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JOURNALS // Pis'ma v Zhurnal Èksperimental'noi i Teoreticheskoi Fiziki // Archive

Pis'ma v Zh. Èksper. Teoret. Fiz., 2017 Volume 105, Issue 8, Pages 504–505 (Mi jetpl5247)

This article is cited in 10 papers

METHODS OF THEORETICAL PHYSICS

Lifshitz transitions via the type-II Dirac and type-II Weyl points

K. Zhangab, G. E. Volovikcb

a State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Laser Spectroscopy, Shanxi University, 030006 Taiyuan, P. R. China
b Low Temperature Laboratory, Aalto University, P.O. Box 15100, FI-00076 Aalto, Finland
c Landau Institute for Theoretical Physics, Russian Academy of Sciences, 119334 Moscow, Russia

Abstract: The type-II Weyl and type-II Dirac points emerge in semimetals and in relativistic systems. In particular, the type-II Weyl fermions may emerge behind the event horizon of black holes. The type-II Weyl and Dirac points also emerge as the intermediate states of the topological Lifshitz transitions. In one case, the type-II Weyl point connects the Fermi pockets, and the Lifshitz transition corresponds to the transfer of the Berry flux between the Fermi pockets. In the other case, the type-II Weyl point connects the outer and inner Fermi surfaces. At the Lifshitz transition, the Weyl point is released from both Fermi surfaces. They loose their Berry flux, which guarantees the global stability, and without the topological support, the inner surface disappears after shrinking to a point at the second Lifshitz transition. These examples reveal the complexity and universality of topological Lifshitz transitions, which originate from the ubiquitous interplay of a variety of topological characters of the momentum-space manifolds.

Received: 14.03.2017

Language: English

DOI: 10.7868/S0370274X17080094


 English version:
Journal of Experimental and Theoretical Physics Letters, 2017, 105:8, 519–525

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© Steklov Math. Inst. of RAS, 2024