摘要
基于第一性原理方法研究了C单掺杂SnO_2和C-X(X=Y,Zr)共掺杂SnO_2的能带结构、态密度以及分电荷分布。结果表明:C掺杂、C-Y、C-Zr共掺杂SnO_2的带隙值分别为1. 109 e V、1. 86 e V、1. 214 e V,较超胞结构的带隙值降低,有利于电子的跃迁; C-Y共掺杂SnO_2的导带底部有3条杂质能级分离出来,C-Zr共掺杂SnO_2的能带价带顶部能级中有3条能级分离出来,其中1条能级贯穿费米能级; C-Y,C-Zr共掺杂SnO_2的态密度中在低能区会产生1个态密度峰值,部分态密度的峰值由Y、Zr的d轨道贡献; C-Y、C-Zr共掺杂SnO_2会打破SnO_2电子平衡状态,致使电荷的重新分布。
Band structures and densities of states of C-X(X=Y,Zr)co-doped SnO 2 by first principles.It is found that the band gap values of C doped,C-Y and C-Zr co-doped SnO 2 are 1.109 eV,1.86 eV,1.214 eV,respectively.Comparing with the pure SnO 2 the band gap decreases will help the transition of electrons.There is a separation of 3 energy levels at the bottom of the conduction band in the C-Y co-doped SnO 2 systems.There are three energy levels in the top of values band of C-Zr Co-doped SnO 2,the first level through the Fermi surface.The density of states of C-Y and C-Zr co-doped SnO 2 have 1 peak densities in the low energy region,the peak of the partial density of States is contributed by the d orbit of Y and Zr.The redistribution of SnO 2 charge is due to the role of C-X(X=Y,Zr)co doping.
作者
伏春平
黄浩
孙凌涛
夏继宏
程正富
FU Chun-ping;HUANG Hao;SUN Ling-tao;XIA Ji-hong;CHENG Zheng-fu(Deptment of Physics, Chongqing University of Arts and Sciences, Yongchuan 402160, China)
出处
《人工晶体学报》
EI
CAS
北大核心
2019年第1期127-130,136,共5页
Journal of Synthetic Crystals
基金
重庆市教委科技项目资助(KJ1601128)
重庆市高校微纳米材料工程与技术重点实验室开放课题基金(KF2016012)
重庆市高校新型储能器件及应用工程研究中心开放课题资助(KF20170106)
关键词
SNO2
能带结构
态密度
SnO 2
band structures
density of states