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应对第三代红外焦平面技术挑战的HgCdTe分子束外延
引用本文:何力,陈路,吴俊,巫艳,王元樟,于梅芳,杨建荣,丁瑞军,胡晓宁,李言谨,张勤耀. 应对第三代红外焦平面技术挑战的HgCdTe分子束外延[J]. 半导体学报, 2006, 27(3): 381-387
作者姓名:何力  陈路  吴俊  巫艳  王元樟  于梅芳  杨建荣  丁瑞军  胡晓宁  李言谨  张勤耀
作者单位:中国科学院上海技术物理研究所,半导体材料器件研究中心,上海,200083;中国科学院上海技术物理研究所,半导体材料器件研究中心,上海,200083;中国科学院上海技术物理研究所,半导体材料器件研究中心,上海,200083;中国科学院上海技术物理研究所,半导体材料器件研究中心,上海,200083;中国科学院上海技术物理研究所,半导体材料器件研究中心,上海,200083;中国科学院上海技术物理研究所,半导体材料器件研究中心,上海,200083;中国科学院上海技术物理研究所,半导体材料器件研究中心,上海,200083;中国科学院上海技术物理研究所,半导体材料器件研究中心,上海,200083;中国科学院上海技术物理研究所,半导体材料器件研究中心,上海,200083;中国科学院上海技术物理研究所,半导体材料器件研究中心,上海,200083;中国科学院上海技术物理研究所,半导体材料器件研究中心,上海,200083
摘    要:叙述了围绕第三代红外焦平面的需求所进行的HgCdTe分子束外延的一些研究结果.75mm HgCdTe薄膜材料的组分均匀性良好,80K下截止波长偏差为0.1μm.对所观察到的HgCdTe表面缺陷成核机制进行了分析讨论,获得的75mm HgCdTe材料平均表面缺陷密度低于300cm-2.研究发现As的表面黏附系数很低,对生长温度十分敏感,在170℃下约为1×10-4.计算表明,As在HgCdTe中的激活能为19.5meV,且随(Na∑Nd)1/3的增大呈线性下降关系,反比系数为3.1×10-5meV·cm.实验发现Hg饱和蒸汽压下,对应不同的温度240,380,440℃,As在HgCdTe中的扩散系数分别为(1.0±0.9)×10-16,(8±3)×10-15,(1.5±0.9)×10-13cm2/s.采用分子束外延生长的HgCdTe材料已用于红外焦平面探测器件的研制,文中报道了一些初步结果.

关 键 词:分子束外延  碲镉汞  红外焦平面
收稿时间:2015-08-20

MBE HgCdTe:A Challenge to the Realization of Third Generation Infrared FPAs
He Li, Chen Lu, Wu Jun, Wu Yan, Wang Yuanzhang, Yu Meifang, Yang Jianrong, Ding Ruijun, Hu Xiaoning, Li Yanjin, Zhang Qinyao. MBE HgCdTe:A Challenge to the Realization of Third Generation Infrared FPAs[J]. Journal of Semiconductors, 2006, In Press. He L, Chen L, Wu J, Wu Y, Wang Y Z, Yu M F, Yang J R, Ding R J, Hu X N, Li Y J, Zhang Q Y. MBE HgCdTe:A Challenge to the Realization of Third Generation Infrared FPAs[J]. Chin. J. Semicond., 2006, 27(3): 381.Export: BibTex EndNote
Authors:He Li  Chen Lu  Wu Jun  Wu Yan  Wang Yuanzhang  Yu Meifang  Yang Jianrong  Ding Ruijun  Hu Xiaoning  Li Yanjin  Zhang Qinyao
Affiliation:Research Center for Advanced Materials and Devices,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200083,China;Research Center for Advanced Materials and Devices,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200084,China;Research Center for Advanced Materials and Devices,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200085,China;Research Center for Advanced Materials and Devices,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200086,China;Research Center for Advanced Materials and Devices,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200087,China;Research Center for Advanced Materials and Devices,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200088,China;Research Center for Advanced Materials and Devices,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200089,China;Research Center for Advanced Materials and Devices,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200090,China;Research Center for Advanced Materials and Devices,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200091,China;Research Center for Advanced Materials and Devices,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200092,China;Research Center for Advanced Materials and Devices,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200093,China
Abstract:Some results on the molecular-beam epitaxial growth of HgCdTe focusing on the requirements of the 3rd generation infrared focal plane arrays are described. Good uniformity is observed over 75mm HgCdTe epilayers,and the deviation in cutoff wavelength is within 0.1μat 80K. A variety of surface defects are observed and the formation mechanism is discussed. The average density of surface defects in 75mm HgCdTe epilayers is found to be less than 300cm- 2. It is found that the surface sticking coefficient of As during HgCdTe growth is very low and is sensitive to growth temperature, being only ~ 1 × 10-4 at 170℃. The activation energy of As in HgCdTe was determined to be 19.5meV, which decreases as (Na - Nd)1/3 with a slope of 3.1 × 10-5 meV · cm. The diffusion coefficients of As in HgCdTe of 1.0 ± 0.9 × 10-16 ,8 ± 3 × 10-15 ,and 1.5 ± 0.9 × 10-13cm2/s are obtained at temperatures of 240,380, and 440℃, respectively under Hg-saturated pressure. The MBE-grown HgCdTe is incorporated into FPA fabrications, and the preliminary results are presented.
Keywords:MBE  HgCdTe  infrared focal plane arrays
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