CLLB晶体生长与闪烁特性研究

Kun Wu, Leilei Zhang, Haijun Li, Guangwei Huang, Jiaming Li, Libin Wang, Siyuan Zhang, Zhiyuan Li, Qinhua Wei, Chunzhi Zhou, Zungang Wang, Huilan Liu, Hongying Zhu, Yushou Song
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摘要

Cs2LiLaBr6:Ce (CLLB)闪烁探测器具有优异的能量分辨率和对伽马射线的高光输出,具有优异的中子/伽马射线鉴别性能。它的应用主要局限于大尺寸、高质量的晶体生长。本文对高性能CLLB进行了生长、封装和测试。采用垂直Bridgman法生长Cs2LiLaBr6:1%Ce晶体。通过调节温度,将生长炉的最大温度梯度调整到结晶析出的位置。为了避免熔点不均匀,采用了原料的非化学计量,增加了100% LiBr的过量。该晶体直径1英寸,长5厘米,密度4.32 g/mL。最后,对晶体进行封装测试,晶体能量分辨率为4.0%,相对光输出为1.14 ~ 0.662 MeV,绝对光输出为47665光子/MeV ~ 0.511 MeV;电荷比较法使中子/伽马射线鉴别的优值(FOM)为1.27。采用光通量模拟方法分别测量了两种信号的闪烁衰减时间,其中快速部分约为0.19 μs,慢速部分约为1.08 μs。结果表明,中子信号在伽马射线信号中具有较高的快分量比例。
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Study on the Growth and Scintillation Properties of CLLB Crystals
Cs2LiLaBr6:Ce (CLLB) scintillation detector has excellent energy resolution and high light output to gamma-rays, with excellent neutron/gamma-rays discrimination performance. Its applications are mainly limited to crystal growth with large size and high quality. In this paper, high performance CLLB was grown, encapsulated and tested. The vertical Bridgman method was employed to grow Cs2LiLaBr6:1%Ce crystals. By regulating the temperature, the maximum temperature gradient of the growth furnace was adjusted to the position of crystal precipitation. To avoid the non-uniform melting component area, the non-stoichiometric of raw materials increasing the excess of 100% LiBr were used. The crystals was developed successfully with 1 inch diameter, 5 cm length, and 4.32 g/mL density. Finally, the crystal was encapsulated and tested, with an energy resolution of 4.0% and relative (NaI) optical output of 1.14 to 0.662 MeV gamma-rays, and an absolute optical output of 47665 Photons/MeV to 0.511 MeV gamma-rays; The figure of merit (FOM) of the neutron/gamma-rays discrimination is 1.27 enabled by charge comparison method. The scintillation decay time of the two kinds of signals is measured respectively by the optical flux simulation method, with a fast component of about 0.19 μs and a slow component of 1.08 μs. Results show that the neutron signals has a higher fast component proportion to gamma-rays signals.
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