2003
DOI: 10.1016/s0167-2789(02)00691-7
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Dynamics of counterpropagating waves in parametrically driven systems: dispersion vs. advection

Abstract: The dynamics of parametrically driven counterpropagating waves in a one-dimensional extended nearly conservative annular system are described by two coupled, damped, parametrically driven nonlinear Schrödinger (NLS) equations with opposite transport terms due to the group velocity, and small dispersion. The system is characterized by two length scales defined by a balance between (a) forcing and dispersion (the dispersive scale), and (b) forcing and advection at the group velocity (the transport scale). Both a… Show more

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Cited by 17 publications
(15 citation statements)
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“…The boundary condition (4.13) must be imposed because since we are including dispersión, (4.5) is second order in £. As explained by Martel et al (2003) (see also Martel & Vega 1996), the appropriate additional boundary condition is the compatibility condition for the hyperbolic equations obtained when dispersión is ignored, which in our case is precisely (4.13). Equation (4.14a) at £ = +L imposes no net mass flux across the lateral sidewalls.…”
Section: Harmonic Surface Waves At Large Aspect Ratio: L > Dmentioning
confidence: 97%
See 1 more Smart Citation
“…The boundary condition (4.13) must be imposed because since we are including dispersión, (4.5) is second order in £. As explained by Martel et al (2003) (see also Martel & Vega 1996), the appropriate additional boundary condition is the compatibility condition for the hyperbolic equations obtained when dispersión is ignored, which in our case is precisely (4.13). Equation (4.14a) at £ = +L imposes no net mass flux across the lateral sidewalls.…”
Section: Harmonic Surface Waves At Large Aspect Ratio: L > Dmentioning
confidence: 97%
“…If dispersión is neglected, then the equations become hyperbolic, as in related dissipative systems (first considered by Daniels 1978, see also Martel & Vega 1998), where small diffusive terms lead to subtle effects (Martel & Vega 1996). Similarly, dispersión cannot be ignored a priori in counterpropagating surface waves (Lapuerta, Martel & Vega 2002;Martel, Vega & Knobloch 2003) because dispersive scales can be destabilized. There are two kinds of surface waves, namely harmonic and subharmonic, whose frequency is the forcing frequency and half of the forcing frequency, respectively.…”
Section: Introductionmentioning
confidence: 99%
“…In this section we will complete these results and give a detailed description of the CW instability regions given by (19).…”
Section: Cw Stability: Transport Scale Perturbationsmentioning
confidence: 99%
“…It is also important to emphasize that this type of dynamics is not contained in the standard dispersion-less NLCME formulation for light propagation in FBG. Moreover, this behavior is just the result of the competition of two effects with different asymptotic order: transport and disper- sion, and this is a generic situation that applies to any propagative extended system unless some special care is taken to reduce the group velocity (similar effects have been previously described in the context of Hopf bifurcation in dissipative systems [13] and in parametrically forced surface waves [14]). …”
Section: )mentioning
confidence: 70%