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Cd_(1-x)Zn_x合金组元分压控制下高阻CdZnTe晶体的熔体生长 被引量:1

CdZnTe Crystal of High Resistivity Melting Growth under Cd_(1-x)Zn_(x)Alloy Partial Pressures Control
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摘要 本文运用热力学关系估算了CdZnTe 熔体平衡分压。尝试以Cd1 - xZnx 合金源替代Cd 源控制Cd 分压和Zn 分压进行了Cd0 .8Zn 0 .2Te 晶体熔体生长,探讨了熔体分压与晶体电阻率的关系。获得的Cd0 .8Zn 0 .2Te 晶体的电阻率接近1010Ω·cm ,高于同类方法文献报道1 ~2 个数量级。晶体的结构完整性较好,平均腐蚀坑密度(EPD) 为2 ×105cm - 2 ,纵向组成分布偏离度在4 % 左右,红外透过率大于60 % ,晶体中第二相和沉淀物明显减少,优于仅采用Cd 分压控制的Cd0 .8Zn0 .2Te 晶体。 Equilibrium partial pressures over CdZnTe melt have been estimated by thermodynamic relationship and Cd 0.8 Zn 0.2 Te crystal growth from the melt has been carried out under controlled Cd/Zn partial pressures,provided by Cd 1- x Zn x alloy source instead of Cd source.The relationship between partial pressures of the melt and the resistivity of crystal is discussed.The resistivity of Cd 0.8 Zn 0.2 Te crystal obtained reached up to about 10 10 Ω·cm,which is 1~2 of order higher than that reported in the literature using the same method.The structure perfection of as grown crystal is rather good.The mean EPD is about 2×10 5cm -2 .The variation in composition along the length of ingots is within 4%.The IR transmittance is larger than 60%.The second phases and precipitates in crystals are obviously decreased.The Cd 0.8 Zn 0.2 Te crystals are better than that obtained only under controlled Cd partial pressure.
出处 《人工晶体学报》 EI CAS CSCD 北大核心 1999年第4期328-334,共7页 Journal of Synthetic Crystals
基金 国家自然科学基金
关键词 CDZNTE晶体 布里奇曼法 Γ探测器 晶体生长 CdZnTe crystal,Bridgman method,equilibrium partial pressures over CdZnTe melt,γray detectors
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参考文献3

  • 1桑文斌 周书铨 等.光吸收法测定CdTe熔体平衡蒸汽分压[J].红外研究,1987,6:415-415.
  • 2Sang Wenbin,J Cryst Growth,1988年,86卷,127页
  • 3桑文斌,红外研究,1987年,6期,415页

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