2018
DOI: 10.7566/jpsj.87.041001
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Recent Progress in the Study of Topological Semimetals

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Cited by 159 publications
(129 citation statements)
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“…In reality, the electron Hamiltonian for a topological semimetal is even simpler than that given by Eqs. (1), (2) [75,76] since for the Dirac point to be stable, an additional crystalline symmetry (other than the time-reversal and inversion symmetries) is necessary [77]; see, e.g., the electron spectrum of Na 3 Bi below.…”
Section: A Spectrum Without Magnetic Fieldmentioning
confidence: 99%
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“…In reality, the electron Hamiltonian for a topological semimetal is even simpler than that given by Eqs. (1), (2) [75,76] since for the Dirac point to be stable, an additional crystalline symmetry (other than the time-reversal and inversion symmetries) is necessary [77]; see, e.g., the electron spectrum of Na 3 Bi below.…”
Section: A Spectrum Without Magnetic Fieldmentioning
confidence: 99%
“…Thus, there is no topological transition with changing ζ in the caseã 2 > 1. The most general k · p HamiltonianĤ for the conduction and valence electron bands in the vicinity of a Weyl point has the form:Ĥ = (ε d + a · p)σ 0 + (a · p)σ z + (v (1) · p)σ x + (v (2) · p)σ y .…”
Section: A Spectrum Without Magnetic Fieldmentioning
confidence: 99%
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“…This new family of materials hosts a wide range of quantum quasiparticles like e.g Dirac, Weyl and Majorana fermions [5]. Material classes such as topological insulators (TI) [6,7], topological crystalline insulators (TCI) [8][9][10], topological superconductors (TSC) [10,11], Weyl semimetals (WSM) [12,13] and Dirac semimetals (DSM) [12,14,15] defined by their band topology are expected to play a major role in quantum technology. The quantization of the Hall conductance observed in a 2-dimensional electron gas (2DEG) [16] challenged the time honoured Landau paradigm [17] for ordered states of matter classified according to spontaneously broken symmetries [4].…”
Section: Introductionmentioning
confidence: 99%
“…The predicted strain-induced Weyl semimetal phase can be conveniently examined by magnetotransport measurements. Established common transport evidence [7,53,54] of a Weyl state includes the non-trivial Berry phase, which can be obtained from quantum oscillation [53], the planar Hall effect (PHE) [55][56][57], and the negative magnetoresistance (MR) induced by the chiral anomaly [56,[58][59][60]. In topological materials, the non-trivial band topology gives rise to a non-trivial Berry phase, which shifts the phase of quantum oscillations.…”
Section: Discussion: Experimental Examination Of the Weyl State In Stmentioning
confidence: 99%