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人工晶体学报 ›› 2022, Vol. 51 ›› Issue (1): 77-84.

• 研究论文 • 上一篇    下一篇

GGA+U方法研究C与Ti掺杂GaN的电子结构和光学性质

刘纪博1, 庞国旺1, 马磊1, 刘丽芝1, 王晓东1, 史蕾倩1, 潘多桥1, 刘晨曦1, 张丽丽1, 雷博程1, 赵旭才1, 黄以能1,2   

  1. 1.伊犁师范大学物理科学与技术学院,新疆凝聚态相变与微结构实验室,伊宁 835000;
    2.南京大学物理学院,固体微结构物理国家重点实验室,南京 210093
  • 收稿日期:2021-10-11 出版日期:2022-01-15 发布日期:2022-02-09
  • 通讯作者: 张丽丽,博士,副教授。E-mail:suyi2046@sina.com;雷博程,讲师。E-mail:lbc0428@sina.com
  • 作者简介:刘纪博(1998—),男,新疆维吾尔族自治区人,硕士研究生。E-mail:liujibo1207@163.com
  • 基金资助:
    伊犁师范大学博士启动基金(2021YSBS009);新疆维吾尔自治区重点实验室开放课题(2021D04015);新疆维吾尔自治区高校科技计划项目(XJEDU2021Y044);伊犁师范大学科研项目(2020YSYB010))

Electronic Structure and Optical Properties of C and Ti Doped GaN by GGA+U Method

LIU Jibo1, PANG Guowang1, MA Lei1, LIU Lizhi1, WANG Xiaodong1, SHI Leiqian1, PAN Duoqiao1, LIU Chenxi1, ZHANG Lili1, LEI Bocheng1, ZHAO Xucai1, HUANG Yineng1,2   

  1. 1. Xinjiang Laboratory of Phase Transitions and Microstructures in Condensed Matters, College of Physical Science and Technology, Yili Normal University, Yining 835000, China;
    2. National Laboratory of Solid State Microstructures, School of Physics, Nanjing University, Nanjing 210093, China
  • Received:2021-10-11 Online:2022-01-15 Published:2022-02-09

摘要: 作为一种优良的半导体材料,GaN所具有的宽禁带导致其只能吸收可见光中的紫光,因此如何增加GaN材料对可见光的利用率是一个值得研究的问题,掺杂是解决这个问题常用的手段。本文利用第一性原理的方法对本征GaN,C单掺、Ti单掺、C-Ti共掺GaN四种体系的电子结构和光学性质做了计算和分析,结果表明:掺杂后的体系都具有良好的稳定性;掺杂后各体系的体积均增大,说明杂质的引入使体系晶格发生畸变,对光生空穴-电子对的分离有促进作用,进而提高材料的光催化性能;杂质元素的引入使体系能级发生劈裂,电子跃迁更加容易;掺杂后各体系的介电函数虚部主峰均向低能区移动,吸收谱均红移至可见光区域,其中共掺体系在蓝绿光区域的吸收系数最大,由此可以推测C-Ti共掺有助于提高GaN的光催化性能。

关键词: 第一性原理, 哈伯德U修正, GaN, 掺杂, 电子结构, 光学性质, 半导体

Abstract: As an excellent semiconductor material, GaN has a wide band gap, which causes it to only absorb violet light in visible light. Therefore, how to increase the utilization rate of visible light of GaN material is a problem worthy of study. Doping is commonly used to solve this problem. Therefore, this paper uses the first-principles method to calculate the electronic structure and optical properties of the intrinsic GaN, C single-doped, Ti single-doped, and C-Ti co-doped GaN. The results show that the stability of the system after doping is all good; the volume of each system increases after doping, indicating that the introduction of impurities causes distortion of the system lattice, which helps to promote the separation of photogenerated hole-electron pairs, and further improves the photocatalytic performance of the material; the energy level of the system is split and the electronic transition is easier after the introduction of impurity elements; after doping, the main peak of the imaginary part of the dielectric function of each system moves to the low-energy region, and the absorption spectrum is red-shifted to the visible light region, and the co-doped system is in the blue-green light region, and the absorption coefficient is the largest, so it can be inferred that C-Ti co-doping will help improve the photocatalytic performance of GaN.

Key words: first-principle, Hubbard U correction, GaN, doping, electronic structure, optical property, semiconductor

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