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一类具有自诱导宇称-时间对称势的非局部非线性薛定谔方程的对称性与精确解

Symmetries and exact solutions of a class of nonlocal nonlinear Schrödinger equations with self-induced parity-time-symmetric potential.

作者信息

Sinha Debdeep, Ghosh Pijush K

机构信息

Department of Physics, Siksha-Bhavana, Visva-Bharati University, Santiniketan 731 235, India.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2015 Apr;91(4):042908. doi: 10.1103/PhysRevE.91.042908. Epub 2015 Apr 17.

Abstract

A class of nonlocal nonlinear Schrödinger equations (NLSEs) is considered in an external potential with a space-time modulated coefficient of the nonlinear interaction term as well as confining and/or loss-gain terms. This is a generalization of a recently introduced integrable nonlocal NLSE with self-induced potential that is parity-time-symmetric in the corresponding stationary problem. Exact soliton solutions are obtained for the inhomogeneous and/or nonautonomous nonlocal NLSE by using similarity transformation, and the method is illustrated with a few examples. It is found that only those transformations are allowed for which the transformed spatial coordinate is odd under the parity transformation of the original one. It is shown that the nonlocal NLSE without the external potential and a (d+1)-dimensional generalization of it admits all the symmetries of the (d+1)-dimensional Schrödinger group. The conserved Noether charges associated with the time translation, dilatation, and special conformal transformation are shown to be real-valued in spite of being non-Hermitian. Finally, the dynamics of different moments are studied with an exact description of the time evolution of the "pseudowidth" of the wave packet for the special case in which the system admits a O(2,1) conformal symmetry.

摘要

考虑一类非局部非线性薛定谔方程(NLSEs),其处于具有时空调制非线性相互作用项系数以及约束和/或增益损耗项的外部势场中。这是对最近引入的具有自诱导势的可积非局部NLSE的推广,该方程在相应的定态问题中是宇称-时间对称的。通过相似变换得到了非齐次和/或非自治非局部NLSE的精确孤子解,并通过几个例子进行了说明。结果发现,只有那些在原始空间坐标的宇称变换下变换后的空间坐标为奇数的变换才是允许的。结果表明,没有外部势的非局部NLSE及其(d + 1)维推广具有(d + 1)维薛定谔群的所有对称性。尽管非厄米,但与时间平移、伸缩和特殊共形变换相关的守恒诺特定荷被证明是实值的。最后,针对系统具有O(2,1)共形对称性的特殊情况,通过对波包“伪宽度”的时间演化进行精确描述,研究了不同矩的动力学。

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