Effective Floquet Hamiltonian in the low-frequency regime

dc.creatorVogl, Michael
dc.creatorRodriguez-Vega, Martin
dc.creatorFiete, Gregory A.
dc.date.accessioned2024-01-18T14:55:19Z
dc.date.available2024-01-18T14:55:19Z
dc.date.issued2020-01-09
dc.description.abstractWe develop a theory to derive effective Floquet Hamiltonians in the weak drive and low-frequency regime. We construct the theory in analogy with band theory for electrons in a spatially-periodic and weak potential, such as occurs in some crystalline materials. As a prototypical example, we apply this theory to graphene driven by circularly polarized light of low intensity. We find an ana- lytic expression for the effective Floquet Hamiltonian in the low-frequency regime which accurately predicts the quasienergy spectrum and the Floquet states. Furthermore, we identify self-consistency as the crucial feature effective Hamiltonians in this regime need to satisfy to achieve high accuracy. The method is useful in providing a realistic description of off-resonant drives for multi-band solid state systems where light-induced topological band structure changes are sought.
dc.description.departmentCenter for Dynamics and Control of Materials
dc.description.sponsorshipThis work was supported by the NSF Ma- terials Research Science and Engineering Center Grant No. DMR-1720595.
dc.identifier.doi10.1103/PhysRevB.101.024303
dc.identifier.urihttps://hdl.handle.net/2152/123438
dc.identifier.urihttps://doi.org/10.26153/tsw/50234
dc.language.isoen_US
dc.relation.ispartofCenter for Dynamics and Control of Materials Publications
dc.rights.restrictionOpen
dc.subjectFloquet Hamiltonian
dc.titleEffective Floquet Hamiltonian in the low-frequency regime
dc.typeArticle

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