2012
DOI: 10.1103/physreva.86.053809
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Breathers inPT-symmetric optical couplers

Abstract: We show that the parity-time (PT ) symmetric coupled optical waveguides with gain and loss support localised oscillatory structures similar to the breathers of the classical φ 4 model. The power carried by the PT -breather oscillates periodically, switching back and forth between the waveguides, so that the gain and loss are compensated on the average. The breathers are found to coexist with solitons and be prevalent in the products of the soliton collisions. We demonstrate that the evolution of the small-ampl… Show more

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Cited by 117 publications
(89 citation statements)
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“…First, we consider a planar PT-symmetric coupler where light experiences diffraction in the x direction and propagates along the z coordinate [77,[82][83][84]. Figure 13(a) shows a schematic presentation of the coupler where the red plane (b)), while blue color indicates loss (white circles, respectively).…”
Section: Solitons In Pt-symmetric Couplersmentioning
confidence: 99%
See 1 more Smart Citation
“…First, we consider a planar PT-symmetric coupler where light experiences diffraction in the x direction and propagates along the z coordinate [77,[82][83][84]. Figure 13(a) shows a schematic presentation of the coupler where the red plane (b)), while blue color indicates loss (white circles, respectively).…”
Section: Solitons In Pt-symmetric Couplersmentioning
confidence: 99%
“…Generalization of the two-channel dispersive coupler [77] to a PT-symmetric arrangement of 2N dispersive waveguides has been done in [66]. The arrays of waveguides in the form of periodic necklaces with alternating and clustered gain and loss distribution [see Fig.…”
Section: Multicore Fibersmentioning
confidence: 99%
“…These include, among others, unconventional beam refraction [13], Bragg scattering [14], symmetry-breaking transitions [4] and associated ghost states [15][16][17][18], a loss-induced optical transparency [5], conical diffraction [19], a new type of Fano resonance [20], chaos [21], nonlocal boundary effects [22], optical switches [23] and diodes [24,25], phase sensitivity of light dynamics [26][27][28], and the possibility of linear and nonlinear wave amplification and filtering [29][30][31]. Unexpected instabilities were also * saadatmand.d@gmail.com † dmitriev.sergey.v@gmail.com ‡ borisovdi@yandex.ru § kevrekid@math.umass.edu identified at the level of PT -symmetric lattices, and nonlinear modes were identified in few-site oligomers, as well as in full lattice settings both in one dimension [32][33][34][35][36][37] and even in two dimensions [38].…”
Section: Introductionmentioning
confidence: 99%
“…It includes the swap of ψ and φ as the P transformation in the direction transverse to x, as in usual P T -symmetric couplers [42][43][44][45][46][47]. Obviously, the system is invariant with respect to the transformation defined by Equation (4).…”
Section: The Coupled Sine-gordon Systemmentioning
confidence: 99%
“…Note that the expansion of Equation (17) for small leads to the same condition, illustrating the consistency of the analysis. The system of coupled NLS Equations (19) and (20) with β = 0 is identical to the above-mentioned model of the P T -symmetric coupler, which may be realized in terms of nonlinear fiber optics, admitting an exact analytical solution for solitons and their stability [42][43][44][45]. The additional terms ∼ β in the coupler model may represent the temporal dispersion of the coupling strength in fiber optics [94,95] (in that case, t and x are replaced, respectively, by the propagation distance and reduced time [13,14]).…”
Section: The Small-amplitude Limit: Coupled Nls Equationsmentioning
confidence: 99%