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Superconductivity of topological matters induced via pressure |
Jun-liang Zhang1,2, Si-jia Zhang1, Hong-ming Weng1, Wei Zhang1, Liu-xiang Yang1, Qing-qing Liu1, Pan-pan Kong1, Jie Zhu1, Shao-min Feng1, Xian-cheng Wang1, Ri-cheng Yu1, Lie-zhao Cao2, Shoucheng Zhang3, Xi Dai1, Zhong Fang1, Chang-qing Jin1( ) |
1. Beijing National Laboratory for Condensed Matter Physics & Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China; 2. Department of Physics, University of Science & Technology of China, Hefei 230026, China; 3. Department of Physics, McCullough Building, Stanford University, Stanford, CA 94305-4045, USA & Center for Advanced Study, Tsinghua University, Beijing 100084, China |
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Abstract By applying pressure on the topological insulator Bi2Te3 single crystal, superconducting phase was found without a crystal structure phase transition. The new superconducting phase is under the pressure range of 3 GPa to 6 GPa. The high pressure Hall effect measurements indicated that the superconductivity caused by bulk hole pockets. The high pressure structure investigations with synchrotron X-ray diffraction indicated that the superconducting phase is of similar structure to that of ambient phase structure with only slight change with lattice parameter and internal atomic position. The topological band structures indicate the superconducting phase under high pressure remained topologically nontrivial. The results suggested that topological superconductivity can be realized in Bi2Te3 due to the proximity effect between superconducting bulk states and Diractype surface states. We also discussed the possibility that the bulk state could be a topological superconductor.
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Keywords
topological insulator
high pressure
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Corresponding Author(s):
Jin Chang-qing,Email:Jin@iphy.ac.cn
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Issue Date: 01 April 2012
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