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HgCdTe—CdTe异质结构的变频导纳特性
引用本文:赵军,郭世平.HgCdTe—CdTe异质结构的变频导纳特性[J].红外与毫米波学报,1996,15(2):87-92.
作者姓名:赵军  郭世平
作者单位:中国科学院上海技术物理研究所
摘    要:采用宽频带导纳测试系统研究了Hg0.66Cd0.34Te-CdTe异质结构和Al-半绝缘CdTe-Hg0.66Cd0.34Te结构样品的变频导纳特性,分析了不同结构样吕的测试结果,表明:异质结HgCdTe表面空穴积累,CdTe表面空穴耗尽,界面处的势垒使载流子局限于HgCdTe体内,样品的光伏响应光谱在2970cm^-1和3650cm^-1处各有一个响应峰,前者对应于界面HgCdTe的本征光伏效庆

关 键 词:HgCdTe  CdTe  异质结  导纳测量

VARIABLE FREQUENCY ADMITTANCE SPECTRA OF HgCdTe CdTe HETEROSTRUCTURE
Zhao Jun,Guo Shiping,Fang Jiaxiong.VARIABLE FREQUENCY ADMITTANCE SPECTRA OF HgCdTe CdTe HETEROSTRUCTURE[J].Journal of Infrared and Millimeter Waves,1996,15(2):87-92.
Authors:Zhao Jun  Guo Shiping  Fang Jiaxiong
Abstract:Admittance voltage characteristics of Hg 0.66 Cd 0.34 Te CdTe heterostructures were studied by using a wide band admittance measurement system.HgCdTe heterostructures were grown by MBE technology.An energy band structure was established according to the analysis of C V and G V results.It was shown that,holes are accumulated at the HgCdTe surface while depleted at the CdTe surface and the barriers formed at the interface make the carriers confined in HgCdTe.The photovoltaic response spectrum shows two peaks,which are located at 2970cm -1 and 3650cm -1 respectively.The former peak is due to the intrinsic photovoltaic effect of HgCdTe,and the latter peak is due to the effect that holes in the accumulation layer are excited by photons and then overpass the hole barrier at the interface, i.e. ,the hole barrier height is about 0.41eV.
Keywords:HgCdTe  CdTe  heterostructure  admittance measurement    
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