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作 者:张继军[1] 王领航[1] 王涛[1] 曾冬梅[1] 介万奇[1]
机构地区:[1]西北工业大学材料科学与工程学院,陕西西安710072
出 处:《功能材料》2007年第A03期1030-1033,共4页Journal of Functional Materials
基 金:国家自然科学基金重点资助项目(50336040).
摘 要:采用垂直Bridgman法生长了In掺杂Cd0.3Mn0.2Te晶体(CdMnTe:In)和本征的Cd0.8Mn0.2Te晶体(CdMnTe)。X射线粉末衍射、X射线双晶摇摆曲线和位错密度测试表明,所生长晶体均为立方闪锌矿结构,半峰宽为40~80arc Sec,位错密度为100~100cm^-2,结晶质量良好.In掺杂不影响晶体的结构和结晶质量。电流.电压(I-V)测试表明,CdMnTe:In晶体的电阻率为1~3×10^9Ω·cm,与CdMnTe晶体相比上升了3个数量级.近红外光透过光谱(IR transmission)研究发现In掺杂后CdMnTe晶体红外透过率降低,在波数范围4000~1000cm^-1,CdMnTe晶体红外透过率为51.2%~56.4%,而CdMnTe:In的红外透光率为15.4%~6%。Adopting vertical Bridgman method, an Indium (In) doped Cd0.8Mn0.2Te (CdMnTe: In) ingot and an intrinsic Cd0.8Mn0.2Te (CdMnTe) were grown. The crystalline structure and quality of the two ingots were verified by X-ray diffraction, double-crystal rocking curve measurement and etch pits density (EPD). The results showed a pure cubic zinc blende structure with the FWHM of 40~80 arc sec and EPD of I04~ 10s cm-2, which mean the as-grown ingots are with high crystalline perfection and the In dopant has no effect on the crystal structure. Current-voltage measurement shows that CdMnTe:In has the resistivity 1~3×10^9Ω·cm, which is three orders higher than that of undoped CdMnTe. IR transmission measurement exhibits that in the wavenumber range of 4000~ 1000 cm^-1 the IR transmittance of CdMnTe:In and CdMnTe is in between 15.4%~21.6% and 51.2%~56.4% respectively, indicating that In-doping results in a remarkable reduction of IR transmittance of CdMnTe crystal.
关 键 词:CDMNTE In掺杂 X射线衍射 电阻率 红外透过率
分 类 号:TN304.2[电子电信—物理电子学]
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