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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.
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页码:125 / 131
页数:7
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