2008
DOI: 10.1016/j.jmaa.2008.05.101
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Separation of internal and interaction dynamics for NLS-described wave packets with different carrier waves

Abstract: We give a detailed analysis of the interaction of two NLS-described wave packets with different carrier waves for a nonlinear wave equation. By separating the internal dynamics of each wave packet from the dynamics caused by the interaction we prove that there is almost no interaction of such wave packets. We also prove the validity of a formula for the envelope shift caused by the interaction of the wave packets.

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Cited by 10 publications
(2 citation statements)
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“…While the previous ansatz contains no internal microsctructure, in [SUW09] the interaction of two (weakly) amplitude modulated pulses of different group velocities c 1 = c 2 and time-independent amplitudes is considered in the chain (1.3) under the dispersive scalings τ = ε 2 t y = ε(γ − c 1,2 t), and it is proved that after interaction the amplitudes retain their shape but experience a shift of order O(ε) in position; see also [BF06]. Analogous results are obtained in [CBea07,CBea08] on a continuous one-dimensional string.…”
Section: Introductionmentioning
confidence: 60%
“…While the previous ansatz contains no internal microsctructure, in [SUW09] the interaction of two (weakly) amplitude modulated pulses of different group velocities c 1 = c 2 and time-independent amplitudes is considered in the chain (1.3) under the dispersive scalings τ = ε 2 t y = ε(γ − c 1,2 t), and it is proved that after interaction the amplitudes retain their shape but experience a shift of order O(ε) in position; see also [BF06]. Analogous results are obtained in [CBea07,CBea08] on a continuous one-dimensional string.…”
Section: Introductionmentioning
confidence: 60%
“…Using the BT, one can construct, for instance, a 2-breather describing the elastic collision of two individual breathers. Such an interaction for small amplitude wave packets in the general KG setting (21) has striking similarities to the breather interaction: to leading order, the shape of the wave packets remains unchanged after collision, the only interaction effects being a shift of envelope and carrier waves (see [40] for KG with constant coefficients and [41] for KG with spatially periodic coefficients). In the case of large amplitudes, however, the situation is far more complex, as is attested also by the complexity of interactions of simpler structures such as kinks in non-integrable KG models [13][14][15][16][17][18].…”
Section: A Continuum Limit: Genuine Breathers and Modulating Pulsesmentioning
confidence: 97%