Geometric Floquet Theory

We derive Floquet theory from quantum geometry. We identify quasienergy folding as a consequence of a broken gauge group of the adiabatic gauge potential U(1)↦Z. Fixing instead the gauge freedom using the parallel-transport gauge uniquely decomposes Floquet dynamics into a purely geometric and a pur...

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Main Authors: Paul M. Schindler, Marin Bukov
Format: Article
Language:English
Published: American Physical Society 2025-08-01
Series:Physical Review X
Online Access:http://doi.org/10.1103/7l91-gw77
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author Paul M. Schindler
Marin Bukov
author_facet Paul M. Schindler
Marin Bukov
author_sort Paul M. Schindler
collection DOAJ
description We derive Floquet theory from quantum geometry. We identify quasienergy folding as a consequence of a broken gauge group of the adiabatic gauge potential U(1)↦Z. Fixing instead the gauge freedom using the parallel-transport gauge uniquely decomposes Floquet dynamics into a purely geometric and a purely dynamical evolution. The dynamical average-energy operator provides an unambiguous sorting of the quasienergy spectrum, identifying a Floquet ground state and suggesting a way to define the filling of Floquet-Bloch bands. We exemplify the features of geometric Floquet theory using an exactly solvable XY model and a nonintegrable kicked Ising chain. We elucidate the geometric origin of inherently nonequilibrium effects, like the π-quasienergy splitting in discrete time crystals or π-edge modes in anomalous Floquet topological insulators. The spectrum of the average-energy operator is a susceptible indicator for both heating and spatiotemporal symmetry-breaking transitions. Last, we demonstrate that the periodic lab-frame Hamiltonian generates transitionless counterdiabatic driving for Floquet eigenstates. This work directly bridges seemingly unrelated areas of nonequilibrium physics.
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spelling doaj-art-593414e5ca7a43aaadfdb4497d41504a2025-08-20T03:39:21ZengAmerican Physical SocietyPhysical Review X2160-33082025-08-0115303103710.1103/7l91-gw77Geometric Floquet TheoryPaul M. SchindlerMarin BukovWe derive Floquet theory from quantum geometry. We identify quasienergy folding as a consequence of a broken gauge group of the adiabatic gauge potential U(1)↦Z. Fixing instead the gauge freedom using the parallel-transport gauge uniquely decomposes Floquet dynamics into a purely geometric and a purely dynamical evolution. The dynamical average-energy operator provides an unambiguous sorting of the quasienergy spectrum, identifying a Floquet ground state and suggesting a way to define the filling of Floquet-Bloch bands. We exemplify the features of geometric Floquet theory using an exactly solvable XY model and a nonintegrable kicked Ising chain. We elucidate the geometric origin of inherently nonequilibrium effects, like the π-quasienergy splitting in discrete time crystals or π-edge modes in anomalous Floquet topological insulators. The spectrum of the average-energy operator is a susceptible indicator for both heating and spatiotemporal symmetry-breaking transitions. Last, we demonstrate that the periodic lab-frame Hamiltonian generates transitionless counterdiabatic driving for Floquet eigenstates. This work directly bridges seemingly unrelated areas of nonequilibrium physics.http://doi.org/10.1103/7l91-gw77
spellingShingle Paul M. Schindler
Marin Bukov
Geometric Floquet Theory
Physical Review X
title Geometric Floquet Theory
title_full Geometric Floquet Theory
title_fullStr Geometric Floquet Theory
title_full_unstemmed Geometric Floquet Theory
title_short Geometric Floquet Theory
title_sort geometric floquet theory
url http://doi.org/10.1103/7l91-gw77
work_keys_str_mv AT paulmschindler geometricfloquettheory
AT marinbukov geometricfloquettheory