J4 ›› 2018, Vol. 35 ›› Issue (4): 507-512.

• 半导体光电 • 上一篇    

Zn空位缺陷ZnS的电子状态,磁性质与光学性质的研究

韦树贡,房 慧,王如志,李凡生,黄灿胜,郝五零,孙 毅   

  1. 1 广西民族师范学院物理与电子工程学院,广西 崇左 532200; 2 北京工业大学材料科学与工程学院,北京 100124; 3 云南师范大学数学学院,云南 昆明 650500; 4 昌吉学院物理系,新疆 昌吉 831100
  • 收稿日期:2017-04-05 修回日期:2017-05-17 出版日期:2018-07-28 发布日期:2018-07-12
  • 通讯作者: 韦树贡(1974-),广西环江人,硕士,讲师,主要从事凝聚态物理及实验方面的研究。 E-mail:weisggxnun@163.com
  • 基金资助:

    Supported by National Natural Science Foundation of China(国家自然科学基金,11347141, 11402225),Natural Science Foundation of Guangxi Province(广西自然科学基金,2015GXNSFBA139014),Natural Science Foundation of Yunnan Province(云南省自然科学基金,2016FB012)

Electronic states, magnetic and optical properties of Zn vacant ZnS

WEI Shugong, FANG Hui, WANG Ruzhi, LI Fansheng, HUANG Cansheng, HAO Wuling, SUN Yi   

  1. 1 College of Physics and Electronic Engineering, Guangxi Normal University for Nationalities, Chongzuo 532200, China; 2 College of Materials Science and Engineering, Beijing University of Technology, Beijing 100124, Beijing; 3 Department of Mathematics, Yunnan Normal University, Kunming 650500, China; 4 Department of Physics,Changji University, Changji 831100,China
  • Received:2017-04-05 Revised:2017-05-17 Published:2018-07-28 Online:2018-07-12

摘要:

基于密度泛函理论第一性原理,研究了Zn空位缺陷对ZnS半导体材料电子状态、磁性质和光学性质的影响。结果表明Zn空位缺陷浓度为6.25%时,ZnS半导体材料仍呈直接带隙型能带结构,带隙较本征ZnS半导体增大了6.4%,达到2.19 eV。缺陷体系s态、p态电子主要在距离费米能量较近的区域产生能带,数量较少;Znd态电子主要在距离费米能量较远的区域产生能带。Zn空位缺陷对ZnS半导体材料是一种空穴型掺杂,Zn空位会增加ZnS的空穴型载流子浓度。其价带空穴具有较大有效质量,导带电子具有较小有效质量,Zn空位缺陷ZnS不显示磁性。Zn空位缺陷ZnS半导体材料210 nm附近介电吸收峰强度降低,170 nm附近介电吸收峰消失,100 nm波长附近出现了较弱的介电吸收峰。

关键词: 材料;ZnS;Zn空位缺陷;磁性;光学性质

Abstract:

Influences of Zn vacancy defect on electronic states, magnetic and optical properties of ZnS semiconductor material are investigated by density functional theory first principle. Results show that when the concentration of Zn vacancy defect is 6.25%, ZnS semiconductor material still exhibits a direct band gap structure. Compared with the intrinsic ZnS semiconductor, the band gap is increased by 6.4%, reaching 2.19 eV. The s and p state electrons of defect system form the energy bands near Fermi energy, few in number, and Znd electrons form the energy bands far from Fermi energy. The Zn vacancy for ZnS semiconductor is a kind of hole doping type and the hole carrier concentration can be increased by Zn vacancy. Its hole carriers within the valence bands are heavy and the electron carriers within the conduction bands are light. Zn vacant ZnS does not show magnetism. The dielectric absorption peak intensity of Zn vacant ZnS semiconductor near 210 nm decreases, the dielectric absorption peak near 170 nm disappears and a weaker dielectric absorption peak near 100 nm emerges.

Key words: materials; ZnS; Zn vacancy defect; magnetic properties; optical properties

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