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Restored thermoluminescence in oxide crystals

In this paper, we present the results of a thermoluminescence study on several oxide crystals, including Y 3Al 5O 12 (YAG), Y 3Al 5O 12:Nd (YAG:Nd), Lu 2SiO 5:Ce (LSO:Ce), Y 2SiO 5:Ce (YSO:Ce), Gd 2SiO 5:Ce (GSO:Ce), PbWO (PWO), and PbWO:La (PWO:La). A phenomenon involving restoration of thermolumin...

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Published in:Journal of luminescence 2010-11, Vol.130 (11), p.2004-2012
Main Authors: Rakov, A.F., Salikhbaev, U.S., Islamov, A.K., Bartram, R.H., Melcher, C.L.
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cited_by cdi_FETCH-LOGICAL-c368t-d9d2dd1c9fa71a4667db2796fe1a0eb9363fb501f70f11942989870e0363a5a23
cites cdi_FETCH-LOGICAL-c368t-d9d2dd1c9fa71a4667db2796fe1a0eb9363fb501f70f11942989870e0363a5a23
container_end_page 2012
container_issue 11
container_start_page 2004
container_title Journal of luminescence
container_volume 130
creator Rakov, A.F.
Salikhbaev, U.S.
Islamov, A.K.
Bartram, R.H.
Melcher, C.L.
description In this paper, we present the results of a thermoluminescence study on several oxide crystals, including Y 3Al 5O 12 (YAG), Y 3Al 5O 12:Nd (YAG:Nd), Lu 2SiO 5:Ce (LSO:Ce), Y 2SiO 5:Ce (YSO:Ce), Gd 2SiO 5:Ce (GSO:Ce), PbWO (PWO), and PbWO:La (PWO:La). A phenomenon involving restoration of thermoluminescence (TL) glow peaks is found to occur in some of the crystals investigated; crystals γ-irradiated at room temperature and subsequently stored for some time in the dark at 77 K exhibit TL glow peaks in the range below room temperature. This phenomenon is caused not by a thermally or optically stimulated process, but rather as a by-product of a tunneling process. The intensity of the restored TL glow peaks measured in LSO:Ce crystals is found to be proportional both to the radiation dose and to the storage-time at low temperature. A phenomenological theoretical model is proposed, in which tunneling recombination occurs between deep electron and hole traps accompanied by the simultaneous ejection of an electron to the conduction band; some of these conduction electrons then repopulate shallow traps. An oxygen vacancy with two trapped electrons is assumed to be the deep electron trap in this model. The role of oxygen vacancies is confirmed by heating in air at 1000 °C. This model is applied specifically to LSO:Ce, and several possible candidates are suggested for shallow traps in that material.
doi_str_mv 10.1016/j.jlumin.2010.05.018
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A phenomenon involving restoration of thermoluminescence (TL) glow peaks is found to occur in some of the crystals investigated; crystals γ-irradiated at room temperature and subsequently stored for some time in the dark at 77 K exhibit TL glow peaks in the range below room temperature. This phenomenon is caused not by a thermally or optically stimulated process, but rather as a by-product of a tunneling process. The intensity of the restored TL glow peaks measured in LSO:Ce crystals is found to be proportional both to the radiation dose and to the storage-time at low temperature. A phenomenological theoretical model is proposed, in which tunneling recombination occurs between deep electron and hole traps accompanied by the simultaneous ejection of an electron to the conduction band; some of these conduction electrons then repopulate shallow traps. An oxygen vacancy with two trapped electrons is assumed to be the deep electron trap in this model. 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A phenomenon involving restoration of thermoluminescence (TL) glow peaks is found to occur in some of the crystals investigated; crystals γ-irradiated at room temperature and subsequently stored for some time in the dark at 77 K exhibit TL glow peaks in the range below room temperature. This phenomenon is caused not by a thermally or optically stimulated process, but rather as a by-product of a tunneling process. The intensity of the restored TL glow peaks measured in LSO:Ce crystals is found to be proportional both to the radiation dose and to the storage-time at low temperature. A phenomenological theoretical model is proposed, in which tunneling recombination occurs between deep electron and hole traps accompanied by the simultaneous ejection of an electron to the conduction band; some of these conduction electrons then repopulate shallow traps. An oxygen vacancy with two trapped electrons is assumed to be the deep electron trap in this model. 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subjects Byproducts
Condensed matter: electronic structure, electrical, magnetic, and optical properties
Crystals
Exact sciences and technology
Heating
Lattice vacancies
Luminescence
Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation
Other luminescence and radiative recombination
Oxide crystals
Oxides
Physics
Restored thermoluminescence
Shallow and deep traps
Thermoluminescence
Tunneling
title Restored thermoluminescence in oxide crystals
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