About: Unique Deep Level in Spectroscopic CdZnTe: Compensation, Trapping, and Polarization     Goto   Sponge   NotDistinct   Permalink

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  • As yet, the role of the main native defects in the compensation, trapping, and polarization of x-ray and gamma-ray room-temperature detectors based on semi-insulated cadmium telluride (CdTe) and cadmium zinc telluride (CdZnTe) is indeterminate. To better quantify it, we assessed the ionization energy, i.e., the binding energy for the hole of the second (2-/1-) acceptor level of Cd vacancies in Cd1-xZnxTe(x approximate to 0.1). We characterized the defects in several ways, including measuring the photoconductivity at below-bandgap excitation, and photoconductivity quenching by comparing their positions in the bandgap with that of the native energy-levels in CdTe quantum dots (QDs) and other II-VI semiconductors. In this way, we determined unambiguously that a deep acceptor, Cd vacancy, behaves as a doubly charged acceptor, and the second ionization level is located at similar to Ev+(0.5 +/- 0.05) eV, i.e., relatively far from the midgap similar to 0.8 eV. This configuration may determine the lifetime of holes, but it does not stabilize precisely the compensation condition, and it is not responsible for electron trapping and polarization.
  • As yet, the role of the main native defects in the compensation, trapping, and polarization of x-ray and gamma-ray room-temperature detectors based on semi-insulated cadmium telluride (CdTe) and cadmium zinc telluride (CdZnTe) is indeterminate. To better quantify it, we assessed the ionization energy, i.e., the binding energy for the hole of the second (2-/1-) acceptor level of Cd vacancies in Cd1-xZnxTe(x approximate to 0.1). We characterized the defects in several ways, including measuring the photoconductivity at below-bandgap excitation, and photoconductivity quenching by comparing their positions in the bandgap with that of the native energy-levels in CdTe quantum dots (QDs) and other II-VI semiconductors. In this way, we determined unambiguously that a deep acceptor, Cd vacancy, behaves as a doubly charged acceptor, and the second ionization level is located at similar to Ev+(0.5 +/- 0.05) eV, i.e., relatively far from the midgap similar to 0.8 eV. This configuration may determine the lifetime of holes, but it does not stabilize precisely the compensation condition, and it is not responsible for electron trapping and polarization. (en)
Title
  • Unique Deep Level in Spectroscopic CdZnTe: Compensation, Trapping, and Polarization
  • Unique Deep Level in Spectroscopic CdZnTe: Compensation, Trapping, and Polarization (en)
skos:prefLabel
  • Unique Deep Level in Spectroscopic CdZnTe: Compensation, Trapping, and Polarization
  • Unique Deep Level in Spectroscopic CdZnTe: Compensation, Trapping, and Polarization (en)
skos:notation
  • RIV/00216208:11320/12:10125920!RIV13-GA0-11320___
http://linked.open...avai/riv/aktivita
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  • I, P(GAP102/10/0148)
http://linked.open...iv/cisloPeriodika
  • 4
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  • 175993
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  • RIV/00216208:11320/12:10125920
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  • photoconductivity; traps; detector; CdTe (en)
http://linked.open.../riv/klicoveSlovo
http://linked.open...odStatuVydavatele
  • US - Spojené státy americké
http://linked.open...ontrolniKodProRIV
  • [EB6D26570513]
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  • IEEE Transactions on Nuclear Science
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  • 59
http://linked.open...iv/tvurceVysledku
  • Franc, Jan
  • Babentsov, V.
  • James, R. B.
  • Dieguez, E.
  • Sochinskyi, M. V.
http://linked.open...ain/vavai/riv/wos
  • 000307893900009
issn
  • 0018-9499
number of pages
http://bibframe.org/vocab/doi
  • 10.1109/TNS.2012.2191159
http://localhost/t...ganizacniJednotka
  • 11320
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