“…The remaining problem is to construct the matrix S by virtue of the solutions of the linear eigenvalue problems (4). However, there are reduction (9) and constraints among elements in Q and the Darboux transformation should keep the reduction and those constraints. Therefore, it is not easy to treat the reduced problem.…”
Section: The Darboux Transformation Of System (3)mentioning
The Darboux transformation is applied to a multi-component nonlinear Schrödinger system, which governs the propagation of polarized optical waves in an isotropic medium. Based on the Lax pair associated with this integrable system, the formula for the n-times iterative Darboux transformation is constructed in the form of block matrices. The purely algebraic iterative algorithm is carried out via symbolic computation, and two different kinds of solutions of practical interest, i. e., bright multi-soliton solutions and periodic solutions, are also presented according to the zero and nonzero backgrounds.
“…The remaining problem is to construct the matrix S by virtue of the solutions of the linear eigenvalue problems (4). However, there are reduction (9) and constraints among elements in Q and the Darboux transformation should keep the reduction and those constraints. Therefore, it is not easy to treat the reduced problem.…”
Section: The Darboux Transformation Of System (3)mentioning
The Darboux transformation is applied to a multi-component nonlinear Schrödinger system, which governs the propagation of polarized optical waves in an isotropic medium. Based on the Lax pair associated with this integrable system, the formula for the n-times iterative Darboux transformation is constructed in the form of block matrices. The purely algebraic iterative algorithm is carried out via symbolic computation, and two different kinds of solutions of practical interest, i. e., bright multi-soliton solutions and periodic solutions, are also presented according to the zero and nonzero backgrounds.
“…Generalization of the mKdV equation to a multicomponent system or matrix equation was studied in [13]. Relatively recently, Iwao and Hirota [14] discussed a simple coupled version of the mKdV equation or the so-called coupled mKdV equation…”
We introduced complexly coupled modified KdV (ccmKdV) equations, which could be derived from a two-layer fluid model [Yang and Mao, Chin. Phys. Lett. 25, 1527 (2008); Hu, J. Phys. A: Math. Theor. 43, 185207 (2009)], and used the Miura transformation to construct expressions for their alternative Lax pair representations. We derived a Lagrangian-based approach to study the Hamiltonian structures of the ccmKdV equations and observed that the complexly coupled mKdV equations have an additional analytic structure. The coupled equations were characterized by two alternative Lagrangians not connected by a gauge term. We examined how the alternative Lagrangian descriptions of the system affect the bi-Hamiltonian structures.
Abstract. Soliton equations whose solutions are expressed by Pfaffians are briefly discussed. Included are a discrete-time Toda equation of BKP type, a modified Toda equation of BKP type, a coupled modified KdV equation and a coupled modified KdV equation of derivative type.
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