2018
DOI: 10.1088/1361-6544/aae031
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General soliton solution to a nonlocal nonlinear Schrödinger equation with zero and nonzero boundary conditions

Abstract: General soliton solutions to a nonlocal nonlinear Schrödinger (NLS) equation with PT-symmetry for both zero and nonzero boundary conditions are considered via the combination of Hirota's bilinear method and the Kadomtsev-Petviashvili (KP) hierarchy reduction method. First, general N-soliton solutions with zero boundary conditions are constructed. Starting from the tau functions of the two-component KP hierarchy, it is shown that they can be expressed in terms of either Gramian or double Wronskian determinants.… Show more

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Cited by 163 publications
(74 citation statements)
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“…By checking qualitative features of the evolution, we note that further decrease of ∆x and/or ∆t did not produce any conspicuous effect. The VAs (5), (7), and (14) are also integrated using the fourth-order Runge-Kutta method. The varying-in-time variables are then inserted back into the ansatz to obtain the spatial profile of the VA. 7…”
Section: Variational Methods For Soliton Collisionsmentioning
confidence: 99%
See 1 more Smart Citation
“…By checking qualitative features of the evolution, we note that further decrease of ∆x and/or ∆t did not produce any conspicuous effect. The VAs (5), (7), and (14) are also integrated using the fourth-order Runge-Kutta method. The varying-in-time variables are then inserted back into the ansatz to obtain the spatial profile of the VA. 7…”
Section: Variational Methods For Soliton Collisionsmentioning
confidence: 99%
“…Various soliton solutions of the nonlocal NLS equation (1) have been obtained, exploiting the integrability of the equations, such as dark and antidark solitons [13,14], standing waves in terms of elliptic functions [15], and rational solutions both in the focusing and defocusing nonlinearity [16,17]. Note, however, that the study of soliton dynamics, especially interactions between solitons, has been done only using Darboux transformation [13,16,18,19] or via a combination of Hirota's bilinear method and the Kadomtsev-Petviashvili (KP) hierarchy [14], which are limited to specific combinations of parameter values and initial conditions. A general study of interactions of many bright, dark and antidark solitons has been presented recently, where again the same transformation method was used [20].…”
Section: Introductionmentioning
confidence: 99%
“…5.2 q(x, y, t) = kp(ε 1 x, ε 2 y, ε 3 t), ε 2 1 = ε 2 2 = ε 2 3 = 1, k is a real constant When we apply this reduction to the AKNS(-3) system (11) and (12), it reduces consistently to the nonlocal complex AKNS(-3) equation,…”
Section: Q(x Y T) = Kp(x Y T) K Is a Real Constantmentioning
confidence: 99%
“…Let us take ε = 1. Hence one-soliton solutions of the AKNS(-3) system given by (11) and (12) and the AKNS(-4) system given by (18) and (19)…”
Section: Introductionmentioning
confidence: 99%
“…Following the introduction of this equation, its properties have been extensively investigated [6,[8][9][10][11][12][13][14][15][16][17][18][19]. In addition, other nonlocal integrable equations have been reported [20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35][36][37][38].…”
Section: Introductionmentioning
confidence: 99%