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LiMgPO4:Tm,Tb的热释光和光释光陷阱参数

郭竞渊 唐强 唐桦明 张纯祥 罗达玲 刘小伟

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LiMgPO4:Tm,Tb的热释光和光释光陷阱参数

郭竞渊, 唐强, 唐桦明, 张纯祥, 罗达玲, 刘小伟

Thermoluminescence and optical stimulated luminescence trap parameters of LiMgPO4: Tm, Tb

Guo Jing-Yuan, Tang Qiang, Tang Hua-Ming, Zhang Chun-Xiang, Luo Da-Ling, Liu Xiao-Wei
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  • 采用高温固相法合成了LiMgPO4:Tm,Tb粉末样品,测定了热释光陷阱参数激发能E 和频率因子s.用脉冲退火和多次退火方法研究了其光释光陷阱参数E和s,并与用多速法得到的热释光的结果进行了比较.对不同射线剂量照射的样品发光曲线的研究表明,300 ℃高温峰属于一级动力学发光峰.通过对热释光和光释光陷阱的相关性研究表明,经200 ℃预热的热释光信号(对应于300 ℃高温峰)和光释光信号很有可能来自于同一深度的陷阱.
    In recent years, the preparation and luminescent properties of LiMgPO4 as a matrix have received much attention, but most of the studies are limited to the trap parameters of thermoluminescence (TL), which do not involve the trap parameters of optical stimulated luminescence (OSL). In this paper, LiMgPO4:Tm, Tb powder samples are synthesized by solid-state reaction at high temperature. All the experiments reported here are measured by Riso TL/OSL-15-B/C reader after being irradiated by beta-rays. The TL glow curves obtained show that the high temperature peak at 300℃ belongs to the first-order kinetic peak because the peak temperature does not change as irradiation dose increases. Based on the first-order kinetics, the TL trap depth E = 1.72 eV and the frequency factor s= 3.97 1014 are determined by the methods of various heating rates.However, LiMgPO4:Tm, Tb is also an OSL material, the analysis of its OSL trap kinetic parameters would help to understand the OSL mechanism and to know the relationship between TL and OSL traps. The pulse annealing method is suitable for OSL trap parameter analysis. For low sensitivity samples, the fluctuation of the pulse annealing method is relatively large. And this method only records the OSL signal of fast decay component, which is suitable for measuring the samples with high sensitivity and fast fading OSL signals. In order to study the OSL signal of slow decay component, the multiple annealing method is proposed based on the pulse annealing method. The multiple annealing procedure is as follows. Firstly, the sample is annealed from room temperature to 500℃ which lasts 30 s. The heating rate is 5℃/s. Secondly, the sample is irradiated with 90Sr beta radiation doses of 1 Gy. Thirdly, the sample is preheated to 150℃ with a heating rate of 0.2 ℃/s. And then OSL measurement lasts 500 s after cooling to room temperature. The above steps are repeated in preheating temperature steps of 10℃. Four repetitive measurements are made for each preheating rate. The preheating rates are 0.2, 0.5, 1, and 2℃/s.Finally, the OSL trap parameters E = 1.69 eV and s = 1.05 1014 are determined by the multiple annealing method. The correlation between TL and OSL trap parameters shows that the TL and OSL signals are likely to come from the same traps. Besides, the trap depth of the main peak of the phosphor shows that the sample has better thermal stability than those of the other phosphors of LiMgPO4 as the matrix.
      通信作者: 唐强, ststq@mail.sysu.edu.cn
    • 基金项目: 国家自然科学基金(批准号:11375278)、广东省自然科学基金(批准号:2016A030313276)和广州市科技计划项目(批准号:20160701168)资助的课题;
      Corresponding author: Tang Qiang, ststq@mail.sysu.edu.cn
    • Funds: Project supported by the National Natural Science Foundation of China (Grant No. 11375278), the Natural Science Foundation of Guangdong Province, China (Grant No. 2016A030313276) and Guangzhou Science and Technology Project, China (Grant No. 20160701168).
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    Garlick G F J, Gibson A F 1948 Proc. Phys. Soc. 60 574

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    [9]

    Li S H, Chen G 2001 J. Phys. D 34 493

    [10]

    Pagonis V, Wintle A G, Chen R 2007 Radiat. Meas. 42 1587

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    Mahesh K, Weng P S, Furetta C 1989 Thermoluminescence in Solids and its Applications (England: Nuclear Technology Publishing)

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    Zhang C X, Tang Q, Luo D Y 2002 Acta Phys. Sin. 51 2881 (in Chinese) [张纯祥, 唐强, 罗达玲 2002 物理学报 51 2881]

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    Hoogenstraaten W 1958 Philips Res. Rep. 13 515

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    Li S H, Tso M Y W, Wong N W 1997 Radiat. Meas. 27 43

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    Bajaj N S, Palan C B, Koparkar K A, Kulkarni M S, Omanwar S K 2016 J. Lumin. 175 9

  • [1]

    Dhabekar B, Menon S N, Raja E A, Singh A K, Chougaokar M P, Mayya Y S 2011 Nucl. Instrum. Methods Phys. Res. Sect. B 269 1844

    [2]

    Menon S N, Dhabekar B, Raja E A, Chouhaonkar M P 2012 Radiat. Meas. 47 236

    [3]

    Gai M Q, Chen Z Y, Fan Y W, Wang J H 2013 J. Rare Earth 31 551

    [4]

    Gai M Q, Chen Z Y, Fan Y W, Yan S Y, Xie Y X, Wang J H, Zhang Y G 2015 Radiat. Meas. 78 48

    [5]

    Guo J Y, Tang Q, Zhang C X, Luo D L, Liu X W J. Rare Earth (in Press)

    [6]

    Randall J T, Wilkins M H F 1945 Proc. Phys. Soc. 184 366

    [7]

    Garlick G F J, Gibson A F 1948 Proc. Phys. Soc. 60 574

    [8]

    Chen R, Kirsh Y 1981 Analysisi of Thermally Stimulated Processes (Oxford: Pergamon Press)

    [9]

    Li S H, Chen G 2001 J. Phys. D 34 493

    [10]

    Pagonis V, Wintle A G, Chen R 2007 Radiat. Meas. 42 1587

    [11]

    Bulur E, BØtter-Jensen L, Murray A S 2000 Radiat. Meas. 32 407

    [12]

    Mahesh K, Weng P S, Furetta C 1989 Thermoluminescence in Solids and its Applications (England: Nuclear Technology Publishing)

    [13]

    Zhang C X, Tang Q, Luo D Y 2002 Acta Phys. Sin. 51 2881 (in Chinese) [张纯祥, 唐强, 罗达玲 2002 物理学报 51 2881]

    [14]

    Hoogenstraaten W 1958 Philips Res. Rep. 13 515

    [15]

    Li S H, Tso M Y W, Wong N W 1997 Radiat. Meas. 27 43

    [16]

    Bajaj N S, Palan C B, Koparkar K A, Kulkarni M S, Omanwar S K 2016 J. Lumin. 175 9

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出版历程
  • 收稿日期:  2017-01-13
  • 修回日期:  2017-03-05
  • 刊出日期:  2017-05-05

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