TY - JOUR
T1 - Hard X-ray response of CdZnTe detectors in the swift burst alert telescope
AU - Suzuki, Masaya
AU - Tashiro, Makoto
AU - Sato, Goro
AU - Watanabe, Shin
AU - Takahashi, Tadayuki
AU - Okada, Yuu
AU - Takahashi, Hiromitsu
AU - Parsons, Ann
AU - Barthelmy, Scott
AU - Cummings, Jay
AU - Gehrels, Neil
AU - Hullinger, Derek
AU - Krimm, Hans
AU - Tueller, Jack
PY - 2003
Y1 - 2003
N2 - The Burst Alert Telescope (BAT) onboard the Swift Gamma-ray Burst Explorer (scheduled for launch in May of 2004) has a coded aperture mask and a detector array of 32,768 Cd 0.9Zn 0.1Te 1.0 (4×4mm 2 large, 2mm thick) semiconductor devices. Due to small mobility and short lifetime of carriers, the electron-hole pairs generated by irradiation of gamma-rays cannot be completely collected. Since the shape of the measured spectra has the broad low-energy tail, it is very useful for us to estimate the obtained spectra to fit the model which considers the charge transport properties depended on the depth of the photon interaction (G.Sato, 2002). The energy calibration of the BAT array and coded mask experiments were carried out at NASA/Goddard Space Flight Center between December 2002 and March 2003. We applied the model fitting to the calibration spectra, to yield the mobility-lifetime products for each detector and these values differ by over 2 orders of magnitude among detectors. Also using the mobility-lifetime parameters, we can identified the detector energy response as a fucntion of the temperature and illumination angle. But we figure out a difference between the model and the obtained data. To determine the difference between the model and the measured data, we conducted the detailed check experiment for a single CdZnTe, to show that the cause of the excess is due to the areal nonuniformity of the mobility-lifetime parameter.
AB - The Burst Alert Telescope (BAT) onboard the Swift Gamma-ray Burst Explorer (scheduled for launch in May of 2004) has a coded aperture mask and a detector array of 32,768 Cd 0.9Zn 0.1Te 1.0 (4×4mm 2 large, 2mm thick) semiconductor devices. Due to small mobility and short lifetime of carriers, the electron-hole pairs generated by irradiation of gamma-rays cannot be completely collected. Since the shape of the measured spectra has the broad low-energy tail, it is very useful for us to estimate the obtained spectra to fit the model which considers the charge transport properties depended on the depth of the photon interaction (G.Sato, 2002). The energy calibration of the BAT array and coded mask experiments were carried out at NASA/Goddard Space Flight Center between December 2002 and March 2003. We applied the model fitting to the calibration spectra, to yield the mobility-lifetime products for each detector and these values differ by over 2 orders of magnitude among detectors. Also using the mobility-lifetime parameters, we can identified the detector energy response as a fucntion of the temperature and illumination angle. But we figure out a difference between the model and the obtained data. To determine the difference between the model and the measured data, we conducted the detailed check experiment for a single CdZnTe, to show that the cause of the excess is due to the areal nonuniformity of the mobility-lifetime parameter.
KW - BAT
KW - CdZnTe
KW - Energy calibration
KW - Gamma-ray detector
KW - Mobility-lifetime products
KW - Spectral modeling
KW - Swift
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M3 - Article
AN - SCOPUS:19944425918
VL - 5
SP - 3550
EP - 3554
JO - Unknown Journal
JF - Unknown Journal
M1 - R14-2
ER -