Sandeep K. Chaudhuri, Ritwik Nag, Utpal N. Roy, Ralph B. James, Krishna C. Mandal
{"title":"用于室温伽马射线探测的 Cd0.9Zn0.1Te0.98Se0.02 四元半导体中电子-空穴对产生能的测定","authors":"Sandeep K. Chaudhuri, Ritwik Nag, Utpal N. Roy, Ralph B. James, Krishna C. Mandal","doi":"10.1049/ell2.70007","DOIUrl":null,"url":null,"abstract":"<p>We report the first-time measurement of the electron-hole pair (ehp) creation energy (<i>W<sub>ehp</sub></i>) in novel Cd<sub>0.9</sub>Zn<sub>0.1</sub>Te<sub>0.98</sub>Se<sub>0.02</sub> (CZTS) quaternary semiconductor. CZTS in single crystalline form is poised to be the future of large-volume room-temperature gamma-ray detectors due to its excellent compositional homogeneity with highly reduced defects, high-Z (atomic number) constituents, wide bandgap (1.6 eV), and superior charge transport properties. Despite a great deal of study of the material and device properties since its inception, the <i>W<sub>ehp</sub></i> in CZTS has not been measured experimentally. Accurate determination of <i>W<sub>ehp</sub></i> is essential for calibration of the spectrometer and other theoretical calculations. In this study we have used an absolute calibration approach, which is based on an iterative approach that yields the <i>W<sub>ehp</sub></i> as the best-fit parameter. Using a <sup>241</sup>Am alpha emitting radioisotope and a planar CZTS detector, the <i>W<sub>ehp</sub></i> in CZTS was calculated to be 4.47 eV. The obtained value has been validated by accurately predicting the peak energy for gamma rays emitted by a <sup>137</sup>Cs source and read by a CZTS detector with different dimensions. The dependences of the calculated <i>W<sub>ehp</sub></i> value on the detector dimensions, type of interaction, and effect of charge trapping are also discussed.</p>","PeriodicalId":11556,"journal":{"name":"Electronics Letters","volume":"60 17","pages":""},"PeriodicalIF":0.7000,"publicationDate":"2024-09-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1049/ell2.70007","citationCount":"0","resultStr":"{\"title\":\"Determination of electron-hole pair creation energy in Cd0.9Zn0.1Te0.98Se0.02 quaternary semiconductor for room-temperature gamma-ray detection\",\"authors\":\"Sandeep K. Chaudhuri, Ritwik Nag, Utpal N. Roy, Ralph B. James, Krishna C. Mandal\",\"doi\":\"10.1049/ell2.70007\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>We report the first-time measurement of the electron-hole pair (ehp) creation energy (<i>W<sub>ehp</sub></i>) in novel Cd<sub>0.9</sub>Zn<sub>0.1</sub>Te<sub>0.98</sub>Se<sub>0.02</sub> (CZTS) quaternary semiconductor. CZTS in single crystalline form is poised to be the future of large-volume room-temperature gamma-ray detectors due to its excellent compositional homogeneity with highly reduced defects, high-Z (atomic number) constituents, wide bandgap (1.6 eV), and superior charge transport properties. Despite a great deal of study of the material and device properties since its inception, the <i>W<sub>ehp</sub></i> in CZTS has not been measured experimentally. Accurate determination of <i>W<sub>ehp</sub></i> is essential for calibration of the spectrometer and other theoretical calculations. In this study we have used an absolute calibration approach, which is based on an iterative approach that yields the <i>W<sub>ehp</sub></i> as the best-fit parameter. Using a <sup>241</sup>Am alpha emitting radioisotope and a planar CZTS detector, the <i>W<sub>ehp</sub></i> in CZTS was calculated to be 4.47 eV. The obtained value has been validated by accurately predicting the peak energy for gamma rays emitted by a <sup>137</sup>Cs source and read by a CZTS detector with different dimensions. The dependences of the calculated <i>W<sub>ehp</sub></i> value on the detector dimensions, type of interaction, and effect of charge trapping are also discussed.</p>\",\"PeriodicalId\":11556,\"journal\":{\"name\":\"Electronics Letters\",\"volume\":\"60 17\",\"pages\":\"\"},\"PeriodicalIF\":0.7000,\"publicationDate\":\"2024-09-02\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://onlinelibrary.wiley.com/doi/epdf/10.1049/ell2.70007\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Electronics Letters\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1049/ell2.70007\",\"RegionNum\":4,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Electronics Letters","FirstCategoryId":"5","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1049/ell2.70007","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
Determination of electron-hole pair creation energy in Cd0.9Zn0.1Te0.98Se0.02 quaternary semiconductor for room-temperature gamma-ray detection
We report the first-time measurement of the electron-hole pair (ehp) creation energy (Wehp) in novel Cd0.9Zn0.1Te0.98Se0.02 (CZTS) quaternary semiconductor. CZTS in single crystalline form is poised to be the future of large-volume room-temperature gamma-ray detectors due to its excellent compositional homogeneity with highly reduced defects, high-Z (atomic number) constituents, wide bandgap (1.6 eV), and superior charge transport properties. Despite a great deal of study of the material and device properties since its inception, the Wehp in CZTS has not been measured experimentally. Accurate determination of Wehp is essential for calibration of the spectrometer and other theoretical calculations. In this study we have used an absolute calibration approach, which is based on an iterative approach that yields the Wehp as the best-fit parameter. Using a 241Am alpha emitting radioisotope and a planar CZTS detector, the Wehp in CZTS was calculated to be 4.47 eV. The obtained value has been validated by accurately predicting the peak energy for gamma rays emitted by a 137Cs source and read by a CZTS detector with different dimensions. The dependences of the calculated Wehp value on the detector dimensions, type of interaction, and effect of charge trapping are also discussed.
期刊介绍:
Electronics Letters is an internationally renowned peer-reviewed rapid-communication journal that publishes short original research papers every two weeks. Its broad and interdisciplinary scope covers the latest developments in all electronic engineering related fields including communication, biomedical, optical and device technologies. Electronics Letters also provides further insight into some of the latest developments through special features and interviews.
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