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The surface states of Weyl semi-metals (SM's) consist of disjointed Fermi-arcs.
X. Wan, A. M. Turner, A. Vishwanath, and S. Y. Savrasov, Topological semimetal and Fermi-arc surface states in the electronic structure of pyrochlore iridates
2011
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Gang Xu, Hongming Weng, Zhijun Wang, Xi Dai, Zhong Fang, Chern semi-metal and Quantized Anomalous Hall Effect in HgCr2Se4
2011
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A.A. Burkov, Leon Balents. Weyl Semimetal in a Topological Insulator Multilayer
2011
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S. M. Young, S. Zaheer, J.C.Y. Teo, C.L. Kane, E.J. Mele, and A.M. Rappe, Dirac Semimetal in Three Dimensions
2012
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Z. Wang, Y. Sun, X.-Q. Chen, C. Franchini, G. Xu, H. Weng, X. Dai, and Z. Fang, Dirac semimetal and topological phase transitions in A 3 Bi (A=Na, K, Rb)
2012
Cited alongside, same era.
Gang Chen, Michael Hermele, Magnetic orders and topological phases from f-d exchange in pyrochlore iridates
2012
Cited alongside, same era.
F. F. Tafti, J. J. Ishikawa, A. McCollam, S. Nakatsuji, S. R. Julian. Pressure Tuned Insulator to Metal Transition in Eu 2 Ir 2 O 7
2012
Cited alongside, same era.
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See Supplementary materials for more details about the surface state and Landau-Level structure of Weyl and Dirac SMs and diabatic corrections to semiclassical motion along the Fermi-arc
Cited in the paper.
Alternative processes in which electrons transfer to non-chiral bulk LLs are not expected to play an important role in forming closed magnetic orbits since the non-chiral states 1) have finite energy gap E n ( k y ) = ± v ⟂ 2 v z v ⟂ ( e B n ) 2 + k y 2 E_{n}(k_{y})=\pm v_{\perp}\sqrt{2\frac{v_{z}}{v_{\perp}}\left(eBn\right)^{2}+k_{y}^{2}} , where ( | n | > 0 ) (|n|>0) [ 16 ] , and 2) propagate massively rather than ballistically. This expectation is confirmed by the good agreement of semiclassical predictions with direct numerical simulations
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This truncation breaks the canonical commutation relations of a a and a † a^{\dagger} for states near the cutoff, N max N_{\text{max}} . This can create spurious low-energy solutions, that have large weight on N max N_{\text{max}} but very low energy. These are removed by adding a regulator term that energetically penalizes | N max ⟩ |N_{\text{max}}\rangle
Cited in the paper.
W. Witczak-Krempa, and Y.B. Kim Topological and magnetic phases of interacting electrons in the pyrochlore iridates
2012
Later among the works it cites.
Z. Wang, H. Weng, Q. Wu, X. Dai, and Z. Fang, Three-dimensional Dirac semimetal and quantum transport in Cd 3 As 2
2013
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2014
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