Ústav technické a experimentální fyziky Institute of Experimental and Applied Physics

Characterization of a 5 mm thick CZT-Timepix3 pixel detector for energy-dispersive γ-ray and particle tracking

NázevTitle
Characterization of a 5 mm thick CZT-Timepix3 pixel detector for energy-dispersive γ-ray and particle trackingCharacterization of a 5 mm thick CZT-Timepix3 pixel detector for energy-dispersive γ-ray and particle tracking
Druh výsledkuResult type
Článek v časopiseJournal article
AutořiAuthors
P. Smolyanskiy, B. Bergmann, P. Burian, A. Cherlin, J. Jelínek, S. Pospíšil
DOIDOI
10.1088/1402-4896/ad10dd
Časopis / citaceJournal / citation
Physica Scripta. 2024, 99(1), ISSN 1402-4896.
RokYear
2024
JazykLanguage
eng
WoSWoS
001126367700001
ScopusScopus
2-s2.0-85180270033
RIVRIV
RIV/68407700:21670/24:00371935!RIV25-GA0-21670___
ProjektProject
Identifikace částic v experimentech fysiky vysokych energií a ve vesmíru s pokročilými detekčními systémyParticle identification in high-energy physics experiments and space with advanced detection systems

AbstraktAbstract

The present manuscript describes a comprehensive characterization of a novel highly segmented 5 mm CZT sensor attached to Timepix3. First, the sensor's IV curve was measured and basic sensor characterization was done with laboratory gamma-radiation sources. The sensor resistivity was determined to be (0.155 +/- 0.02) GOhm <middle dot> cm. The sensor showed decent homogeneity, both for the per-pixel count rate and electron mobility-lifetime product mu e tau e. The latter was measured to be = 1.3 x 10(-3) cm2/V with a standard deviation sigma = 0.4 x 10(-3) cm(2)/V describing the dispersion of values for different pixels. The basic sensor characterization is complemented by measurements at grazing angle in a 120 GeV/c at the CERN's Super Proton Synchrotron. The penetrating nature of these particles together with the pixelation of the sensor allows for a determination of the charge collection efficiency (CCE), as well as charge carrier drift properties (drift times, lateral charge cloud expansion) as a function of the interaction depths in the sensor. While CCE drops by 30%-40% towards the cathode side of the sensor, from the drift time dependency on interaction depth, the electron mobility mu e was extracted to be (944.8 +/- 1.3) cm(2)/V/s and tau e = (1.38 +/- 0.31) mu s. The spectroscopic performance was assessed in photon fields and extracted from energy loss spectra measured at different angles in the pion beam. While at photon energies below 120 keV incomplete charge collection leads to an underestimation of the photon energy when irradiated from the front side, at higher energies the relative energy resolution was found to be -4.5%, while a relative energy resolution of -7.5% was found for the particle energy loss spectra. It is shown that the drift time information can be used to reconstruct particle interactions in the sensor in 3D, providing a spatial resolution of sigma xyz = 241 mu m within the sensor volume and a particle trajectory measurement precision Delta(xyz) = 100 mu m, at a distance of 1 m from the sensor. We demonstrate by measurement with a 22Na source, that the energy resolution combined with the 3D reconstruction allows for detection of gamma-ray source location and polarity using Compton scattering within the sensor (Compton camera and scatter polarimeter).

The present manuscript describes a comprehensive characterization of a novel highly segmented 5 mm CZT sensor attached to Timepix3. First, the sensor's IV curve was measured and basic sensor characterization was done with laboratory gamma-radiation sources. The sensor resistivity was determined to be (0.155 +/- 0.02) GOhm <middle dot> cm. The sensor showed decent homogeneity, both for the per-pixel count rate and electron mobility-lifetime product mu e tau e. The latter was measured to be = 1.3 x 10(-3) cm2/V with a standard deviation sigma = 0.4 x 10(-3) cm(2)/V describing the dispersion of values for different pixels. The basic sensor characterization is complemented by measurements at grazing angle in a 120 GeV/c at the CERN's Super Proton Synchrotron. The penetrating nature of these particles together with the pixelation of the sensor allows for a determination of the charge collection efficiency (CCE), as well as charge carrier drift properties (drift times, lateral charge cloud expansion) as a function of the interaction depths in the sensor. While CCE drops by 30%-40% towards the cathode side of the sensor, from the drift time dependency on interaction depth, the electron mobility mu e was extracted to be (944.8 +/- 1.3) cm(2)/V/s and tau e = (1.38 +/- 0.31) mu s. The spectroscopic performance was assessed in photon fields and extracted from energy loss spectra measured at different angles in the pion beam. While at photon energies below 120 keV incomplete charge collection leads to an underestimation of the photon energy when irradiated from the front side, at higher energies the relative energy resolution was found to be -4.5%, while a relative energy resolution of -7.5% was found for the particle energy loss spectra. It is shown that the drift time information can be used to reconstruct particle interactions in the sensor in 3D, providing a spatial resolution of sigma xyz = 241 mu m within the sensor volume and a particle trajectory measurement precision Delta(xyz) = 100 mu m, at a distance of 1 m from the sensor. We demonstrate by measurement with a 22Na source, that the energy resolution combined with the 3D reconstruction allows for detection of gamma-ray source location and polarity using Compton scattering within the sensor (Compton camera and scatter polarimeter).