custom LBNL-designed <span class="hlt">CCD</span>, with 480×480 pixels and 96 outputs, giving very fast readout.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MNRAS.tmp.1148L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MNRAS.tmp.1148L"><span><span class="hlt">High</span> <span class="hlt">precision</span> pulsar timing and spin frequency second derivatives</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, X. J.; Bassa, C. G.; Stappers, B. W.</p> <p>2018-05-01</p> <p>We investigate the impact of intrinsic, kinematic and gravitational effects on <span class="hlt">high</span> <span class="hlt">precision</span> pulsar timing. We present an analytical derivation and a numerical computation of the impact of these effects on the first and second derivative of the pulsar spin frequency. In addition, in the presence of white noise, we derive an expression to determine the expected measurement uncertainty of a second derivative of the spin frequency for a given timing <span class="hlt">precision</span>, observing cadence and timing baseline and find that it strongly depends on the latter (∝t-7/2). We show that for pulsars with significant proper motion, the spin frequency second derivative is dominated by a term dependent on the radial velocity of the pulsar. Considering the data sets from three Pulsar Timing Arrays, we find that for PSR J0437-4715 a detectable spin frequency second derivative will be present if the absolute value of the radial velocity exceeds 33 km s-1. Similarly, at the current timing <span class="hlt">precision</span> and cadence, continued timing observations of PSR J1909-3744 for about another eleven years, will allow the measurement of its frequency second derivative and determine the radial velocity with an accuracy better than 14 km s-1. With the ever increasing timing <span class="hlt">precision</span> and observing baselines, the impact of the, largely unknown, radial velocities of pulsars on <span class="hlt">high</span> <span class="hlt">precision</span> pulsar timing can not be neglected.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4152160','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4152160"><span>Effects of biomechanical forces on signaling in the cortical collecting duct (<span class="hlt">CCD</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>Carrisoza-Gaytan, Rolando; Liu, Yu; Flores, Daniel; Else, Cindy; Lee, Heon Goo; Rhodes, George; Sandoval, Ruben M.; Kleyman, Thomas R.; Lee, Francis Young-In; Molitoris, Bruce; Satlin, Lisa M.</p> <p>2014-01-01</p> <p>An increase in tubular fluid flow rate (TFF) stimulates Na reabsorption and K secretion in the cortical collecting duct (<span class="hlt">CCD</span>) and subjects cells therein to biomechanical forces including fluid shear stress (FSS) and circumferential stretch (CS). Intracellular MAPK and extracellular autocrine/paracrine PGE2 signaling regulate cation transport in the <span class="hlt">CCD</span> and, at least in other systems, are affected by biomechanical forces. We hypothesized that FSS and CS differentially affect MAPK signaling and PGE2 release to modulate cation transport in the <span class="hlt">CCD</span>. To validate that CS is a physiological force in vivo, we applied the intravital microscopic approach to rodent kidneys in vivo to show that saline or furosemide injection led to a 46.5 ± 2.0 or 170 ± 32% increase, respectively, in distal tubular diameter. Next, murine <span class="hlt">CCD</span> (mpk<span class="hlt">CCD</span>) cells were grown on glass or silicone coated with collagen type IV and subjected to 0 or 0.4 dyne/cm2 of FSS or 10% CS, respectively, forces chosen based on prior biomechanical modeling of ex vivo microperfused CCDs. Cells exposed to FSS expressed an approximately twofold greater abundance of phospho(p)-ERK and p-p38 vs. static cells, while CS did not alter p-p38 and p-ERK expression compared with unstretched controls. FSS induced whereas CS reduced PGE2 release by ∼40%. In conclusion, FSS and CS differentially affect ERK and p38 activation and PGE2 release in a cell culture model of the CD. We speculate that TFF differentially regulates biomechanical signaling and, in turn, cation transport in the <span class="hlt">CCD</span>. PMID:24872319</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24872319','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24872319"><span>Effects of biomechanical forces on signaling in the cortical collecting duct (<span class="hlt">CCD</span>).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Carrisoza-Gaytan, Rolando; Liu, Yu; Flores, Daniel; Else, Cindy; Lee, Heon Goo; Rhodes, George; Sandoval, Ruben M; Kleyman, Thomas R; Lee, Francis Young-In; Molitoris, Bruce; Satlin, Lisa M; Rohatgi, Rajeev</p> <p>2014-07-15</p> <p>An increase in tubular fluid flow rate (TFF) stimulates Na reabsorption and K secretion in the cortical collecting duct (<span class="hlt">CCD</span>) and subjects cells therein to biomechanical forces including fluid shear stress (FSS) and circumferential stretch (CS). Intracellular MAPK and extracellular autocrine/paracrine PGE2 signaling regulate cation transport in the <span class="hlt">CCD</span> and, at least in other systems, are affected by biomechanical forces. We hypothesized that FSS and CS differentially affect MAPK signaling and PGE2 release to modulate cation transport in the <span class="hlt">CCD</span>. To validate that CS is a physiological force in vivo, we applied the intravital microscopic approach to rodent kidneys in vivo to show that saline or furosemide injection led to a 46.5 ± 2.0 or 170 ± 32% increase, respectively, in distal tubular diameter. Next, murine <span class="hlt">CCD</span> (mpk<span class="hlt">CCD</span>) cells were grown on glass or silicone coated with collagen type IV and subjected to 0 or 0.4 dyne/cm(2) of FSS or 10% CS, respectively, forces chosen based on prior biomechanical modeling of ex vivo microperfused CCDs. Cells exposed to FSS expressed an approximately twofold greater abundance of phospho(p)-ERK and p-p38 vs. static cells, while CS did not alter p-p38 and p-ERK expression compared with unstretched controls. FSS induced whereas CS reduced PGE2 release by ∼40%. In conclusion, FSS and CS differentially affect ERK and p38 activation and PGE2 release in a cell culture model of the CD. We speculate that TFF differentially regulates biomechanical signaling and, in turn, cation transport in the <span class="hlt">CCD</span>. Copyright © 2014 the American Physiological Society.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5876596','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5876596"><span>A Manganin Thin Film <span class="hlt">Ultra-High</span> Pressure Sensor for Microscale Detonation Pressure Measurement</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, Guodong; Zhao, Yulong; Zhao, Yun; Wang, Xinchen; Ren, Wei; Li, Hui; Zhao, You</p> <p>2018-01-01</p> <p>With the development of energetic materials (EMs) and microelectromechanical systems (MEMS) initiating explosive devices, the measurement of detonation pressure generated by EMs in the microscale has become a pressing need. This paper develops a manganin thin film <span class="hlt">ultra-high</span> pressure sensor based on MEMS technology for measuring the output pressure from micro-detonator. A reliable coefficient is proposed for designing the sensor’s sensitive element better. The sensor employs sandwich structure: the substrate uses a 0.5 mm thick alumina ceramic, the manganin sensitive element with a size of 0.2 mm × 0.1 mm × 2 μm and copper electrodes of 2 μm thick are sputtered sequentially on the substrate, and a 25 μm thick insulating layer of polyimide is wrapped on the sensitive element. The static test shows that the piezoresistive coefficient of manganin thin film is 0.0125 GPa−1. The dynamic experiment indicates that the detonation pressure of micro-detonator is 12.66 GPa, and the response time of the sensor is 37 ns. In a word, the sensor developed in this study is suitable for measuring <span class="hlt">ultra-high</span> pressure in microscale and has a shorter response time than that of foil-like manganin gauges. Simultaneously, this study could be beneficial to research on <span class="hlt">ultra-high</span>-pressure sensors with smaller size. PMID:29494519</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/ED579146.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/ED579146.pdf"><span>Documentation to the 2015-16 Common Core of Data (<span class="hlt">CCD</span>) Universe Files. NCES 2017-074</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>Glander, Mark</p> <p>2017-01-01</p> <p>The Common Core of Data (<span class="hlt">CCD</span>) is a national statistical program that collects and compiles administrative data from SEAs covering the universe of all public elementary and secondary schools and school districts in the United States. The first <span class="hlt">CCD</span> collection was for SY 1986-87. The predecessor to <span class="hlt">CCD</span> was the Elementary and Secondary General…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070031977&hterms=Silicide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DSilicide','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070031977&hterms=Silicide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DSilicide"><span><span class="hlt">Ultra-High</span> Temperature Materials Characterization for Space and Missile Applications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rogers, Jan; Hyers, Robert</p> <p>2007-01-01</p> <p>Numerous advanced space and missile technologies including propulsion systems require operations at <span class="hlt">high</span> temperatures. Some very <span class="hlt">high</span>-temperature materials are being developed to meet these needs, including refractory metal alloys, carbides, borides, and silicides. System design requires data for materials properties at operating temperatures. Materials property data are not available at the desired operating temperatures for many materials of interest. The objective of this work is to provide important physical property data at <span class="hlt">ultra-high</span> temperatures. The MSFC Electrostatic Levitation (ESL) facility can provide measurements of thermophysical properties which include: creep strength, emissivity, density and thermal expansion. ESL uses electrostatic fields to position samples between electrodes during processing and characterization experiments. Samples float between the electrodes during studies and are free from any contact with a container or test apparatus. This provides a <span class="hlt">high</span> purity environment for the study of <span class="hlt">high</span>-temperature, reactive materials. ESL can be used to process a wide variety of materials including metals, alloys, ceramics, glasses and semiconductors. A system for the determination of total hemispherical emissivity is being developed for the MSFC ESL facility by AZ Technology Inc. The instrument has been designed to provide emissivity measurements for samples during ESL experiments over the temperature range 700-3400K. A novel non-contact technique for the determination of <span class="hlt">high</span>-temperature creep strength has been developed. Data from selected ESL-based characterization studies will be presented. The ESL technique could advance space and missile technologies by advancing the knowledge base and the technology readiness level for <span class="hlt">ultra-high</span> temperature materials. Applications include non-eroding nozzle materials and lightweight, <span class="hlt">high</span>-temperature alloys for turbines and structures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28968651','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28968651"><span>Kinome expression profiling of human neuroblastoma tumors identifies potential drug targets for <span class="hlt">ultra</span> <span class="hlt">high</span>-risk patients.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Russo, Roberta; Cimmino, Flora; Pezone, Lucia; Manna, Francesco; Avitabile, Marianna; Langella, Concetta; Koster, Jan; Casale, Fiorina; Raia, Maddalena; Viola, Giampietro; Fischer, Matthias; Iolascon, Achille; Capasso, Mario</p> <p>2017-10-01</p> <p>Neuroblastoma (NBL) accounts for >7% of malignancies in patients younger than 15 years. Low- and intermediate-risk patients exhibit excellent or good prognosis after treatment, whereas for <span class="hlt">high</span>-risk (HR) patients, the estimated 5-year survival rates is still <40%. The ability to stratify HR patients that will not respond to standard treatment strategies is critical for informed treatment decisions. In this study, we have generated a specific kinome gene signature, named Kinome-27, which is able to identify a subset of HR-NBL tumors, named <span class="hlt">ultra</span>-HR NBL, with <span class="hlt">highly</span> aggressive clinical behavior that not adequately respond to standard treatments. We have demonstrated that NBL cell lines expressing the same kinome signature of <span class="hlt">ultra</span>-HR tumors (<span class="hlt">ultra</span>-HR-like cell lines) may be selectively targeted by the use of two drugs [suberoylanilide hydroxamic acid (SAHA) and Radicicol], and that the synergic combination of these drugs is able to block the <span class="hlt">ultra</span>-HR-like cells in G2/M phase of cell cycle. The use of our signature in clinical practice will allow identifying patients with negative outcome, which would benefit from new and more personalized treatments. Preclinical in vivo studies are needed to consolidate the SAHA and Radicicol treatment in <span class="hlt">ultra</span>-HR NBL patients. © The Author 2017. Published by Oxford University Press. All rights reserved. For Permissions, please email: journals.permissions@oup.com.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012SPIE.8383E..0QW','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012SPIE.8383E..0QW"><span><span class="hlt">Ultra-high</span> resolution and <span class="hlt">high</span>-brightness AMOLED</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wacyk, Ihor; Ghosh, Amal; Prache, Olivier; Draper, Russ; Fellowes, Dave</p> <p>2012-06-01</p> <p>As part of its continuing effort to improve both the resolution and optical performance of AMOLED microdisplays, eMagin has recently developed an SXGA (1280×3×1024) microdisplay under a US Army RDECOM CERDEC NVESD contract that combines the world's smallest OLED pixel pitch with an <span class="hlt">ultra-high</span> brightness green OLED emitter. This development is aimed at next-generation HMD systems with "see-through" and daylight imaging requirements. The OLED pixel array is built on a 0.18-micron CMOS backplane and contains over 4 million individually addressable pixels with a pixel pitch of 2.7 × 8.1 microns, resulting in an active area of 0.52 inches diagonal. Using both spatial and temporal enhancement, the display can provide over 10-bits of gray-level control for <span class="hlt">high</span> dynamic range applications. The new pixel design also enables the future implementation of a full-color QSXGA (2560 × RGB × 2048) microdisplay in an active area of only 1.05 inch diagonal. A low-power serialized low-voltage-differential-signaling (LVDS) interface is integrated into the display for use as a remote video link for tethered systems. The new SXGA backplane has been combined with the <span class="hlt">high</span>-brightness green OLED device developed by eMagin under an NVESD contract. This OLED device has produced an output brightness of more than 8000fL with all pixels on; lifetime measurements are currently underway and will presented at the meeting. This paper will describe the operational features and first optical and electrical test results of the new SXGA demonstrator microdisplay.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ApPhL.103j1104K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ApPhL.103j1104K"><span>Enhancement of absorption and color contrast in <span class="hlt">ultra</span>-thin <span class="hlt">highly</span> absorbing optical coatings</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kats, Mikhail A.; Byrnes, Steven J.; Blanchard, Romain; Kolle, Mathias; Genevet, Patrice; Aizenberg, Joanna; Capasso, Federico</p> <p>2013-09-01</p> <p>Recently a new class of optical interference coatings was introduced which comprises <span class="hlt">ultra</span>-thin, <span class="hlt">highly</span> absorbing dielectric layers on metal substrates. We show that these lossy coatings can be augmented by an additional transparent subwavelength layer. We fabricated a sample comprising a gold substrate, an <span class="hlt">ultra</span>-thin film of germanium with a thickness gradient, and several alumina films. The experimental reflectivity spectra showed that the additional alumina layer increases the color range that can be obtained, in agreement with calculations. More generally, this transparent layer can be used to enhance optical absorption, protect against erosion, or as a transparent electrode for optoelectronic devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22398990-ultra-thin-distributed-bragg-reflectors-via-stacked-single-crystal-silicon-nanomembranes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22398990-ultra-thin-distributed-bragg-reflectors-via-stacked-single-crystal-silicon-nanomembranes"><span><span class="hlt">Ultra</span>-thin distributed Bragg reflectors via stacked single-crystal silicon nanomembranes</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>Cho, Minkyu; Seo, Jung-Hun; Lee, Jaeseong</p> <p>2015-05-04</p> <p>In this paper, we report <span class="hlt">ultra</span>-thin distributed Bragg reflectors (DBRs) via stacked single-crystal silicon (Si) nanomembranes (NMs). Mesh hole-free single-crystal Si NMs were released from a Si-on-insulator substrate and transferred to quartz and Si substrates. Thermal oxidation was applied to the transferred Si NM to form <span class="hlt">high</span>-quality SiO{sub 2} and thus a Si/SiO{sub 2} pair with uniform and <span class="hlt">precisely</span> controlled thicknesses. The Si/SiO{sub 2} layers, as smooth as epitaxial grown layers, minimize scattering loss at the interface and in between the layers. As a result, a reflection of 99.8% at the wavelength range from 1350 nm to 1650 nm can be measuredmore » from a 2.5-pair DBR on a quartz substrate and 3-pair DBR on a Si substrate with thickness of 0.87 μm and 1.14 μm, respectively. The <span class="hlt">high</span> reflection, <span class="hlt">ultra</span>-thin DBRs developed here, which can be applied to almost any devices and materials, holds potential for application in <span class="hlt">high</span> performance optoelectronic devices and photonics applications.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160006055','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160006055"><span><span class="hlt">Precision</span> of FLEET Velocimetry Using <span class="hlt">High</span>-Speed CMOS Camera Systems</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Peters, Christopher J.; Danehy, Paul M.; Bathel, Brett F.; Jiang, Naibo; Calvert, Nathan D.; Miles, Richard B.</p> <p>2015-01-01</p> <p>Femtosecond laser electronic excitation tagging (FLEET) is an optical measurement technique that permits quantitative velocimetry of unseeded air or nitrogen using a single laser and a single camera. In this paper, we seek to determine the fundamental <span class="hlt">precision</span> of the FLEET technique using <span class="hlt">high</span>-speed complementary metal-oxide semiconductor (CMOS) cameras. Also, we compare the performance of several different <span class="hlt">high</span>-speed CMOS camera systems for acquiring FLEET velocimetry data in air and nitrogen free-jet flows. The <span class="hlt">precision</span> was defined as the standard deviation of a set of several hundred single-shot velocity measurements. Methods of enhancing the <span class="hlt">precision</span> of the measurement were explored such as digital binning (similar in concept to on-sensor binning, but done in post-processing), row-wise digital binning of the signal in adjacent pixels and increasing the time delay between successive exposures. These techniques generally improved <span class="hlt">precision</span>; however, binning provided the greatest improvement to the un-intensified camera systems which had low signal-to-noise ratio. When binning row-wise by 8 pixels (about the thickness of the tagged region) and using an inter-frame delay of 65 microseconds, <span class="hlt">precisions</span> of 0.5 meters per second in air and 0.2 meters per second in nitrogen were achieved. The camera comparison included a pco.dimax HD, a LaVision Imager scientific CMOS (sCMOS) and a Photron FASTCAM SA-X2, along with a two-stage LaVision <span class="hlt">High</span>Speed IRO intensifier. Excluding the LaVision Imager sCMOS, the cameras were tested with and without intensification and with both short and long inter-frame delays. Use of intensification and longer inter-frame delay generally improved <span class="hlt">precision</span>. Overall, the Photron FASTCAM SA-X2 exhibited the best performance in terms of greatest <span class="hlt">precision</span> and highest signal-to-noise ratio primarily because it had the largest pixels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160006537','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160006537"><span><span class="hlt">Precision</span> of FLEET Velocimetry Using <span class="hlt">High</span>-speed CMOS Camera Systems</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Peters, Christopher J.; Danehy, Paul M.; Bathel, Brett F.; Jiang, Naibo; Calvert, Nathan D.; Miles, Richard B.</p> <p>2015-01-01</p> <p>Femtosecond laser electronic excitation tagging (FLEET) is an optical measurement technique that permits quantitative velocimetry of unseeded air or nitrogen using a single laser and a single camera. In this paper, we seek to determine the fundamental <span class="hlt">precision</span> of the FLEET technique using <span class="hlt">high</span>-speed complementary metal-oxide semiconductor (CMOS) cameras. Also, we compare the performance of several different <span class="hlt">high</span>-speed CMOS camera systems for acquiring FLEET velocimetry data in air and nitrogen free-jet flows. The <span class="hlt">precision</span> was defined as the standard deviation of a set of several hundred single-shot velocity measurements. Methods of enhancing the <span class="hlt">precision</span> of the measurement were explored such as digital binning (similar in concept to on-sensor binning, but done in post-processing), row-wise digital binning of the signal in adjacent pixels and increasing the time delay between successive exposures. These techniques generally improved <span class="hlt">precision</span>; however, binning provided the greatest improvement to the un-intensified camera systems which had low signal-to-noise ratio. When binning row-wise by 8 pixels (about the thickness of the tagged region) and using an inter-frame delay of 65 micro sec, <span class="hlt">precisions</span> of 0.5 m/s in air and 0.2 m/s in nitrogen were achieved. The camera comparison included a pco.dimax HD, a LaVision Imager scientific CMOS (sCMOS) and a Photron FASTCAM SA-X2, along with a two-stage LaVision <span class="hlt">High</span> Speed IRO intensifier. Excluding the LaVision Imager sCMOS, the cameras were tested with and without intensification and with both short and long inter-frame delays. Use of intensification and longer inter-frame delay generally improved <span class="hlt">precision</span>. Overall, the Photron FASTCAM SA-X2 exhibited the best performance in terms of greatest <span class="hlt">precision</span> and highest signal-to-noise ratio primarily because it had the largest pixels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890052918&hterms=physics+astrophysics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dphysics%2Bastrophysics','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890052918&hterms=physics+astrophysics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dphysics%2Bastrophysics"><span>Performance characteristics of CCDs for the ACIS experiment. [Advanced X-ray Astrophysics Facility <span class="hlt">CCD</span> Imaging Spectrometer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Garmire, Gordon P.; Nousek, John; Burrows, David; Ricker, George; Bautz, Mark; Doty, John; Collins, Stewart; Janesick, James</p> <p>1988-01-01</p> <p>The search for the optimum <span class="hlt">CCD</span> to be used at the focal surface of the Advanced X-ray Astrophysics Facility (AXAF) is described. The physics of the interaction of X-rays in silicon through the photoelectric effect is reviewed. <span class="hlt">CCD</span> technology at the beginning of the AXAF definition phase is summarized, and the results of the <span class="hlt">CCD</span> enhancement program are discussed. Other sources of optimum CCDs are examined, and <span class="hlt">CCD</span> enhancements made at MIT Lincoln Laboratory are addressed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840020210','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840020210"><span><span class="hlt">High</span> <span class="hlt">precision</span> measurements in crustal dynamic studies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wyatt, F.; Berger, J.</p> <p>1984-01-01</p> <p>The development of <span class="hlt">high-precision</span> instrumentation for monitoring benchmark stability and evaluating coseismic strain and tilt signals is reviewed. Laser strainmeter and tilt observations are presented. Examples of coseismic deformation in several geographic locations are given. Evidence suggests that the Earth undergoes elastic response to abrupt faulting.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29861810','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29861810"><span>Dotette: Programmable, <span class="hlt">high-precision</span>, plug-and-play droplet pipetting.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fan, Jinzhen; Men, Yongfan; Hao Tseng, Kuo; Ding, Yi; Ding, Yunfeng; Villarreal, Fernando; Tan, Cheemeng; Li, Baoqing; Pan, Tingrui</p> <p>2018-05-01</p> <p>Manual micropipettes are the most heavily used liquid handling devices in biological and chemical laboratories; however, they suffer from low <span class="hlt">precision</span> for volumes under 1  μ l and inevitable human errors. For a manual device, the human errors introduced pose potential risks of failed experiments, inaccurate results, and financial costs. Meanwhile, low <span class="hlt">precision</span> under 1  μ l can cause severe quantification errors and <span class="hlt">high</span> heterogeneity of outcomes, becoming a bottleneck of reaction miniaturization for quantitative research in biochemical labs. Here, we report Dotette, a programmable, plug-and-play microfluidic pipetting device based on nanoliter liquid printing. With automated control, protocols designed on computers can be directly downloaded into Dotette, enabling programmable operation processes. Utilizing continuous nanoliter droplet dispensing, the <span class="hlt">precision</span> of the volume control has been successfully improved from traditional 20%-50% to less than 5% in the range of 100 nl to 1000 nl. Such a <span class="hlt">highly</span> automated, plug-and-play add-on to existing pipetting devices not only improves <span class="hlt">precise</span> quantification in low-volume liquid handling and reduces chemical consumptions but also facilitates and automates a variety of biochemical and biological operations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JNuM..487..229Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JNuM..487..229Y"><span><span class="hlt">Ultra-high</span> temperature tensile properties of ODS steel claddings under severe accident conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yano, Y.; Tanno, T.; Oka, H.; Ohtsuka, S.; Inoue, T.; Kato, S.; Furukawa, T.; Uwaba, T.; Kaito, T.; Ukai, S.; Oono, N.; Kimura, A.; Hayashi, S.; Torimaru, T.</p> <p>2017-04-01</p> <p><span class="hlt">Ultra-high</span> temperature ring tensile tests were performed to investigate the tensile behavior of oxide dispersion strengthened (ODS) steel claddings and wrapper materials under severe accident conditions with temperatures ranging from room temperature to 1400 °C which is close to the melting point of core materials. The experimental results showed that the tensile strength of 9Cr-ODS steel claddings was highest in the core materials at <span class="hlt">ultra-high</span> temperatures of 900-1200 °C, but there was significant degradation in the tensile strength of 9Cr-ODS steel claddings above 1200 °C. This degradation was attributed to grain boundary sliding deformation with γ/δ transformation, which is associated with reduced ductility. By contrast, the tensile strength of recrystallized 12Cr-ODS and FeCrAl-ODS steel claddings retained its <span class="hlt">high</span> value above 1200 °C, unlike the other tested materials.</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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