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负带隙HgCdTe体材料的磁输运特性研究
引用本文:沈丹萍,张晓东,孙艳,康亭亭,戴宁,褚君浩,俞国林.负带隙HgCdTe体材料的磁输运特性研究[J].物理学报,2017,66(24):247301-247301.
作者姓名:沈丹萍  张晓东  孙艳  康亭亭  戴宁  褚君浩  俞国林
作者单位:1. 东华大学理学院, 上海 201620;2. 中国科学院上海技术物理研究所, 红外物理国家重点实验室, 上海 200083
基金项目:国家重点研发计划(批准号:2016YFA0202201)和国家自然科学基金(批准号:11774367)资助的课题.
摘    要:通过单晶生长了Cd组分为0.1的p型HgCdTe体材料,并制备了具有倒置型能带序的HgCdTe场效应器件.通过磁输运测试,在负带隙HgCdTe体材料中观察到明显的量子霍尔平台效应和Shubnikov-de Haas(SdH)振荡效应,证明样品具有较好的质量.利用SdH振荡对1/B关系的快速傅里叶变换,得到了样品的零场自旋分裂能约为26.55 meV,证明样品中存在强自旋-轨道耦合作用.进一步分析SdH中的拍频节点估算了样品中的有效g因子约为–11.54.

关 键 词:HgCdTe  Shubnikov-de  Haas振荡  零场自旋分裂能
收稿时间:2017-06-14

Magnetotransport property of negative band gap HgCdTe bulk material
Shen Dan-Ping,Zhang Xiao-Dong,Sun Yan,Kang Ting-Ting,Dai Ning,Chu Jun-Hao,Yu Guo-Lin.Magnetotransport property of negative band gap HgCdTe bulk material[J].Acta Physica Sinica,2017,66(24):247301-247301.
Authors:Shen Dan-Ping  Zhang Xiao-Dong  Sun Yan  Kang Ting-Ting  Dai Ning  Chu Jun-Hao  Yu Guo-Lin
Affiliation:1. Science College, Donghua University, Shanghai 201620, China;2. State Key Laboratory of Infrared Physics, Shanghai Institute of Technical Physics, Chinese Academy of Sciences, Shanghai 200083, China
Abstract:In recent years, spintronic devices have attracted more and more attention because of their good characteristics. The spin-orbit coupling of HgCdTe is one of the most important parts in the study of narrow gap semiconductors. The magneotransport properties of the Hg0.9Cd0.1Te bulk material with an inverted band structure have been hardly reported so far. The spin-orbit coupling strength of HgCdTe is closely related to the band gap. The strength of the spin-orbit coupling increases with the width of the band gap decreasing. Thus, Hg0.9Cd0.1Te should have strong spin-orbit coupling. Meanwhile it should be one of the most suitable materials to fabricate spintronic devices. The main propose of our experiments is to prove this inference. Inside the sample, Rashba spin-orbit interaction (SOI) strongly influences the spin-splitting due to the lack of structural inversion symmetry. In other words, Rashba SOI is the main part of the zero field spin splitting 0. The band structure of Hg1-xCdxTe can be precisely tuned by changing the composition of Cd which keeps an inverted band order when 0 < x < 0.165 and returns to the normal case with the Γ8 band lying below the Γ6 band (or equivalently a positive band gap) when x0.165. In this paper, the p-type HgCdTe bulk material with Cd component of 0.1 is grown by single crystal. Anodic oxidation is used to induce an inversion layer on the HgCdTe bulk, and indium is used to facilitate Ohmic contacts. The magnetoresistance is measured in the van der Pauw configuration, and the magnetic field is applied perpendicularly to the film. All measurements are carried out in an Oxford Instruments He cryogenic system. At 1.5 K and zero gate voltage, the carrier density n is 1.3×1016 m-2. Clear Shubnikov-de Haas (SdH) oscillation in ρxx and quantum Hall plateaus of Rxy are observed in the Hg0.9Cd0.1Te bulk material with an inverted band structure is investigated in magnetotransport experiment. This indicates that our sample is a good transistor. Fast Fourier transformation is used to deduce the zero-field spin-splitting 0 which is about 26.55 meV. By studying the beating patterns in SdH oscillations we find that the effective g-factor is about-11.54. Both the large zero field spin splitting and the negative effective g-factor suggest that Hg0.9Cd0.1Te has really strong spin-orbit coupling. The investigation of SOI in Hg0.9Cd0.1Te can increase our knowledge of Hg-based narrow-gap semiconductors and benefit the field of spintronics.
Keywords:HgCdTe  Shubnikov-de Haas oscillation  zero-field spin-splitting
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