Topological phase transition induced extreme magnetoresistance in TaSb
arXiv:1603.01717
Abstract
We report extremely large positive magnetoresistance of 1.72 million percent in single crystal TaSb at moderate conditions of 1.5 K and 15 T. The quadratic growth of magnetoresistance (MR ) is not saturating up to 15 T, a manifestation of nearly perfect compensation with mismatch between electron and hole pockets in this semimetal. The compensation mechanism is confirmed by temperature-dependent MR, Hall and thermoelectric coefficients of Nernst and Seebeck, revealing two pronounced Fermi surface reconstruction processes without spontaneous symmetry breaking, \textit{i.e.} Lifshitz transitions, at around 20 K and 60 K, respectively. Using quantum oscillations of magnetoresistance and magnetic susceptibility, supported by density-functional theory calculations, we determined that the main hole Fermi surface of TaSb forms a unique shoulder structure along the line. The flat band top of this shoulder pocket is just a few meV above the Fermi level, leading to the observed topological phase transition at 20 K when the shoulder pocket disappears. Further increase in temperature pushes the Fermi level to the band top of the main hole pocket, induced the second Lifshitz transition at 60 K when hole pocket vanishes completely.
4 figures
Cited by in corpus (7)
- The extremely large magnetoresistance in the Candidate Type-II Weyl semimetal MoTe2
- Negative Magnetoresistance in Weyl semimetals NbAs and NbP: Intrinsic Chiral Anomaly and Extrinsic Effects
- Extremely large magnetoresistance in topologically trivial semimetal -WP
- Tuning the electronic and the crystalline structure of LaBi by pressure
- Anisotropic Fermi surface probed by the de Haas-van Alphen oscillation in proposed Dirac Semimetal TaSb
- Negative Magnetoresistance in Topological Semimetals of Transition-Metal Dipnictides with Nontrivial Z2 Indices
- Magnetoresistance and Scaling Laws in Type-II Weyl Semimetal WP_2