Universal superconductivity phase diagram for pressurized tetradymite topological insulators

Shu Cai, S. K. Kushwaha, Jing Guo, Vladimir A. Sidorov, Congcong Le, Yazhou Zhou, Honghong Wang, Gongchang Lin, Xiaodong Li, Yanchuan Li, Ke Yang, Aiguo Li, Qi Wu, Jiangping Hu, Robert J. Cava, and Liling Sun
Phys. Rev. Materials 2, 114203 – Published 13 November 2018
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Abstract

We show that two different superconducting phases exist at high pressures in the optimized tetradymite topological insulators Bi2Te2Se (BTS) and Bi1.1Sb0.9Te2S (BSTS). The superconducting phases emerge at structural phase transitions; the first at 8.4GPa for BTS and 12.4GPa for BSTS, and the second at 13.6 GPa for BTS and 20.4 GPa, for BSTS. Electronic structure calculations show that these phases do not have topological character. Comparison of our results with prior work on Bi2Se3, Bi2Te3, and (Bi,Sb)2(Se,Te)3 allows us to uncover a universal phase diagram for pressure-induced superconductivity in tetradymites, providing a basis for understanding the relationships between topological behavior, crystal structure, and superconductivity for these materials.

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  • Received 4 September 2018

DOI:https://doi.org/10.1103/PhysRevMaterials.2.114203

©2018 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Shu Cai1,4, S. K. Kushwaha2,9, Jing Guo1, Vladimir A. Sidorov3, Congcong Le1,5, Yazhou Zhou1, Honghong Wang1,4, Gongchang Lin1,4, Xiaodong Li6, Yanchuan Li6, Ke Yang7, Aiguo Li7, Qi Wu1, Jiangping Hu1,4, Robert J. Cava2,*, and Liling Sun1,4,8,†

  • 1Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 2Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA
  • 3Institute for High Pressure Physics, Russian Academy of Sciences, 142190 Troitsk, Moscow, Russia
  • 4University of Chinese Academy of Sciences, Beijing 100190, China
  • 5Kavli Institute of Theoretical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
  • 6Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China
  • 7Shanghai Synchrotron Radiation Facilities, Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai 201204, China
  • 8Songshan Lake Materials Laboratory, Dongguan, Guangdong 523808, China
  • 9National High Magnetic Field Laboratory, LANL, Los Alamos, New Mexico 87504, USA

  • *Author to whom correspondence should be addressed: rcava@Princeton.EDU
  • llsun@iphy.ac.cn

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Issue

Vol. 2, Iss. 11 — November 2018

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