1992
DOI: 10.1109/23.211437
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Measurement of X-ray spectrum using a small size CdTe multichannel detector

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Cited by 10 publications
(5 citation statements)
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“…A CdTe Schottky diode detector of 1 mm thickness was employed ͑Amptek XR-100T-CdTe͒. The size of the CdTe crystal was 3ϫ3ϫ1 mm 3 , and the density was 5.85 g/cm 3 . A CdZnTe detector of 2 mm thickness ͑Amptek XR-100T-CZT͒ was also used for comparison.…”
Section: A Detectors Used In This Studymentioning
confidence: 99%
See 1 more Smart Citation
“…A CdTe Schottky diode detector of 1 mm thickness was employed ͑Amptek XR-100T-CdTe͒. The size of the CdTe crystal was 3ϫ3ϫ1 mm 3 , and the density was 5.85 g/cm 3 . A CdZnTe detector of 2 mm thickness ͑Amptek XR-100T-CZT͒ was also used for comparison.…”
Section: A Detectors Used In This Studymentioning
confidence: 99%
“…Tsutui et al investigated the cause of spectral distortion in a 0.3 mm thick CdTe-array detector. 3 The dominant factors of the distortion were the energy dependency of photoelectric absorption and the escape of Cd-and Te-K fluorescent x rays. Spectral distortion due to the escape of Compton scattered x rays and secondary electrons was negligible.…”
Section: Introductionmentioning
confidence: 99%
“…The shape of the output bremsstrahlung spectrum extends up to the peak voltage (kVp) between the cathode and the anode of the generating X-ray tube. Most of the flux from traditional X-ray sources covers an extremely broad range, well over half the total energy range, and a maximum around one-third the peak value. , For example, for a 250 kVp source the X-ray output ranges between 40 and 250 keV photon energies, with a broad maximum around ∼80 keV. Since the Au K-edge E I (K) = 80.729 keV, a 250 kVp source is capable of ionizing all inner n -shells and subshells of the gold atom with L,M,N,O,P edges at approximately 12−14, 3.4−2.2, 0.11−0.9, 0.01−0.11, and 0.0.009 keV, respectively.…”
Section: Introductionmentioning
confidence: 99%
“…Tsutsui et al measured diagnostic x-ray spectra with a CdTe crystal of 0.3 mm thickness, and analyzed the causes of spectral distortion. 2 They concluded that the major causes of the distortion were the energy dependency of the photoelectric absorption process and the escape of Cd-and Te-K x rays. Additionally, they mentioned that the escape of secondary electrons also caused the distortion in the high-energy region, because the crystal was thin compared to the range of electrons.…”
Section: Introductionmentioning
confidence: 99%