Gapless Floquet topology

Fuente: arXiv
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Main Authors: Cardoso, Gabriel, Yeh, Hsiu-Chung, Korneev, Leonid, Abanov, Alexander G., Mitra, Aditi
Format: Preprint
Published: 2024
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author Cardoso, Gabriel
Yeh, Hsiu-Chung
Korneev, Leonid
Abanov, Alexander G.
Mitra, Aditi
author_facet Cardoso, Gabriel
Yeh, Hsiu-Chung
Korneev, Leonid
Abanov, Alexander G.
Mitra, Aditi
contents Symmetry-protected topological (SPT) phases in insulators and superconductors are known for their robust edge modes, linked to bulk invariants through the bulk-boundary correspondence. While this principle traditionally applies to gapped phases, recent advances have extended it to gapless systems, where topological edge states persist even in the absence of a bulk gap. We extend this framework to periodically driven chains with chiral symmetry, revealing the existence of topological edge zero- and pi-modes despite the lack of bulk gaps in the quasienergy spectrum. By examining the half-period decomposition of chiral evolutions, we construct topological invariants that circumvent the need to define the Floquet Hamiltonian, making them more suitable for generalization to the gapless regime. We provide explicit examples, including generalizations of the Kitaev chain and related spin models, where localized pi-modes emerge even when the bulk is gapless at the same quasi-energy as the edge modes. We numerically study the effect of interactions, which give a finite lifetime to the edge modes in the thermodynamic limit with the decay rate consistent with Fermi's Golden Rule.
format Preprint
id arxiv_https___arxiv_org_abs_2411_02526
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Gapless Floquet topology
Cardoso, Gabriel
Yeh, Hsiu-Chung
Korneev, Leonid
Abanov, Alexander G.
Mitra, Aditi
Strongly Correlated Electrons
Mesoscale and Nanoscale Physics
Statistical Mechanics
Quantum Physics
Symmetry-protected topological (SPT) phases in insulators and superconductors are known for their robust edge modes, linked to bulk invariants through the bulk-boundary correspondence. While this principle traditionally applies to gapped phases, recent advances have extended it to gapless systems, where topological edge states persist even in the absence of a bulk gap. We extend this framework to periodically driven chains with chiral symmetry, revealing the existence of topological edge zero- and pi-modes despite the lack of bulk gaps in the quasienergy spectrum. By examining the half-period decomposition of chiral evolutions, we construct topological invariants that circumvent the need to define the Floquet Hamiltonian, making them more suitable for generalization to the gapless regime. We provide explicit examples, including generalizations of the Kitaev chain and related spin models, where localized pi-modes emerge even when the bulk is gapless at the same quasi-energy as the edge modes. We numerically study the effect of interactions, which give a finite lifetime to the edge modes in the thermodynamic limit with the decay rate consistent with Fermi's Golden Rule.
title Gapless Floquet topology
topic Strongly Correlated Electrons
Mesoscale and Nanoscale Physics
Statistical Mechanics
Quantum Physics
url https://arxiv.org/abs/2411.02526