2013
DOI: 10.1088/1742-6596/435/1/012024
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Variational analysis of soliton scattering by external potentials

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Cited by 13 publications
(16 citation statements)
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“…which is written in the stationary frame of the soliton, with stationary coordinates (x, t). To accurately describe the perturbation dynamics, we choose a general variational ansatz of the form [71,83] ψ (x, t) ≡ a sech (…”
Section: B Variational Equationsmentioning
confidence: 99%
“…which is written in the stationary frame of the soliton, with stationary coordinates (x, t). To accurately describe the perturbation dynamics, we choose a general variational ansatz of the form [71,83] ψ (x, t) ≡ a sech (…”
Section: B Variational Equationsmentioning
confidence: 99%
“…The Equation () can be derived from the following Lagrangian density: scriptL=i2()ψψ˙*ψ*trueψ˙+12ψ2V0sech2()xitalicutψ2g2ψ4, through the Euler–Lagrange equation: scriptLψ*t()Ltrueψ˙*x()Lψ*=0. The choice of the ansatz shape is very important [29]. In our case, a natural choice is the hyperbolic secant function [33] because at the linear limit of the 1D‐GPE it is possible to obtain the ground state solution of the one‐dimensional Schrödinger equation for the PT potential. Another plausible reason for choosing this ansatz is the fact that the hyperbolic secant function is an exact soliton solution (nonlinear solution) of the one‐dimensional nonlinear Schrödinger equation.…”
Section: Methodsmentioning
confidence: 99%
“…Now, in order to obtain the equations that govern the dynamic behavior of the variational parameters, we insert Equation () into Equation () and calculate the effective Lagrangian L by the average Lagrangian density: L=〈〉L=+scriptLitalicdx. Therefore, after integrating Lagrangian density over the spatial coordinate, we obtain the following effective Lagrangian: L=N[]π212w2truec˙+π26w2c2trueξ˙22+trueδ˙+16w2gN6wV02w+sech2()xitalicutsech2()xξwitalicdx. The evolution equations for variational parameters can be obtained from the Euler–Lagrange equation: ddt()Lq˙Lq=0, where q are the generalized coordinates, q ≡ { δ , c , ξ , w }, related to variational parameters. The equation for the phase δ reduces to dN / dt = 0 and illustrates the conservation of the norm of the wave function or number of atoms in the BEC [33]. The other equations yield a set of coupled nonlinear integral equations: truew˙=2italiccw trueξ¨=V0w2+sech2()xitalicuttanh()xξw…”
Section: Methodsmentioning
confidence: 99%
“…This method provides a set of ordinary differential equations describing the dynamics of system approximately. It can be used in BEC studies with several external potentials including harmonic potentials, optical lattice (OL) or time modulated potentials [4][5][6][7][8][9][10][11][12][13][14][15][16][17]. It is well known that the collapse of condensate occurs when the atom number exists a critical value in the attractive nonlinearity regime.…”
Section: Introductionmentioning
confidence: 99%
“…Modulational instability analysis has been done for one-dimensional OL by taking higher order interactions into account [11]. Matter wave solutions like bright and dark solitons have been also investigated by the variational method [12][13][14][15]. Dynamics in disordered or random potentials is another topic of interest.…”
Section: Introductionmentioning
confidence: 99%