Richard F. Foster
Massachusetts Institute of Technology
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Featured researches published by Richard F. Foster.
Astronomical Telescopes and Instrumentation | 2000
Gregory Y. Prigozhin; Steven E. Kissel; Mark W. Bautz; Catherine E. Grant; Beverly LaMarr; Richard F. Foster; George R. Ricker; Gordon Garmire
Front side illuminated CCDs comprising focal plane of Chandra X-ray telescope have suffered some radiation damage in the beginning of the mission. Measurements of CTI and dark current at different temperatures led us to conclusion that the type of damage is inconsistent with the much studied type of damage created by protons with energies higher than 10 MeV. Intensive ground based investigation showed that irradiation of CCD with low energy protons (about 100 keV) results in the device characteristics very similar to the ones of the flight chips (very low dark current, the shape of the CTI temperature dependence). We were able to reliably determine that only image section of the flight chips was damaged and therefore only fast transfer from image to frame store section was affected. We have developed several techniques in order to determine the parameters of the electron traps introduced into the transfer channel of the irradiated device.
Astronomical Telescopes and Instrumentation | 2003
Tadayasu Dotani; Masanobu Ozaki; Hiroshi Murakami; Katsuji Koyama; Takeshi Go Tsuru; H. Matsumoto; Hiroshi Tsunemi; Kiyoshi Hayashida; Emi Miyata; Shunji Kitamoto; Hisamitsu Awaki; Mark W. Bautz; John P. Doty; George R. Ricker; Richard F. Foster; Gregory Y. Prigozhin; Steven E. Kissel; Barry E. Burke; Allen D. Pillsbury
We report on design updates for the XIS (X-ray Imaging Spectrometer) on-board the Astro-E2 satellite. Astro-E2 is a recovery mission of Astro-E, which was lost during launch in 2000. Astro-E2 carries a total of 5 X-ray telescopes, 4 of which have XIS sensors as their focal plane detectors. Each XIS CCD camera covers a field of view of 19×19 arcmin in the energy range of 0.4-12 keV. The design of the Astro-E2 XIS is basically the same as that for Astro-E, but some improvements will be implemented. These are (1) CCD charge injection capability, (2) a revised heat-sink assembly, and (3) addition of a 55Fe radio-isotope on the door. Charge injection may be used to compensate for and calibrate radiation-induced degradation of the CCD charge transfer efficiency. This degradation is expected to become significant after a few years operation in space. The new heat-sink assembly is expected to increase the mechanical reliability and cooling capability of the XIS sensor. The new radio-isotope on the door will provide better calibration data. We present details of these improvements and summarize the overall design of the XIS.
SPIE's International Symposium on Optical Science, Engineering, and Instrumentation | 1998
Kiyoshi Hayashida; Shunji Kitamoto; Emi Miyata; Hiroshi Tsunemi; K. Hashimotodani; Kazunori Katayama; Takayoshi Kohmura; Reiko Asakura; Kumi Yoshita; Haruyoshi Katayama; Makoto Shouho; Katsuji Koyama; Takeshi Go Tsuru; Hisamitsu Awaki; Tadayasu Dotani; Masanobu Ozaki; George R. Ricker; John P. Doty; Mark W. Bautz; Steven E. Kissel; Richard F. Foster
The x-ray imaging spectrometers (XIS) are x-ray CCD cameras on-board the Astro-E satellite launched in 2000. The XIS consists of 4 cameras, each of them will be installed on a focal plane of the Astro-E X-ray Telescope (XRT). The XIS not only have a higher sensitivity, which comes from a larger effective area of the XRT and thicker depletion layers of the XIS CCDs, than ASCA SIS. But also have several features that will overcome the radiation damage effects anticipated in the orbit. The calibration experiment at Osaka focuses on the soft x-ray response of the XIS. The calibration system employs a grating spectrometer which irradiates the CCD with dispersed x-rays. We have obtained preliminary results on the XIS proto model, including the energy-pulse-height relation, the energy-resolution relation, and the quantum efficiency at the energy range of 0.25-2.2 keV.
IEEE Transactions on Nuclear Science | 2013
S. Ryu; Takeshi Go Tsuru; Gregory Y. Prigozhin; Steve Kissel; Marshall W. Bautz; Beverly LaMarr; Shinya Nakashima; Richard F. Foster; Ayaki Takeda; Yasuo Arai; Toshifumi Imamura; Takafumi Ohmoto; Atsushi Iwata
We have been developing monolithic active pixel sensors with 0.2 μm Silicon-On-Insulator (SOI) CMOS technology, called SOIPIX, for high-speed wide-band X-ray imaging spectroscopy on future astronomical satellites. In this work, we investigate a revised chip (XRPIX1b) for soft X-rays used in frontside illumination. The Al Kα line at 1.5 keV is successfully detected and energy resolution of 188 eV (FWHM) is achieved from a single pixel at this energy. The responsivity is improved to 6 μV/electron and the readout noise is 18 electrons rms. Data from 3 ×3 pixels irradiated with 6.4 keV (Fe Kα) X-rays demonstrates that the circuitry crosstalk between adjacent pixels is less than 0.5%.
Astronomical Telescopes and Instrumentation | 2000
Kiyoshi Hayashida; Shunji Kitamoto; Emi Miyata; Hiroshi Tsunemi; Kumi Yoshita; Takayoshi Kohmura; Kouji Mori; Kazunori Katayama; Haruyoshi Katayama; Makoto Shouho; Motoari Ohta; Tadayasu Dotani; Masanobu Ozaki; Katsuji Koyama; Hisamitsu Awaki; Takeshi Go Tsuru; George R. Ricker; Mark W. Bautz; Richard F. Foster; Steven E. Kissel
Soft X-ray response of X-ray Imaging Spectrometers (XIS) for the Astro-E satellite is measured with a grating spectrometer system at Osaka. First, relation between incident X-ray energy and output pulse height peak (E-PH relation) is examined with an SX grating. It is found that jump in the E-PH relation around Si-K edge is at most 2.7 eV. Second, quantum efficiency (QE) of the XIS in 0.4 - 2.2 keV range is measured relatively to the reference CCD of which absolute QE was calibrated with a gas proportional counter. The QE is fitted with a model in which CCD gate structures are considered. Systematic error on the QE results is estimated by referring an independent measurement. Third, tuning and improvement of the response function is performed. We employ six components to reproduce the response profile of the XIS. In this paper, improvement of one component which is originated in the events absorbed in the channel-stop is presented. Nevertheless, Astro-E was lost due to the launch failure. We overview the XIS project in its flight model phase, modified points of the design, problems and solutions etc., in order to be utilized in a possible recovery of the satellite.
Space Telescopes and Instrumentation 2018: Ultraviolet to Gamma Ray | 2018
Marshall W. Bautz; Andrew Malonis; Richard F. Foster; Beverly LaMarr; Gregory Y. Prigozhin; Catherine E. Grant; Eric D. Miller; Barry E. Burke; Michael J. Cooper; David M. Craig; Christopher Leitz; Daniel R. Schuette; Vyshnavi Suntharalingam
Future X-ray missions such as Lynx require large-format imaging detectors with performance at least as good as the best current-generation devices but with much higher readout rates. We are investigating a Digital CCD detector architecture, under development at MIT Lincoln Laboratory, for use in such missions. This architecture features a CMOS-compatible detector integrated with parallel CMOS signal processing chains. Fast, low-noise amplifiers and highly parallel signal processing provide the high frame-rates required. CMOS-compatibility of the CCD provides low-power charge transfer and signal processing. We report on the performance of CMOS-compatible test CCDs read at rates up to 5 Mpix s−1 (50 times faster than Chandra ACIS CCDs), with transfer clock swings as low as ±1.5 V (power/area < 10% of that of ACIS CCDs). We measure read noise below 6 electrons RMS at 2.5 MHz and X-ray spectral resolution better than 150 eV FWHM at 5.9 keV for single-pixel events. We discuss expected detector radiation tolerance at these relatively high transfer rates. We point out that the high pixel ’aspect ratio’ (depletion-depth : pixel size ≈ 9 : 1) of our test devices is similar to that expected for Lynx detectors, and illustrate some of the implications of this geometry for X-ray performance and noise requirements.
Astronomical Telescopes and Instrumentation | 2000
J. E. Hill; Kevin T. Lewis; Richard F. Foster; Mark W. Bautz; S. K. Brown; Peter W. A. Roming; Ann Elizabeth Hornschemeier; David N. Burrows; Gordon Garmire
The energy resolution degradation of the ACIS CCDs on board the Chandra X-ray Observatory has been under investigation since the effect was first recognized two months after launch. A series of laboratory CCD irradiations with electrons and protons have taken place, leading to the belief that low energy protons are responsible for the damage. In order to confirm this, an experiment has been devised to represent the flight experience of the ACIS CCDs, and the results to date are shown here.
Proceedings of SPIE | 2016
Gregory Y. Prigozhin; Keith C. Gendreau; John P. Doty; Richard F. Foster; Ronald A. Remillard; Andrew Malonis; Beverly LaMarr; Michael L. Vezie; Mark Egan; Jesus Noel Samonte Villasenor; Zaven Arzoumanian; Wayne H. Baumgartner; Frank Scholze; Christian Laubis; Michael Krumrey; Alan Huber
An instrument called Neutron Star Interior Composition ExploreR (NICER) will be placed on-board the Inter- national Space Station in 2017. It is designed to detect soft X-ray emission from compact sources and to provide both spectral and high resolution timing information about the incoming ux. The focal plane is populated with 56 customized Silicon Drift Detectors. The paper describes the detector system architecture, the electronics and presents the results of the laboratory testing of both ight and engineering units, as well as some of the calibration results obtained with synchrotron radiation in the laboratory of PTB at BESSY II.
Astronomical Telescopes and Instrumentation | 2000
Kouji Mori; Makoto Shouho; Haruyoshi Katayama; Shunji Kitamoto; Hiroshi Tsunemi; Kiyoshi Hayashida; Emi Miyata; Motoari Ohta; Takayoshi Kohmura; Katsuji Koyama; Mark W. Bautz; Richard F. Foster; Steven E. Kissel
We measure various spectral response characteristics around the oxygen and silicon K absorption edges of a Charge- Coupled Device X-ray detector used in the X-ray Imaging Spectrometer developed for the ASTRO-E mission. We have evaluated X-ray Absorption Fine Structure (XAFS) around oxygen K edge in detail. A strong absorption peak of 45% is confirmed just above the oxygen K edge and an oscillatory structure follows whose amplitude decreases from 20% at the edge to less than 1% at 0.9 keV. We also show XAFS and discuss on a change of the response function around the silicon K edge. The discontinuity of the signal pulse height at the silicon K edge is less than 1.8 eV. We determine the thickness of silicon, silicon dioxide, and silicon nitride in the dead layer using the depth of the absorption edge.
SPIE's International Symposium on Optical Science, Engineering, and Instrumentation | 1999
Haruyoshi Katayama; Makoto Shouho; Takayoshi Kohmura; Kazunori Katayama; Motoari Ohta; Hiroshi Tsunemi; Shunji Kitamoto; Kiyoshi Hayashida; Emi Miyata; Kumi Yoshita; Katsuji Koyama; George R. Ricker; Mark W. Bautz; Richard F. Foster; Steven E. Kissel; John P. Doty
The ASTRO-E X-ray Imaging Spectrometers (XISs) consists of four sets of X-ray CCD camera for the ASTRO-E mission. The XISs have been calibrated at Osaka University, Kyoto University, ISAS and MIT. The calibration experiment at Osaka focuses on the soft x-ray response of the XIS. The calibration of the XIS flight model has been performed since August 1998. We measured the signal-pulse height, the energy resolution and the quantum efficiency of the XIS as a function of energy, all of which are essential to construct the response function of the XIS. The detailed shape of the pulse-height-distribution are also investigated. We also constructed a numerical simulator of the XIS, which tracks the physical process in the CCD so as to reproduce the measured data. With a help of this simulator, we propose a model of the pulse-height-distribution of the XIS for single energy incident x-rays. The model consists of four components; two Gaussians, a constant, plus a triangle-shape component.