1999
DOI: 10.1238/physica.regular.060a00418
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Modulational Instabilities in the Dual-Core Nonlinear Optical Fiber

Abstract: We describe modulational instability (MI) of the continuous-wave (cw) states in the dual-core nonlinear optical ¢ber with normal dispersion.We show that the asymmetric cw states (existing above the bifurcation point), as well as the symmetric ones (below the bifurcation point) exhibit MI at all values of the intensity (the instability of the symmetric cw states was known previously).Below the bifurcation, the MI's peak gain (with respect to the perturbation frequency, holding the intensity of the symmetric cw … Show more

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Cited by 42 publications
(25 citation statements)
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“…1 The phenomenon of the spontaneous symmetry breaking in analog with the doublewell potential are realized in a nonlinear dual-core directional fiber. [2][3][4] Spontaneous symmetry breaking was demonstrated recently by Brazhnyi and Malomed in a linear discrete chain (Schrödinger lattice) with two nonlinear sites. 5 They have shown as analytically as well as numerically the existence of symmetric, antisymmetric, and nonsymmetric eigenmodes with eigenfrequencies below the propagation band of the chain, and that a variation of the population of modes can give rise to a bifurcation from one to another mode.…”
Section: Introductionmentioning
confidence: 93%
“…1 The phenomenon of the spontaneous symmetry breaking in analog with the doublewell potential are realized in a nonlinear dual-core directional fiber. [2][3][4] Spontaneous symmetry breaking was demonstrated recently by Brazhnyi and Malomed in a linear discrete chain (Schrödinger lattice) with two nonlinear sites. 5 They have shown as analytically as well as numerically the existence of symmetric, antisymmetric, and nonsymmetric eigenmodes with eigenfrequencies below the propagation band of the chain, and that a variation of the population of modes can give rise to a bifurcation from one to another mode.…”
Section: Introductionmentioning
confidence: 93%
“…We take the light velocity to be equal to unit. However if there are defects with instantaneous Kerr nonlinearity, the displacement electric vector interior to the defects has a nonlinear contribution D( r, t) = ǫ 0 ( r) E( r, t)+χ (3) [ E( r, t)] 2 E( r, t) [25,26]. A substitution of the electric field in the form [ E( r, t) = 1 2 [ E( r)e iωt + E * ( r)e −iωt ] into Eq.…”
Section: Basic Equationsmentioning
confidence: 99%
“…(24) is smaller by a factor of 2 than that obtained by setting  = 0 in Eq. (21). The reason is that the input power for the zero-birefringence fiber ( = 0), as defined by Eq.…”
Section: Zero-birefringence Tcf:  =mentioning
confidence: 99%