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.
Boundary Strong Zero Modes
1 Pith paper cite this work. Polarity classification is still indexing.
abstract
Strong zero modes are edge-localized degrees of freedom capable of storing information at infinite temperature, even in systems with no disorder. To date, their stability has only been systematically explored at the physical edge of a system. Here, we extend the notion of strong zero modes to the boundary between two systems, and present a unifying framework for the stability of these boundary strong zero modes. Unlike zero-temperature topological edge modes, which are guaranteed to exist at the interface between a trivial and topological phase, the robustness of boundary strong zero modes is significantly more subtle. This subtlety is perhaps best illustrated by the following dichotomy: we find that the interface between a trivial and ordered phase does not guarantee the existence of a strong zero mode, while the interface between two ordered phases can, in certain cases, lead to an exact strong zero mode.
citation-role summary
citation-polarity summary
fields
cond-mat.str-el 1years
2025 1verdicts
CONDITIONAL 1roles
background 1polarities
unclear 1representative citing papers
citing papers explorer
-
Almost Strong Zero Modes at Finite Temperature
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.