首页> 外文期刊>Modern Physics Letters, B. Condensed Matter Physics, Statistical Physics, Applied Physics >Nonautonomous solitons in terms of the double Wronskian determinant for a variable-coefficient Gross-Pitaevskii equation in the Bose-Einstein condensate
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Nonautonomous solitons in terms of the double Wronskian determinant for a variable-coefficient Gross-Pitaevskii equation in the Bose-Einstein condensate

机译:Bose-Einstein凝聚体中变系数Gross-Pitaevskii方程的双Wronskian行列式表示的非自治孤子

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Under investigation in this paper is a variable-coefficient Gross-Pitaevskii equation which describes the Bose-Einstein condensate. Lax pair, bilinear forms and bilinear Backlund transformation for the equation under some integrable conditions are derived. Based on the Lax pair and bilinear forms, double Wronskian solutions are constructed and verified. The Nth-order nonautonomous solitons in terms of the double Wronskian determinant are given. Propagation and interaction for the first- and second-order nonautonomous solitons are discussed from three cases. Amplitudes of the first- and second-order nonautonomous solitons are affected by a real parameter related to the variable coefficients, but independent of the gain-or-loss coefficient m(0)(t) and linear external potential coefficient m(1)(t). For Case 1 left perpendicularm(0)(t) = 0right perpendicular, m(1)(t) leads to the accelerated propagation of nonautonomous solitons. Parabolic-, cubic-, exponential-and cosine-type nonautonomous solitons are exhibited due to the different choices of m(1)(t). For Case 2 [m(1)(t) = 0], if the real part of the spectral parameter equals 0, stationary soliton can be formed. If we take the harmonic external potential coefficient m(2)(t) as a positive constant and let the real parts of the two spectral parameters be the same, bound-state-like structures can be formed, but there are only one attractive and two repulsive procedures. For Case 3 [m(0)(t) and m(1)(t) are taken as nonzero constants], head-on interaction, overtaking interaction and bound-state structure can be formed based on the signs of the two spectral parameters.
机译:本文正在研究的是一个可变系数的Gross-Pitaevskii方程,它描述了Bose-Einstein冷凝物。推导了方程在某些可积分条件下的松弛对,双线性形式和双线性Backlund变换。基于Lax对和双线性形式,构造并验证了双Wronskian解。给出了双Wronskian行列式形式的N阶非自治孤子。从三种情况讨论了一阶和二阶非自治孤子的传播和相互作用。一阶和二阶非自治孤子的幅度受与可变系数相关的实参数的影响,但与损益系数m(0)(t)和线性外部电势系数m(1)( t)。对于情况1左垂直m(0)(t)= 0垂直垂直,m(1)(t)导致非自治孤子的加速传播。由于m(1)(t)的不同选择,所以出现了抛物线型,三次型,指数型和余弦型非孤子。对于情况2 [m(1)(t)= 0],如果光谱参数的实部等于0,则可以形成平稳孤子。如果我们将谐波外部电势系数m(2)(t)作为正常数,并让两个光谱参数的实部相同,则可以形成束缚态结构,但只有一个吸引人的结构,两种排斥程序。对于情况3 [m(0)(t)和m(1)(t)被视为非零常数),可以基于两个光谱参数的符号来形成正面互动,超越互动和束缚态结构。

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