TY - JOUR
T1 - Resonant nonlinearity management for nonlinear Schrödinger solitons
AU - Sakaguchi, Hidetsugu
AU - Malomed, Boris A.
PY - 2004
Y1 - 2004
N2 - We consider effects of a periodic modulation of the nonlinearity coefficient on fundamental and higher-order solitons in the one-dimensional NLS equation, which is an issue of direct interest to Bose-Einstein condensates in the context of the Feshbach-resonance control, and fiber-optic telecommunications as concerns periodic compensation of the nonlinearity. We find from simulations, and explain by means of a straightforward analysis, that the response of a fundamental soliton to the weak perturbation is resonant, if the modulation frequency [Formula presented] is close to the intrinsic frequency of the soliton. For higher-order [Formula presented]-solitons with [Formula presented] and 3, the response to an extremely weak perturbation is also resonant, if [Formula presented] is close to the corresponding intrinsic frequency. More importantly, a slightly stronger drive splits the 2- or 3-soliton, respectively, into a set of two or three moving fundamental solitons. The dependence of the threshold perturbation amplitude, necessary for the splitting, on [Formula presented] has a resonant character too. Amplitudes and velocities of the emerging fundamental solitons are accurately predicted, using exact and approximate conservation laws of the perturbed NLS equation.
AB - We consider effects of a periodic modulation of the nonlinearity coefficient on fundamental and higher-order solitons in the one-dimensional NLS equation, which is an issue of direct interest to Bose-Einstein condensates in the context of the Feshbach-resonance control, and fiber-optic telecommunications as concerns periodic compensation of the nonlinearity. We find from simulations, and explain by means of a straightforward analysis, that the response of a fundamental soliton to the weak perturbation is resonant, if the modulation frequency [Formula presented] is close to the intrinsic frequency of the soliton. For higher-order [Formula presented]-solitons with [Formula presented] and 3, the response to an extremely weak perturbation is also resonant, if [Formula presented] is close to the corresponding intrinsic frequency. More importantly, a slightly stronger drive splits the 2- or 3-soliton, respectively, into a set of two or three moving fundamental solitons. The dependence of the threshold perturbation amplitude, necessary for the splitting, on [Formula presented] has a resonant character too. Amplitudes and velocities of the emerging fundamental solitons are accurately predicted, using exact and approximate conservation laws of the perturbed NLS equation.
UR - http://www.scopus.com/inward/record.url?scp=85036346220&partnerID=8YFLogxK
U2 - 10.1103/PhysRevE.70.066613
DO - 10.1103/PhysRevE.70.066613
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AN - SCOPUS:85036346220
VL - 70
SP - 7
JO - Physical Review E
JF - Physical Review E
SN - 2470-0045
IS - 6
ER -