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B,P掺杂β-Si3N4的电子结构和光学性质研究
引用本文:程超群,李刚,张文栋,李朋伟,胡杰,桑胜波,邓霄.B,P掺杂β-Si3N4的电子结构和光学性质研究[J].物理学报,2015,64(6):67102-067102.
作者姓名:程超群  李刚  张文栋  李朋伟  胡杰  桑胜波  邓霄
作者单位:1. 太原理工大学,新型传感器与智能控制教育部和山西省重点实验室, 信息工程学院微纳系统研究中心, 太原 030024;2. 太原理工大学 物理与光电工程学院, 太原 030024
基金项目:国家自然科学基金(批准号:51205275,51205276,51205273);国家高技术研究发展计划(批准号:2013AA041109);山西省自然科学基金(批准号:2013021017-1);山西省回国留学人员科研资助项目(批准号:2013-035)资助的课题~~
摘    要:运用第一性原理方法, 计算了B, P两种元素单掺杂和共掺杂的β -Si3N4材料的电子结构和光学性质. 结果表明: B掺杂体系的稳定性更高, 而P掺杂体系的离子性更强; 单掺和共掺杂均窄化带隙, 且共掺在禁带中引入深能级, 使局域态增强; 单掺杂体系介电函数虚部、吸收谱和能量损失谱各峰均发生红移、幅值减小, 而共掺后介电函数虚部主峰出现蓝移、能量损失峰展宽、高能区电子跃迁大大增强, 且控制共掺杂的B, P比例可获得较低的带电缺陷浓度.

关 键 词:β  相氮化硅  掺杂  第一性原理  光电性质
收稿时间:2014-06-23

Electronic structures and optical properties of boron and phosphorus doped β-Si3N4
Cheng Chao-Qun;Li Gang;Zhang Wen-Dong;Li Peng-Wei;Hu Jie;Sang Sheng-Bo;Deng Xiao.Electronic structures and optical properties of boron and phosphorus doped β-Si3N4[J].Acta Physica Sinica,2015,64(6):67102-067102.
Authors:Cheng Chao-Qun;Li Gang;Zhang Wen-Dong;Li Peng-Wei;Hu Jie;Sang Sheng-Bo;Deng Xiao
Institution:1. MicroNano System Research Center, Key Laboratory of Advanced Transducers and Intelligent Control (Shanxi Province and Ministry of Education) and College of Information Engineering, Taiyuan University of Technology, Taiyuan 030024, China;2. College of Physics and Optoelectronics, Taiyuan University of Technology, Taiyuan 030024, China
Abstract:The electronic structures and optical properties of boron/phosphorus mono- and co-doped β silicon nitride are studied by the first-principles plane-wave ultrasoft pseudopotential method with the generalized gradient approximation. The results are obtained as follows. The B-doped system has a better stability than the P-doped system, while the P-doped structure has a stronger ionicity. The mono-doping and co-doping can narrow the band gap of β silicon nitride while the co-doping introduces the deep impurity levels and strengthens the localized states. The mono-doping causes the imaginary part of dielectric function, the peaks of absorption spectra and energy loss spectra to red-shift, and their amplitudes to decrease, resulting in a significant difference from the intrinsic state. The co-doping induces the peak of imaginary part of the dielectric function to blue-shift, broadens the energy loss peak, greatly enhances the electronic transition in the high energy region, and controlling the ratio of the numbers of atoms (B and P) in co-doping can achieve a low charged defect concentration, implying its potential application in the field of microelectronics.
Keywords:β-Si3N4  doping  first-principles  optical and electrical properties
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