2017
DOI: 10.1007/s10948-017-4095-4
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Majorana States in 2D Topological Superconductor Hosting Abrikosov Vortices

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Cited by 4 publications
(6 citation statements)
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“…In some situations even when the s-wave superconducting pairing gap is nonzero, gapless edge states and zero-energy Majorana modes in vortex cores emerge [4][5][6]. It is possible in some range of parameters, when the system is in the topologically non-trivial phase [7][8][9][10]. Recent experiments performed in Bi 2 Te 3 /NbSe 2 heterostructure seem to confirm this hypothesis [11] by observation of the zero-bias peak in the tunneling differential conductance at the vortex center [12].…”
Section: Introductionmentioning
confidence: 92%
“…In some situations even when the s-wave superconducting pairing gap is nonzero, gapless edge states and zero-energy Majorana modes in vortex cores emerge [4][5][6]. It is possible in some range of parameters, when the system is in the topologically non-trivial phase [7][8][9][10]. Recent experiments performed in Bi 2 Te 3 /NbSe 2 heterostructure seem to confirm this hypothesis [11] by observation of the zero-bias peak in the tunneling differential conductance at the vortex center [12].…”
Section: Introductionmentioning
confidence: 92%
“…First of all, it should be noted that if ∆ ± k are the real functions, then the BdG Hamiltonian (11) can easily be transformed to an off-diagonal view:…”
Section: Topological Invariants and Majorana Fermions In 2d Magnetic ...mentioning
confidence: 99%
“…It is known that the effective time-reversal symmetry can be present in the exact 1D theoretical models similar to (11) even in the presence of the magnetic field (see for example [83,90,99,127,131,132]). Such an additional symmetry leads to the BDI class topological symmetry instead of the D class.…”
Section: Topological Invariants and Majorana Fermions In 2d Magnetic ...mentioning
confidence: 99%
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