2014
DOI: 10.1117/12.2057259
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Design improvements and x-ray performance of a time projection chamber polarimeter for persistent astronomical sources

Abstract: The design of the Time-Projection Chamber (TPC) Polarimeter for the Gravity and Extreme Magnetism Small Explorer (GEMS) was demonstrated to Technology Readiness Level 6 (TRL-6) 3 and the flight detectors fabricated, assembled and performance tested. A single flight detector was characterized at the Brookhaven National Laboratory Synchrotron Light Source with polarized X-rays at 10 energies from 2.3-8.0 keV at five detector positions. The detector met all of the GEMS performance requirements. Lifetime measureme… Show more

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Cited by 8 publications
(11 citation statements)
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“…This improvement is reported in detail in Hill et al 2014 18 where we need only one free parameter to calibrate the polarimeter.…”
Section: Detector Performancementioning
confidence: 55%
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“…This improvement is reported in detail in Hill et al 2014 18 where we need only one free parameter to calibrate the polarimeter.…”
Section: Detector Performancementioning
confidence: 55%
“…[14][15][16] Although the GEMS mission, originally planned to be launched in 2013, was not confirmed for implementation, the verification and development of the polarimeter has continued. [17][18][19] The X-ray polarimeter at the GEMS focal plane is a gas proportional counter enhanced by a time projection chamber (TPC) technique. 1 Figure 1 illustrates a readout concept of the TPC X-ray polarimeter.…”
Section: Introductionmentioning
confidence: 99%
“…To maximize sensitivity we have developed a gas polarimeter that employs the Time Projection Chamber (TPC) technique [8,9,10,11,12]. In this case the detection plane is parallel to the incident X-rays.…”
Section: Introductionmentioning
confidence: 99%
“…In this case, the training set is a set of photoelectron track images with initial direction and 2-D position. The photoelectric polarimeter that we have developed can make a photoelectron track with 30 × 30 pixels of a size of 121 × 121 µm [7]. Although, in actual experiment, we can easily regulate the Xray polarization direction, we cannot control the photoelectron direction which is randomized according to the differential cross section, cos 2 (φ).…”
Section: Input Data: Photoelectron Track Imagesmentioning
confidence: 99%