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Pressure-induced superconductivity in topological parent compound Bi2Te3.


ABSTRACT: We report a successful observation of pressure-induced superconductivity in a topological compound Bi(2)Te(3) with T(c) of ?3 K between 3 to 6 GPa. The combined high-pressure structure investigations with synchrotron radiation indicated that the superconductivity occurred at the ambient phase without crystal structure phase transition. The Hall effects measurements indicated the hole-type carrier in the pressure-induced superconducting Bi(2)Te(3) single crystal. Consequently, the first-principles calculations based on the structural data obtained by the Rietveld refinement of X-ray diffraction patterns at high pressure showed that the electronic structure under pressure remained topologically nontrivial. The results suggested that topological superconductivity can be realized in Bi(2)Te(3) due to the proximity effect between superconducting bulk states and Dirac-type surface states. We also discuss the possibility that the bulk state could be a topological superconductor.

SUBMITTER: Zhang JL 

PROVIDER: S-EPMC3017179 | biostudies-literature | 2011 Jan

REPOSITORIES: biostudies-literature

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Pressure-induced superconductivity in topological parent compound Bi2Te3.

Zhang J L JL   Zhang S J SJ   Weng H M HM   Zhang W W   Yang L X LX   Liu Q Q QQ   Feng S M SM   Wang X C XC   Yu R C RC   Cao L Z LZ   Wang L L   Yang W G WG   Liu H Z HZ   Zhao W Y WY   Zhang S C SC   Dai X X   Fang Z Z   Jin C Q CQ  

Proceedings of the National Academy of Sciences of the United States of America 20101220 1


We report a successful observation of pressure-induced superconductivity in a topological compound Bi(2)Te(3) with T(c) of ∼3 K between 3 to 6 GPa. The combined high-pressure structure investigations with synchrotron radiation indicated that the superconductivity occurred at the ambient phase without crystal structure phase transition. The Hall effects measurements indicated the hole-type carrier in the pressure-induced superconducting Bi(2)Te(3) single crystal. Consequently, the first-principle  ...[more]

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