Nearly isotropic superconductivity in layered Weyl semimetal WTe at 98.5 kbar
arXiv:1711.00666 · doi:10.1103/PhysRevB.96.180504
Abstract
Layered transition metal dichalcogenide WTe has recently attracted significant attention due to the discovery of an extremely large magnetoresistance, a predicted type-II Weyl semimetallic state, and the pressure-induced superconducting state. By a careful measurement of the superconducting upper critical fields as a function of the magnetic field angle at a pressure as high as 98.5 kbar, we provide the first detailed examination of the dimensionality of the superconducting condensate in WTe. Despite the layered crystal structure, the upper critical field exhibits a negligible field anisotropy. The angular dependence of the upper critical field can be satisfactorily described by the anisotropic mass model from 2.2 K () to 0.03 K (), with a practically identical anisotropy factor . The temperature dependence of the upper critical field, determined for both and , can be understood by a conventional orbital depairing mechanism. Comparison of the upper critical fields along the two orthogonal field directions results in the same value of , leading to a temperature independent anisotropy factor from near to . Our findings thus identify WTe as a nearly isotropic superconductor, with an anisotropy factor among one of the lowest known in superconducting transition metal dichalcogenides.
arXiv comment6 pages, 4 figures. Accepted for publication in Phys. Rev. B (Rapid Comm.)
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