2017
DOI: 10.1088/1367-2630/aa50d5
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Weyl-Majorana solenoid

Abstract: A Weyl semimetal wire with an axial magnetization has metallic surface states (Fermi arcs) winding along its perimeter, connecting bulk Weyl cones of opposite topological charge (Berry curvature). We investigate what happens to this 'Weyl solenoid' if the wire is covered with a superconductor, by determining the dispersion relation of the surface modes propagating along the wire. Coupling to the superconductor breaks up the Fermi arc into a pair of Majorana modes, separated by an energy gap. Upon variation of … Show more

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Cited by 25 publications
(23 citation statements)
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“…As they pass through the center of the Brillouin zone, the chirality blockade is no longer operative and the Fermi arcs acquire a mixed electron-hole character. At k z = 0, the surface states are charge neutral Majorana fermions [24].…”
Section: Fermi-arc Mediated Josephson Effectmentioning
confidence: 99%
“…As they pass through the center of the Brillouin zone, the chirality blockade is no longer operative and the Fermi arcs acquire a mixed electron-hole character. At k z = 0, the surface states are charge neutral Majorana fermions [24].…”
Section: Fermi-arc Mediated Josephson Effectmentioning
confidence: 99%
“…1c) and unusual electromagnetic wave transmission [20][21][22][23] (Fig. 1d), and the emergence of Majorana modes when coupled with superconductivity 24 . Therefore, the capability of controlling and modifying the SFAs, especially the switching of SFAs between Weyl-points pairs (see Fig.…”
Section: Introductionmentioning
confidence: 97%
“…1 and addressing the question "What is the charge transported along the vortices in a chiral Landau level?" It is known [10] that the charge of Weyl fermions in a superconductor (pair potential ∆ 0 ) is reduced by a factor κ = K(∆ 0 )/K(0). We find a direct manifestation of this charge renormalization in the electrical conductance, which is quantized at 1 2 (eκ) 2 /h per vortex.…”
Section: Introductionmentioning
confidence: 99%