Phase transition between the quantum spin Hall and insulator phases in 3D: emergence of a topological gapless phase
By Shuichi Murakami. 2007
978 citations recorded by the source corpus.
The discussion on page 9 of the published article, including figures 3 and 4, needs to be corrected. Please see the PDF for details.
Subfields: Atomic and Molecular Physics, and Optics, Materials Chemistry
View Paper: https://www.semanticscholar.org/paper/b81c9fa01a8367c217582bd0fd5c78a8da6f8b44
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In Atomic and Molecular Physics, and Optics
In Materials Chemistry
Citations in the corpus
- Discovery of a Weyl fermion semimetal and topological Fermi arcs (2015, background): “Recently, it was understood that a Weyl fermion can emerge as a quasiparticle in certain crystals, Weyl fermion semimetals (1-22).”
- Reciprocal skin effect and its realization in a topolectrical circuit (2019, methodology): “To conceptualize this, consider an analogy to the 2D Chern insulator and the 3D Weyl semimetal [42].”
- Recent developments in transport phenomena in Weyl semimetals (2013, background): “Therefore, it is possible to fine tune Bi1−xSbx to the critical point separating the two phases (Fu and Kane [10], Murakami [25], Hsieh et al. [19]).”
- Experimental discovery of Weyl semimetal TaAs (2015, background): “Separated Weyl nodes are topologically stable [19,20] because any perturbation respecting the translational symmetry can shift but not annihilate them [21,22].”
- Weyl and Dirac semimetals in three-dimensional solids (2017, background): “Since the net topological charge enclosed within Brillouin is zero, this latter situation further requires the existence of two additional compensating partner Weyl nodes (Halász and Balents, 2012; Murakami, 2007).”