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Dive into the research topics where Kirk Gilmore is active.

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Featured researches published by Kirk Gilmore.


Proceedings of SPIE | 2010

Soft gamma-ray detector for the ASTRO-H mission

Hiroyasu Tajima; R. D. Blandford; Teruaki Enoto; Yasushi Fukazawa; Kirk Gilmore; Tuneyoshi Kamae; J. Kataoka; Madoka Kawaharada; Motohide Kokubun; Philippe Laurent; Francois Lebrun; Olivier Limousin; Greg M. Madejski; Kazuo Makishima; T. Mizuno; Kazuhiro Nakazawa; M. Ohno; Masayuki Ohta; Goro Sato; Rie Sato; H. Takahashi; Tadayuki Takahashi; T. Tanaka; Makoto Tashiro; Yukikatsu Terada; Y. Uchiyama; Shin Watanabe; Kazutaka Yamaoka; Daisuke Yonetoku

The Soft Gamma-ray Detector (SGD) on board ASTRO-H (Japanese next high-energy astrophysics mission) is a Compton telescope with narrow fleld-of-view, which utilizes Compton kinematics to enhance its background rejection capabilities. It is realized as a hybrid semiconductor detector system which consists of silicon and CdTe (cadmium telluride) detectors. It can detect photons in a wide energy band (50-600 keV) at a background level 10 times better than that of the Suzaku Hard X-ray Detector, and is complimentary to the Hard X-ray Imager on board ASTRO-H with an energy coverage of 5-80 keV. Excellent energy resolution is the key feature of the SGD, allowing it to achieve good background rejection capability taking advantage of good angular resolution. An additional capability of the SGD, its ability to measure gamma-ray polarization, opens up a new window to study properties of gamma-ray emission processes. Here we describe the instrument design of the SGD, its expected performance, and its development status.


Proceedings of SPIE | 2010

Hard x-ray imager (HXI) for the ASTRO-H Mission

Motohide Kokubun; Kazuhiro Nakazawa; Teruaki Enoto; Yasushi Fukazawa; Kirk Gilmore; J. Kataoka; Madoka Kawaharada; Philippe Laurent; Francois Lebrun; Olivier Limousin; Kazuo Makishima; T. Mizuno; K. Mori; T. Nakamori; M. Ohno; Masayuki Ohta; Goro Sato; Hiroyasu Tajima; H. Takahashi; Tadayuki Takahashi; T. Tanaka; Yukikatsu Terada; Hideki Uchiyama; Y. Uchiyama; Shin Watanabe; Yoichi Yatsu; Kazutaka Yamaoka

The Hard X-ray Imager (HXI) is one of four detectors on board the ASTRO-H mission (6th Japanese X-ray satellite), which is scheduled to be launched in 2014. Using the hybrid structure composed of double-sided silicon strip detectors and a cadmium telluride double-sided strip detector, the instrument fully covers the energy range of photons collected with the hard X-ray telescope up to 80 keV with a high quantum efficiency. High spatial resolution of 250 μm and an energy resolution of 1-2 keV (FWHM) are both achieved with low noise front-end ASICs. In addition, the thick BGO active shields surrounding the main detector package is a heritage of the successful performance of the Hard X-ray Detector on board the Suzaku satellite. This feature enables the instrument to achieve an extremely high background reduction caused by cosmic-ray particles, cosmic X-ray background, and in-orbit radiation activation. In this paper, we present the detector concept, design, latest results of the detector development, and the current status of the hardware.


Monthly Notices of the Royal Astronomical Society | 2013

Spurious shear in weak lensing with the large synoptic survey telescope

C. Chang; S. M. Kahn; J. G. Jernigan; J. R. Peterson; Yusra AlSayyad; Z. Ahmad; J. Bankert; Deborah Bard; Andrew J. Connolly; Robert R. Gibson; Kirk Gilmore; E. Grace; M. Hannel; M. A. Hodge; M. J. Jee; Lynne Jones; S. K. Krughoff; S. Lorenz; Philip J. Marshall; S. L. Marshall; A. Meert; S. Nagarajan; E. Peng; Andrew P. A Rasmussen; Marina Shmakova; N. Sylvestre; N. Todd; M. Young

The complete 10-year survey from the Large Synoptic Survey Telescope (LSST) will image {approx} 20,000 square degrees of sky in six filter bands every few nights, bringing the final survey depth to r {approx} 27.5, with over 4 billion well measured galaxies. To take full advantage of this unprecedented statistical power, the systematic errors associated with weak lensing measurements need to be controlled to a level similar to the statistical errors. This work is the first attempt to quantitatively estimate the absolute level and statistical properties of the systematic errors on weak lensing shear measurements due to the most important physical effects in the LSST system via high fidelity ray-tracing simulations. We identify and isolate the different sources of algorithm-independent, additive systematic errors on shear measurements for LSST and predict their impact on the final cosmic shear measurements using conventional weak lensing analysis techniques. We find that the main source of the errors comes from an inability to adequately characterise the atmospheric point spread function (PSF) due to its high frequency spatial variation on angular scales smaller than {approx} 10{prime} in the single short exposures, which propagates into a spurious shear correlation function at the 10{sup -4}-10{sup -3} level on these scales. With the large multi-epoch dataset that will be acquired by LSST, the stochastic errors average out, bringing the final spurious shear correlation function to a level very close to the statistical errors. Our results imply that the cosmological constraints from LSST will not be severely limited by these algorithm-independent, additive systematic effects.


The Astrophysical Journal | 2013

EFFECT OF MEASUREMENT ERRORS ON PREDICTED COSMOLOGICAL CONSTRAINTS FROM SHEAR PEAK STATISTICS WITH LARGE SYNOPTIC SURVEY TELESCOPE

D. Bard; Jan M. Kratochvil; C. Chang; M. May; S. M. Kahn; Yusra AlSayyad; Z. Ahmad; J. Bankert; Andrew J. Connolly; Robert R. Gibson; Kirk Gilmore; E. Grace; Zoltan Haiman; M. Hannel; K. M. Huffenberger; J. G. Jernigan; Lynne Jones; S. K. Krughoff; S. Lorenz; S. L. Marshall; A. Meert; S. Nagarajan; E. Peng; J. R. Peterson; Andrew P. A Rasmussen; Marina Shmakova; N. Sylvestre; N. Todd; M. Young

We study the effect of galaxy shape measurement errors on predicted cosmological constraints from the statistics of shear peak counts with the Large Synoptic Survey Telescope (LSST). We use the LSST Image Simulator in combination with cosmological N-body simulations to model realistic shear maps for different cosmological models. We include both galaxy shape noise and, for the first time, measurement errors on galaxy shapes. We find that the measurement errors considered have relatively little impact on the constraining power of shear peak counts for LSST.


Proceedings of SPIE | 2014

A framework for modeling the detailed optical response of thick, multiple segment, large format sensors for precision astronomy applications

Andrew P. A Rasmussen; P. Antilogus; Pierre Astier; Chuck Claver; Peter Doherty; Gregory P. Dubois-Felsmann; Kirk Gilmore; Steven M. Kahn; I.V. Kotov; Robert H. Lupton; Paul O'Connor; A. Nomerotski; Steve Ritz; Christopher W. Stubbs

Near-future astronomical survey experiments, such as LSST, possess system requirements of unprecedented fidelity that span photometry, astrometry and shape transfer. Some of these requirements flow directly to the array of science imaging sensors at the focal plane. Availability of high quality characterization data acquired in the course of our sensor development program has given us an opportunity to develop and test a framework for simulation and modeling that is based on a limited set of physical and geometric effects. In this paper we describe those models, provide quantitative comparisons between data and modeled response, and extrapolate the response model to predict imaging array response to astronomical exposure. The emergent picture departs from the notion of a fixed, rectilinear grid that maps photo-conversions to the potential well of the channel. In place of that, we have a situation where structures from device fabrication, local silicon bulk resistivity variations and photo-converted carrier patterns still accumulating at the channel, together influence and distort positions within the photosensitive volume that map to pixel boundaries. Strategies for efficient extraction of modeling parameters from routinely acquired characterization data are described. Methods for high fidelity illumination/image distribution parameter retrieval, in the presence of such distortions, are also discussed.


Proceedings of SPIE | 2008

Optical design of the LSST camera

Scot S. Olivier; Lynn G. Seppala; Kirk Gilmore

The Large Synoptic Survey Telescope (LSST) uses a novel, three-mirror, modified Paul-Baker design, with an 8.4- meter primary mirror, a 3.4-m secondary, and a 5.0-m tertiary feeding a camera system that includes a set of broad-band filters and refractive corrector lenses to produce a flat focal plane with a field of view of 9.6 square degrees. Optical design of the camera lenses and filters is integrated with optical design of telescope mirrors to optimize performance, resulting in excellent image quality over the entire field from ultra-violet to near infra-red wavelengths. The LSST camera optics design consists of three refractive lenses with clear aperture diameters of 1.55 m, 1.10 m and 0.69 m and six interchangeable, broad-band, filters with clear aperture diameters of 0.75 m. We describe the methodology for fabricating, coating, mounting and testing these lenses and filters, and we present the results of detailed tolerance analyses, demonstrating that the camera optics will perform to the specifications required to meet their performance goals.


Proceedings of SPIE | 2006

LSST Camera Optics

Scot S. Olivier; Lynn G. Seppala; Kirk Gilmore; Layton C. Hale; Wayne Whistler

The Large Synoptic Survey Telescope (LSST) is a unique, three-mirror, modified Paul-Baker design with an 8.4m primary, a 3.4m secondary, and a 5.0m tertiary feeding a camera system that includes corrector optics to produce a 3.5 degree field of view with excellent image quality (<0.3 arcsecond 80% encircled diffracted energy) over the entire field from blue to near infra-red wavelengths. We describe the design of the LSST camera optics, consisting of three refractive lenses with diameters of 1.6m, 1.0m and 0.7m, along with a set of interchangeable, broad-band, interference filters with diameters of 0.75m. We also describe current plans for fabricating, coating, mounting and testing these lenses and filters.


Proceedings of SPIE | 2008

The LSST camera overview: design and performance

Kirk Gilmore; Steven M. Kahn; Martin Nordby; Paul O'Connor; J. Oliver; V. Radeka; Terry Schalk; R. Schindler; Rick Van Berg

The LSST camera is a wide-field optical (0.35-1μm) imager designed to provide a 3.5 degree FOV with 0.2 arcsecond/pixel sampling. The detector format will be a circular mosaic providing approximately 3.2 Gigapixels per image. The camera includes a filter mechanism and shuttering capability. It is positioned in the middle of the telescope where cross-sectional area is constrained by optical vignetting and where heat dissipation must be controlled to limit thermal gradients in the optical beam. The fast f/1.2 beam will require tight tolerances on the focal plane mechanical assembly. The focal plane array operates at a temperature of approximately -100°C to achieve desired detector performance. The focal plane array is contained within a cryostat which incorporates detector front-end electronics and thermal control. The cryostat lens serves as an entrance window and vacuum seal for the cryostat. Similarly, the camera body lens serves as an entrance window and gas seal for the camera housing, which is filled with a suitable gas to provide the operating environment for the shutter and filter change mechanisms. The filter carousel accommodates 5 filters, each 75 cm in diameter, for rapid exchange without external intervention.


Proceedings of SPIE | 2006

The LSST camera system overview

Kirk Gilmore; Steven M. Kahn; Martin Nordby; David L. Burke; Paul O'Connor; J. Oliver; V. Radeka; Terry Schalk; R. Schindler

The LSST camera is a wide-field optical (0.35-1um) imager designed to provide a 3.5 degree FOV with better than 0.2 arcsecond sampling. The detector format will be a circular mosaic providing approximately 3.2 Gigapixels per image. The camera includes a filter mechanism and, shuttering capability. It is positioned in the middle of the telescope where cross-sectional area is constrained by optical vignetting and heat dissipation must be controlled to limit thermal gradients in the optical beam. The fast, f/1.2 beam will require tight tolerances on the focal plane mechanical assembly. The focal plane array operates at a temperature of approximately -100°C to achieve desired detector performance. The focal plane array is contained within an evacuated cryostat, which incorporates detector front-end electronics and thermal control. The cryostat lens serves as an entrance window and vacuum seal for the cryostat. Similarly, the camera body lens serves as an entrance window and gas seal for the camera housing, which is filled with a suitable gas to provide the operating environment for the shutter and filter change mechanisms. The filter carousel can accommodate 5 filters, each 75 cm in diameter, for rapid exchange without external intervention.


Proceedings of SPIE | 2016

Integration and verification testing of the Large Synoptic Survey Telescope camera

Travis Lange; Tim Bond; James Chiang; Kirk Gilmore; Seth W. Digel; Richard Dubois; Tom Glanzman; Tony Johnson; Margaux Lopez; Scott P. Newbry; Martin Nordby; Andrew P. A Rasmussen; K. Reil; A. Roodman

We present an overview of the Integration and Verification Testing activities of the Large Synoptic Survey Telescope (LSST) Camera at the SLAC National Accelerator Lab (SLAC). The LSST Camera, the sole instrument for LSST and under construction now, is comprised of a 3.2 Giga-pixel imager and a three element corrector with a 3.5 degree diameter field of view. LSST Camera Integration and Test will be taking place over the next four years, with final delivery to the LSST observatory anticipated in early 2020. We outline the planning for Integration and Test, describe some of the key verification hardware systems being developed, and identify some of the more complicated assembly/integration activities. Specific details of integration and verification hardware systems will be discussed, highlighting some of the technical challenges anticipated.

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J. G. Jernigan

University of California

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