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利用GDMS分别测试了用Bridgman方法生长的十个全尺寸钨酸铅晶体顶、底两端的杂质含量,发现在PWO晶体中,K、Na、Mo、As、Y等杂质元素富集于晶体的顶部,具有分凝系数小于1 的特征.Ca和Ba杂质则富集于晶体的底部,具有分凝系数大于1 的特征,Al、Si、Cu等杂质的分布缺乏明显的规律性.这些杂质主要来源于生长晶体时所使用的WO3原料.根据掺杂实验,认为K、Na、Mo、As等是影响PWO闪烁性能的有害杂质,Ca和Ba是无害杂质,Y是有益杂质,Al、Si、Cu等杂质的行为尚不明确.

参考文献

[1] 陈福泉.晶体生长对原料纯度的要求[J].人工晶体学报,1990(01):84.
[2] Lecoq P.;Auffray E.;Schneegans M.;Korzhik MV.;Missevitch OV.;Pavlenko VB.;Fedorov AA.;Annenkov AN.;Kostylev VL.;Ligun VD.;Dafinei I. .LEAD TUNGSTATE (PBWO4) SCINTILLATORS FOR LHC EM CALORIMETRY[J].Nuclear Instruments and Methods in Physics Research, Section A. Accelerators, Spectrometers, Detectors and Associated Equipment,1995(2/3):291-298.
[3] Annenkov AN.;Galez P.;Kachanov VA.;Korzhik MV.;Ligun VD. Moreau JM.;Nefedov VN.;Pavlenko VB.;Peigneux JP.;Timoshchenko TM. Zadneprovskii BA.;Fedorov AA. .THE INFLUENCE OF ADDITIONAL DOPING ON THE SPECTROSCOPIC AND SCINTILLATION PARAMETERS OF PBWO4 CRYSTALS[J].Physica Status Solidi, A. Applied Research,1996(2):493-504.
[4] 王绍华,沈定中,任国浩,蔡晓林,殷之文.下降法生长PWO晶体中光散射中心的观察与分析[J].人工晶体学报,1999(03):263-270.
[5] Kobayashi M et al.Significant Improvement of PbWO4 Scintillating Crystals by Doping with Trivalent Ions[J].Nuclear Instruments and Methods in Physics Research,1999,A399:412.
[6] Groenink J A;Blasse G .Some New Observation on the Luminescence of PbMO4 and PbWO4[J].Journal of Solid State Chemistry,1980,32:9.
[7] Nikl M. .Wide band gap scintillation materials: Progress in the technology and material understanding [Review][J].Physica Status Solidi, A. Applied Research,2000(2):595-620.
[8] Kobayashi M.;Ishii M.;Yazawa T.;Hara K.;Tanaka M.;Nikl M. Nitsch K.;Usuki Y. .IMPROVEMENT IN TRANSMITTANCE AND DECAY TIME OF PBWO4 SCINTILLATING CRYSTALS BY LA-DOPING[J].Nuclear Instruments and Methods in Physics Research, Section A. Accelerators, Spectrometers, Detectors and Associated Equipment,1997(2/3):261-268.
[9] 张明荣 .钨酸铅闪烁晶体的结构与光学特性的研究[D].中国科学院上海硅酸盐研究所,1998.
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