(6) with cx = cos k(N ) x = ±1 referring to diﬀerent nodal points

in the vicinity of the spinorbit interaction nodal points tk ≈ t sign(tx)cx(k2 y − k2 x) (5) λ kσ ≈ −2λc x(τ ky + iσk x), ∆ k ≈ ∆ 0 + 2cx(∆ x − ∆ yτ)

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Coexistence of gapless and gapped vortex modes with Majorana corner states in a 2D second-order topological superconductor

cond-mat.supr-con · 2024-11-22 · conditional · novelty 6.0

Zero-energy vortex modes coexist with Majorana corner modes in a 2D second-order topological superconductor only when the normal-state spectrum is gapless with Dirac cones.

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Coexistence of gapless and gapped vortex modes with Majorana corner states in a 2D second-order topological superconductor cond-mat.supr-con · 2024-11-22 · conditional · none · ref 5
Zero-energy vortex modes coexist with Majorana corner modes in a 2D second-order topological superconductor only when the normal-state spectrum is gapless with Dirac cones.

(6) with cx = cos k(N ) x = ±1 referring to diﬀerent nodal points

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