scholarly journals Fermi Arc Criterion for Surface Majorana Modes in Superconducting Time-Reversal Symmetric Weyl Semimetals

2021 ◽  
Vol 127 (18) ◽  
Author(s):  
Rauf Giwa ◽  
Pavan Hosur
Science ◽  
2019 ◽  
Vol 365 (6459) ◽  
pp. 1286-1291 ◽  
Author(s):  
Noam Morali ◽  
Rajib Batabyal ◽  
Pranab Kumar Nag ◽  
Enke Liu ◽  
Qiunan Xu ◽  
...  

Bulk–surface correspondence in Weyl semimetals ensures the formation of topological “Fermi arc” surface bands whose existence is guaranteed by bulk Weyl nodes. By investigating three distinct surface terminations of the ferromagnetic semimetal Co3Sn2S2, we verify spectroscopically its classification as a time-reversal symmetry-broken Weyl semimetal. We show that the distinct surface potentials imposed by three different terminations modify the Fermi-arc contour and Weyl node connectivity. On the tin (Sn) surface, we identify intra–Brillouin zone Weyl node connectivity of Fermi arcs, whereas on cobalt (Co) termination, the connectivity is across adjacent Brillouin zones. On the sulfur (S) surface, Fermi arcs overlap with nontopological bulk and surface states. We thus resolve both topologically protected and nonprotected electronic properties of a Weyl semimetal.


2021 ◽  
Author(s):  
S M Rafi-Ul-Islam ◽  
Zhuo Bin Siu ◽  
Mansoor Jalil

Abstract We propose a 3D topolectrical (TE) network that can be tuned to realize various higher-order topological gapless and chiral phases. We first study a higher-order Dirac semimetal phase that exhibits a hinge-like Fermi arc linking the Dirac points. This circuit can be extended to host highly tunable first- and second-order Weyl semimetals phases by introducing a non-reciprocal resistive coupling in the x − y plane that breaks time reversal symmetry. The first- and second-order Weyl points are connected by zero-admittance surface and hinge states, respectively. We also study the emergence of first- and second-order chiral modes induced by resistive couplings between similar nodes in the z-direction. These modes respectively occur in the midgap of the surface and hinge admittance bands in our circuit model without the need for any external magnetic field.


2014 ◽  
Vol 90 (4) ◽  
Author(s):  
Pavan Hosur ◽  
Xi Dai ◽  
Zhong Fang ◽  
Xiao-Liang Qi

2018 ◽  
Vol 97 (8) ◽  
Author(s):  
Giacomo Resta ◽  
Shu-Ting Pi ◽  
Xiangang Wan ◽  
Sergey Y. Savrasov

2019 ◽  
Vol 99 (24) ◽  
Author(s):  
Robert C. McKay ◽  
Timothy M. McCormick ◽  
Nandini Trivedi

2017 ◽  
Vol 95 (12) ◽  
Author(s):  
Serguei Tchoumakov ◽  
Marcello Civelli ◽  
Mark O. Goerbig
Keyword(s):  
Type I ◽  
Type Ii ◽  

2016 ◽  
Vol 93 (23) ◽  
Author(s):  
E. V. Gorbar ◽  
V. A. Miransky ◽  
I. A. Shovkovy ◽  
P. O. Sukhachov
Keyword(s):  

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