2014
DOI: 10.1016/j.optcom.2014.03.040
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Spatiotemporal coupled-mode theory in dispersive media under a dynamic modulation

Abstract: A simple and general formalism for mode coupling by a spatial, temporal or spatiotemporal perturbation in dispersive materials is developed. This formalism can be used for studying various linear and non-linear optical interactions involving a dynamic modulation of the interaction parameters such as non-reciprocal phenomena, time reversal of signals and spatiotemporal quasi phase matching.

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Cited by 12 publications
(19 citation statements)
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References 17 publications
(26 reference statements)
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“…The second argument of ε(ω,a) denotes the implicit dependence of ε on the modal amplitudes a μ through the inversion D. The effective permittivity (9) can be decomposed into a steady-state-amplitude dispersive term and a nonlinear nondispersive term (similar in spirit to [75]). The key point here is that, to lowest order, there are two corrections to the permittivity in the presence of noise: the dispersive correction due to any shift in frequency at the unperturbed amplitudes a μ0 and the nonlinear correction due to any shift in amplitude at the unperturbed frequency.…”
Section: The N-salt Tcmt Equationsmentioning
confidence: 99%
“…The second argument of ε(ω,a) denotes the implicit dependence of ε on the modal amplitudes a μ through the inversion D. The effective permittivity (9) can be decomposed into a steady-state-amplitude dispersive term and a nonlinear nondispersive term (similar in spirit to [75]). The key point here is that, to lowest order, there are two corrections to the permittivity in the presence of noise: the dispersive correction due to any shift in frequency at the unperturbed amplitudes a μ0 and the nonlinear correction due to any shift in amplitude at the unperturbed frequency.…”
Section: The N-salt Tcmt Equationsmentioning
confidence: 99%
“…Our derivation extends the work by the Bahabad group [81] by exactly accounting for the effect of structural dispersion, and allowing for more general perturbations, specifically, perturbations consisting of pulses rather than a discrete set of higher harmonics. Conveniently, our formalism requires only minimal modifications to that of [81], but is more accurate and far more general. Our approach also extends the standard models of nonlinear wave propagation and mixing (e.g., [11,108]) which typically involve only one mode in each frequency, to account for mode coupling.…”
Section: Discussionmentioning
confidence: 88%
“…When the system includes pulses centered at well-separated frequencies (as e.g., in [81]), then, one needs to replace ω 0 by ω p and sum over the modes p, see below [118]. Now, using the ansatz (9a) and Eqs.…”
Section: B Derivationmentioning
confidence: 99%
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