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B在Hg0.75Cd0.25Te中掺杂效应的第一性原理研究
引用本文:唐冬华,薛林,孙立忠,钟建新.B在Hg0.75Cd0.25Te中掺杂效应的第一性原理研究[J].物理学报,2012,61(2):27102-027102.
作者姓名:唐冬华  薛林  孙立忠  钟建新
作者单位:湘潭大学量子工程与微纳能源技术湖南省高校重点实验室, 湘潭 411105;湘潭大学材料与光电物理学院, 湘潭 411105;湘潭大学量子工程与微纳能源技术湖南省高校重点实验室, 湘潭 411105;湘潭大学材料与光电物理学院, 湘潭 411105;湘潭大学量子工程与微纳能源技术湖南省高校重点实验室, 湘潭 411105;湘潭大学材料与光电物理学院, 湘潭 411105;湘潭大学量子工程与微纳能源技术湖南省高校重点实验室, 湘潭 411105;湘潭大学材料与光电物理学院, 湘潭 411105
基金项目:国家自然科学基金(批准号:10874143,10774127),教育部博士点新教师基金 (批准号:20070530008)和湖南省高校创新平台开放基金(批准号:10K065)资助的课题.
摘    要:基于密度泛函理论的第一性原理方法,通过形成能和束缚能的计算研究了B在Hg0.75Cd0.25Te 中的掺杂效应.结果表明B在Hg0.75Cd0.25Te中存在着两种主要形态:第一种是在完整的 Hg0.75Cd0.25Te材料中B稳定存在于六角间隙位置而非替位.此时,B形成容易激活的三级施主使材料表现为n型.另一种是在有Hg空位存在的Hg0.75Cd0.25Te中B更容易与Hg空位结合形成缺陷复合体,其束缚能达到了0.96 eV.这种复合体在Hg0.75Cd0.25Te材料中形成单施主也使材料表现为n型.考虑到辐照损伤形成的Hg空位受主,这种B与Hg空位的复合体是制约B离子在MCT中注入激活的一个重要因素.

关 键 词:碲镉汞(MCT)  B掺杂  第一性原理  形成能
收稿时间:2012-02-27

Doping effect of boron in Hg0.75Cd0.25Te: first-principles study
Tang Dong-Hu,Xue Lin,Sun Li-Zhong and Zhong Jian-Xin.Doping effect of boron in Hg0.75Cd0.25Te: first-principles study[J].Acta Physica Sinica,2012,61(2):27102-027102.
Authors:Tang Dong-Hu  Xue Lin  Sun Li-Zhong and Zhong Jian-Xin
Institution:Laboratory for Quantum Engineering and Micro-Nano Energy Technology Xiangtan 411105, China; Faculty of Materials, Optoelectronics and Physics of Xiangtan University, Xiangtan 411105, China;Laboratory for Quantum Engineering and Micro-Nano Energy Technology Xiangtan 411105, China; Faculty of Materials, Optoelectronics and Physics of Xiangtan University, Xiangtan 411105, China;Laboratory for Quantum Engineering and Micro-Nano Energy Technology Xiangtan 411105, China; Faculty of Materials, Optoelectronics and Physics of Xiangtan University, Xiangtan 411105, China;Laboratory for Quantum Engineering and Micro-Nano Energy Technology Xiangtan 411105, China; Faculty of Materials, Optoelectronics and Physics of Xiangtan University, Xiangtan 411105, China
Abstract:Using the first-principles method based on the density functional theory, we study the doping effect of B impurity in HgCdTe (MCT).We find that the most stable configuration of the impurity is at the B hexagonal interstitial position, rather than at the in-situ substitution. The electronic structures and the density of states of B hexagonal interstitial doped MCT are systematically investigated. Near neighbour (NN) and next-near-neighbor (NNN) atoms around the B impurity are obviously relaxed. The relaxation induces the breaking of NN Te-Hg covalent bond. Moreover, B hexagonal interstitial behaves as triple n-type dopant. The charged state analysis indicates that Bih(2Hg1Cd) with three positive charges is most stable and forms an effecient donor. However, as long as the Hg vacancy exists, complex impurity between Hg vacancy and B impurity can be easily formed, its binding energy reaches up to 0.96 eV. Such complex behaves as single n-type dopant. Considering radiation damage of B ion implantation, the complex is a main factor restricting the activation of B ion in MCT.
Keywords:mercury cadmium telluride(MCT)  B doping  formation energy  first-principles study
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