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Fe掺杂GaN晶体非极性面的光学各向异性研究
引用本文:武圆梦,胡俊杰,王淼,易觉民,张育民,王建峰,徐科. Fe掺杂GaN晶体非极性面的光学各向异性研究[J]. 人工晶体学报, 2022, 51(6): 996-1002
作者姓名:武圆梦  胡俊杰  王淼  易觉民  张育民  王建峰  徐科
作者单位:中国科技大学纳米技术与纳米仿生学院,合肥 230026;中国科学院苏州纳米技术与纳米仿生研究所,苏州 215123;中国科技大学纳米技术与纳米仿生学院,合肥 230026;中国科学院苏州纳米技术与纳米仿生研究所,苏州 215123;江苏第三代半导体研究院,苏州 215000;中国科技大学纳米技术与纳米仿生学院,合肥 230026;中国科学院苏州纳米技术与纳米仿生研究所,苏州 215123;江苏第三代半导体研究院,苏州 215000;苏州纳维科技股份有限公司,苏州 215123
基金项目:国家自然科学基金(62174175);
摘    要:本文利用低温光致发光谱(PL)研究了Fe掺杂GaN晶体非极性a面{1120}、m面{1100} 的带边峰和Fe3+相关峰(4T1(G)- 6A1(S))的偏振发光特性。结果表明:a面与m面光学各向异性差别较小,线偏振光的电矢量E平行于c轴[0001]时(E∥c),GaN带边峰强度最小,而Fe3+零声子峰(1.299 eV)强度最强。带边峰线偏振度小,而Fe3+零声子峰线偏振度大,a面带边峰的线偏振度为26%,Fe3+零声子峰的偏振度在a面和m面分别达到55%和58%。在5 K低温下,进一步测量了Fe3+精细峰和声子伴线的偏振特性,结果表明,除了一个微弱的峰外,其他精细峰和声子伴线与Fe3+零声子峰偏振特性一致。本研究有助于拓展Fe掺杂GaN晶体材料在新型偏振光电器件领域的应用。

关 键 词:氮化镓  Fe掺杂  半绝缘  非极性面  光学各向异性  光电特性  偏振光
收稿时间:2022-03-08

Optical Anisotropy of Non-Polar Surfaces of Fe-Doped GaN Crystal
WU Yuanmeng,HU Junjie,WANG Miao,YI Juemin,ZHANG Yumin,WANG Jianfeng,XU Ke. Optical Anisotropy of Non-Polar Surfaces of Fe-Doped GaN Crystal[J]. Journal of Synthetic Crystals, 2022, 51(6): 996-1002
Authors:WU Yuanmeng  HU Junjie  WANG Miao  YI Juemin  ZHANG Yumin  WANG Jianfeng  XU Ke
Affiliation:1. School of Nano-Tech and Nano-Bionics, University of Science and Technology of China, Hefei 230026, China; 2. Suzhou Institute of Nano-Tech and Nano-Bionics, Chinese Academy of Sciences, Suzhou 215123, China; 3. Jiangsu Institute of Advanced Semiconductors Ltd., Suzhou 215000, China; 4. Suzhou Nanowin Science and Technology Co., Ltd., Suzhou 215123, China
Abstract:In this paper, the polarization luminescence characteristics of the near-band-edge peak and Fe3+ related emission peaks(4T1(G)-6A1(S)) of the non-polar surfaces including a-plane {1120} and m-plane {1100} of Fe-doped GaN crystal were studied by low-temperature photoluminescence(PL) measurement. The results show that the optical anisotropy of a-plane and m-plane are similar. When the linearly polarized electric-field vector E is parallel to the c-direction [0001] (E//c), the intensity of GaN near-band-edge peak is the lowest, and the intensity of Fe3+ zero-phonon line (1.299 eV) is the strongest. The degree of polarization of Fe3+ zero-phonon line is greater than that of near-band-edge peak. The degree of polarization of near-band-edge peak of a-plane is 26%, while the degree of polarization of Fe3+ zero-phonon line reaches up to 55% and 58% of a-plane and m-plane GaN, respectively. The polarization characteristics of Fe3+ fine peak and the additional lines are further measured at 5 K. The results show that, except for one weak peak, other peaks are consistent with the polarization characteristics of Fe3+ zero-phonon line. This study is helpful to expand the application of Fe-doped GaN crystal in the field of novel optical and electrical devices.
Keywords:GaN   Fe doping   semi-insulating   non-polar surface   optical anisotropy   optical and electrical property   polarized light  
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