2001
DOI: 10.1088/0305-4470/34/16/305
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Floquet theory: exponential perturbative treatment

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Cited by 126 publications
(179 citation statements)
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“…In Section 4, we argue how, nevertheless, the general formalism of MMFT can still lead to valid results, in agreement with prior work [35,[45][46][47][49][50][51]. In Section 5, we derive a generalisation of the Floquet-Magnus expansion [52], which provides a perturbative exponential expansion of the time-evolution operator that has the desired structure. With this, we advocate the possibility to identify effective Hamiltonians that characterise well the effective dynamics of quasi-periodically driven systems in a fast-driving regime and exemplify in Section 6 the results with a quasi-periodically driven Lambda system.…”
Section: Introductionsupporting
confidence: 69%
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“…In Section 4, we argue how, nevertheless, the general formalism of MMFT can still lead to valid results, in agreement with prior work [35,[45][46][47][49][50][51]. In Section 5, we derive a generalisation of the Floquet-Magnus expansion [52], which provides a perturbative exponential expansion of the time-evolution operator that has the desired structure. With this, we advocate the possibility to identify effective Hamiltonians that characterise well the effective dynamics of quasi-periodically driven systems in a fast-driving regime and exemplify in Section 6 the results with a quasi-periodically driven Lambda system.…”
Section: Introductionsupporting
confidence: 69%
“…In practice, this is often done through an expansion in terms of powers of |ω| −1 . In this section, we will derive a generalisation of the Floquet-Magnus expansion [52,58,59] to quasi-periodic systems and provide a perturbative exponential expansion of the time-evolution operator with the desired Floquet representation. This will allow us to identify H Q as the effective Hamiltonian that captures the dynamics of the system in a suitable fast-driving regime.…”
Section: Generalised Floquet-magnus Expansionmentioning
confidence: 99%
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“…In the case of a linearly polarized pump, the latter introduces additional anisotropy in the system via renormalization of the parameters of the effective SOI Hamiltonian. In the high-frequency regime the formal derivation of the effective time-independent Hamiltonian can be performed in a rather intuitive way, and the rigorous mathematical procedure is based on either Floquet-Magnus expansion 39,40 or the BrillouinWigner perturbation theory 41 : If this is the case, Floquet bands are nearly uncoupled, while the corresponding Floquet Hamiltonian becomes almost block diagonal, which results in a very weak dependence on time of the effective Floquet operator. We solve directly the evolution equation that governs the dynamics of RashbaDresselhaus spin-orbit-coupled electron gas under an intense linearly polarized field.…”
Section: Hybrid Surface Waves Under Intense Pumpingmentioning
confidence: 99%
“…The Floquet Magnus expansion is a new theoretical tool for describing spin dynamics recently introduced in solid-state NMR and spin physics [34]- [36]. This unique approach (FME) is an extension of the popular Magnus expansion and average Hamiltonian theory and is useful to shed new lights on AHT and FLT [27] [28].…”
Section: Floquet-magnus Expansionmentioning
confidence: 99%