Weyl electrons kiss
By L. Balents. 2011
189 citations recorded by the source corpus.
Subfields: Atomic and Molecular Physics, and Optics, Materials Chemistry
View Paper: https://www.semanticscholar.org/paper/6a63040370517aa4c9cca82263caba153ee3255a
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In Atomic and Molecular Physics, and Optics
In Materials Chemistry
Citations in the corpus
- Weyl and Dirac semimetals in three-dimensional solids (2017, methodology): “…across the Weyl or Dirac node when the chemical potential (EF ) is at the Weyl or Dirac point is σ1(ω) = N e2 12h |ω| vF (40) where vF is the Fermi velocity and N is number of nodes (Burkov and Balents, 2011; Hosur et al., 2012; Hosur and Qi, 2013; Tabert et al., 2016; Wan et al., 2011).”
- Experimental discovery of Weyl semimetal TaAs (2015, background): “Since a Dirac node is composed of two “kissing”Weyl nodes with opposite chirality [3,4], it serves as both a Fermi arc “source” and “sink” at the same time.”
- Weyl Semimetal Phase in Noncentrosymmetric Transition-Metal Monophosphides (2014, unknown): “011029-6”
- Observation of Weyl nodes in TaAs (2015, background): “xistence of Weyl fermionic quasiparticles in TaAs. The massless Dirac equation in the three-dimensional (3D) momentum space can be regarded as the overlap of two Weyl fermions with opposite chirality [1, 2]. The Dirac fermionic quasiparticle is stable under the protection of some crystal symmetry in”