EPR identification of defects responsible for thermoluminescence in Cu-doped lithium tetraborate (Li2B4O7) crystals

被引:34
|
作者
Brant, A. T. [1 ]
Buchanan, D. A. [1 ]
McClory, J. W. [1 ]
Dowben, P. A. [2 ]
Adamiv, V. T. [3 ]
Burak, Ya V. [3 ]
Halliburton, L. E. [4 ]
机构
[1] USAF, Inst Technol, Dept Engn Phys, Wright Patterson AFB, OH 45433 USA
[2] Univ Nebraska, Dept Phys & Astron, Nebraska Ctr Mat & Nanosci, Lincoln, NE 68588 USA
[3] Inst Phys Opt, UA-79005 Lvov, Ukraine
[4] W Virginia Univ, Dept Phys, Morgantown, WV 26505 USA
关键词
Lithium tetraborate; Electron paramagnetic resonance; Copper doping; Crystal defects; Radiation dosimetry; Thermoluminescence; THERMALLY STIMULATED LUMINESCENCE; SINGLE-CRYSTALS; OPTICAL-ABSORPTION; GROWTH; AG; PHOTOLUMINESCENCE; PARAMETERS;
D O I
10.1016/j.jlumin.2013.02.023
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
Electron paramagnetic resonance (EPR) is used to identify the electron and hole traps responsible for thermoluminescence (TL) peaks occurring near 100 and 200 degrees C in copper-doped lithium tetraborate (Li2B4O7) crystals. As-grown crystals have Cu+ and Cu2+ ions substituting for lithium and have Cu+ ions at interstitial sites. All of the substitutional Cu2+ ions in the as-grown crystals have an adjacent lithium vacancy and give rise to a distinct EPR spectrum. Exposure to ionizing radiation at room temperature produces a second and different Cu2+ EPR spectrum when a hole is trapped by substitutional Cu+ ions that have no nearby defects. These two Cu2+ trapped-hole centers are referred to as Cu2+-V-Li and Cu-active(2+), respectively. Also during the irradiation, two trapped-electron centers in the form of interstitial Cu-0 atoms are produced when interstitial Cu+ ions trap electrons. They are observed with EPR and are labeled Cu-A(0) and Cu-B(0). When an irradiated crystal is warmed from 25 to 150 degrees C, the Cu-active(2+) centers have a partial decay step that correlates with the TL peak near 100 degrees C. The concentrations of Cu-A(0) and Cu-B(0) centers, however, increase as the crystal is heated through this range. As the crystal is further warmed between 150 and 250 degrees C, the EPR signals from the Cu-active(2+) hole centers and Cu-A(0) and Cu-B(0) electron centers decay simultaneously. This decay step correlates with the intense TL peak near 200 degrees C. Published by Elsevier B.V.
引用
收藏
页码:125 / 131
页数:7
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