Detection of Hole Pockets in the Candidate Type-II Weyl Semimetal MoTe2 from Shubnikov-de Haas Quantum Oscillations

被引:16
|
作者
Hu, Y. J. [1 ]
Yu, W. C. [1 ,2 ]
Lai, Kwing To [1 ]
Sun, D. [3 ]
Balakirev, F. F. [3 ]
Zhang, W. [1 ]
Xie, J. Y. [1 ]
Yip, K. Y. [1 ]
Aulestia, E. I. Paredes [1 ]
Jha, Rajveer [4 ]
Higashinaka, Ryuji [4 ]
Matsuda, Tatsuma D. [4 ]
Yanase, Y. [5 ]
Aoki, Yuji [4 ]
Goh, Swee K. [1 ]
机构
[1] Chinese Univ Hong Kong, Dept Phys, Shatin, Hong Kong, Peoples R China
[2] City Univ Hong Kong, Dept Phys, Kowloon, Hong Kong, Peoples R China
[3] Los Alamos Natl Lab, Natl High Magnet Field Lab, Los Alamos, NM 87545 USA
[4] Tokyo Metropolitan Univ, Dept Phys, Hachioji, Tokyo 1920397, Japan
[5] Kyoto Univ, Dept Phys, Kyoto 6068502, Japan
基金
美国国家科学基金会;
关键词
Tellurium compounds - Electronic structure - Molybdenum compounds;
D O I
10.1103/PhysRevLett.124.076402
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The bulk electronic structure of T-d-MoTe2 features large hole Fermi pockets at the Brillouin zone center (Gamma) and two electron Fermi surfaces along the Gamma-X direction. However, the large hole pockets, whose existence has important implications for the Weyl physics of T-d-MoTe2, has never been conclusively detected in quantum oscillations. This raises doubt about the realizability of Majorana states in T-d-MoTe2, because these exotic states rely on the existence of Weyl points, which originated from the same band structure predicted by density functional theory (DFT). Here, we report an unambiguous detection of these elusive hole pockets via Shubnikov-de Haas (SdH) quantum oscillations. At ambient pressure, the quantum oscillation frequencies for these pockets are 988 and 1513 T, when the magnetic field is applied along the c axis. The quasiparticle effective masses m* associated with these frequencies are 1.50 and 2.77 m(e), respectively, indicating the importance of Coulomb interactions in this system. We further measure the SdH oscillations under pressure. At 13 kbar, we detected a peak at 1798 T with m* = 2.86 m(e). Relative to the oscillation data at a lower pressure, the amplitude of this peak experienced an enhancement, which can be attributed to the reduced curvature of the hole pockets under pressure. Combining our experimental data with DFT + U calculations, where U is the Hubbard parameter, our results shed light on why these important hole pockets have not been detected until now.
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页数:6
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