Therefore, the gap size ∆s scales inversely with L in the pristine limit, which is qualitatively consistent with the power-law fit in the upper right inset of Fig

Near the TQPT, the gap size ∆ s is governed by the band edge at k = 0 in the continuum limit, giving ∆s = E1(k = 0) = VZ − p µ2 + ∆2

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cond-mat.mes-hall · 2025-06-30 · unverdicted · novelty 5.0

Exponential protection of Majorana zero modes in finite disordered nanowires holds only for disorder much smaller than the superconducting gap.

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Majorana zero modes in semiconductor-superconductor hybrid structures: Defining topology in short and disordered nanowires through Majorana splitting cond-mat.mes-hall · 2025-06-30 · unverdicted · none · ref 1
Exponential protection of Majorana zero modes in finite disordered nanowires holds only for disorder much smaller than the superconducting gap.