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Panel (a) shows the autocorrelation func- tion

TDVP vs Lanczos wt 0 5 1 0 15 2 0 C饾浗(t) 0 · 2000

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Almost Strong Zero Modes at Finite Temperature

cond-mat.str-el 路 2025-01-19 路 conditional 路 novelty 6.0

For the Kitaev-Hubbard chain, the finite-temperature decay rate of the Majorana edge mode follows an Arrhenius law with an effective gap systematically larger than the many-body gap.

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  • Almost Strong Zero Modes at Finite Temperature cond-mat.str-el 路 2025-01-19 路 conditional 路 none 路 ref 5

    For the Kitaev-Hubbard chain, the finite-temperature decay rate of the Majorana edge mode follows an Arrhenius law with an effective gap systematically larger than the many-body gap.