Investigation of the composite structure of peak 5 in the thermoluminescent glow curve of LiF:Mg,Ti (TLD-100) using optical bleaching

被引:40
作者
Weizman, Y [1 ]
Horowitz, YS
Oster, L
机构
[1] Ben Gurion Univ Negev, Dept Phys, IL-84105 Beer Sheva, Israel
[2] Technol Coll Beersheva, Sch Engn, IL-84100 Beer Sheva, Israel
关键词
D O I
10.1088/0022-3727/32/16/322
中图分类号
O59 [应用物理学];
学科分类号
摘要
The composite structure of glow peak 5 in LiF:Mg,Ti (TLD-100), has been investigated using optical bleaching by 310 nm (4 eV) light. The decay of composite peak 5 and the growth of peak 4 are described by two exponential components of the same mean lives for both peaks. Using computerized glow curve deconvolution and contrary to previous investigations, it is determined that peak 4 does not decrease in intensity at long bleaching times and is therefore not associated with the 4 eV absorption band. The fast and slow components of the exponential decay are associated with the bleaching of peaks 5a and 5, respectively. Optical bleaching as a function of the temperature of post-irradiation annealing reveals that the conversion efficiency of peak 5a to peak 4 is very high, at a constant value of approximately 30%, whereas the conversion efficiency of peak 5 is no greater than a few per cent. The behaviour of the conversion efficiency as a function of the temperature of the post-irradiation anneal is explained in the framework of the spatially correlated trapping centre/luminescent (TC/LC) centre model. In this model, the TL of peak 5a results from the geminate recombination of a locally trapped electron-hole pair: peak 5 results from recombination via electron diffusion in the conduction band following thermal release of a singly-trapped electron in the TC/LC structure. Peak 4 arises from a singly-trapped hole in the TC/LC structure. The high conversion efficiency of peak 5a to peak 4 arises from direct optical ionization of the electron in the electron-hole pair, leaving behind a singly-trapped hole (glow peak 4), a direct mechanism not subject to competitive processes. Optical ionization of the 'singly-trapped' electron (peak 5), however, can lead to peak 4 only via a multi-stage mechanism involving charge carrier transport in the conduction band, a mechanism subject to competitive processes, which leads to an order-of-magnitude decrease in the observed efficiency.
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页码:2118 / 2127
页数:10
相关论文
共 25 条
[1]  
[Anonymous], COMMUNICATION
[2]   Temperature dependent absorption spectrometry on LiF:Mg,Ti [J].
Bos, AJJ ;
De Haas, JTM .
RADIATION MEASUREMENTS, 1998, 29 (3-4) :349-353
[3]  
BOS AJJ, 1993, 13193005 IRI CIEMAT
[4]   COMPETITION BETWEEN EXCITATION AND BLEACHING OF THERMOLUMINESCENCE [J].
CHEN, R ;
HORNYAK, WF ;
MATHUR, VK .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 1990, 23 (06) :724-728
[5]   THERMOLUMINESCENCE AND COLOR CENTERS IN LIF [J].
CHRISTY, RW ;
JOHNSON, NM ;
WILBARG, RR .
JOURNAL OF APPLIED PHYSICS, 1967, 38 (05) :2099-&
[6]   NEW EVIDENCE AGAINST THE PRESENCE OF PEAK-IV IN THE TL AND PTTL GLOW CURVES OF HEAVILY ANNEALED TLD-100 [J].
DELGADO, A ;
ROS, JMG ;
PORTILLO, JC .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 1988, 21 (06) :1015-1018
[7]   THERMOLUMINESCENCE OF LIF TLD-100 - GLOW-CURVE KINETICS [J].
FAIRCHILD, RG ;
MATTERN, PL ;
LENGWEILER, K ;
LEVY, PW .
JOURNAL OF APPLIED PHYSICS, 1978, 49 (08) :4523-4533
[8]  
Horowitz Y., 1995, Radiat. Prot. Dosim, V60, P3
[9]   The unified interaction model applied to the gamma-induced supralinearity and sensitisation of peaks 4 and 5 in LiF:Mg,Ti (TLD-100) [J].
Horowitz, YS ;
Mahajna, S ;
Oster, L ;
Weizman, Y ;
Satinger, D ;
Yossian, D .
RADIATION PROTECTION DOSIMETRY, 1998, 78 (03) :169-193
[10]   Ionisation density effects in the thermoluminescence of TLD-100:: Computerised Tm-Tstop glow curve analysis [J].
Horowitz, YS ;
Satinger, D ;
Yossian, D ;
Brandan, ME ;
Buenfil, AE ;
Gamboa-deBuen, I ;
Rodriguez-Villafuerte, M ;
Ruiz, CG .
RADIATION PROTECTION DOSIMETRY, 1999, 84 (1-4) :239-242