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ISRN Applied Mathematics
Volume 2013 (2013), Article ID 186376, 6 pages
Darboux Transformation and Explicit Solutions for a Generalized Sawada-Kotera Equation
1Department of Mathematics and Information Science, Zhengzhou University of Light Industry, Zhengzhou 450002, China
2Department of Mathematics, Henan Institute of Engineering, Zhengzhou 451191, China
Received 17 April 2013; Accepted 13 May 2013
Academic Editors: A. Bellouquid, M. Mei, J. Park, and F. Tadeo
Copyright © 2013 Guo-Liang He and Ting Su. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
A generalized Sawada-Kotera equation and its Lax pairs are proposed. With the help of the gauge transformation between spectral problems, a Darboux transformation for the generalized SK equation is constructed. As an application of the Darboux transformation, we give some explicit solutions of the generalized SK equation such as the rational solutions, soliton solutions, and periodic solutions.
The Sawada-Kotera (SK) equation was first proposed by Sawada and Kotera when they gave a method for finding N-soliton solutions of the KdV equation and the KdV-like equation . In , Caudrey et al. showed that (1) was a member of a new hierarchy of KdV equations. The SK equation’s physical importance was illustrated by Aiyer et al. in . Then, the equation has been investigated by many authors [4–8]. The aim of the present paper is using the Darboux transformation [9–12] to study a generalized SK equation:
The present paper is organized as follows. In Section 2, with the aid of the Lax pairs of the SK equation [13, 14] and extending them by adding one potential function, we propose a generalized SK equation and its Lax pairs. Based on the gauge transformation between spectral problems, we derive a Darboux transformation of the generalized SK equation. In Section 3, the Darboux transformation is applied to the generalized SK equation, by which explicit solutions (we have verified the correctness of the solutions by using the Mathematic 5.0.) of the generalized SK equation are derived, including rational solutions, soliton solutions, and periodic solutions.
2. Darboux Transformation of the Generalized Sawada-Kotera Equation
In this section, we will derive a generalized SK equation and its Darboux transformation. To this end, we first introduce the Lax pairs: where operators and are defined as follows: Then the compatibility condition between the two equations of (3) yields the Lax equation, , which is equivalent to the generalized SK equation: If we choose and , (5) can be, respectively, reduced to the SK equation: and the Kaup-Kupershmidt equation:
Proof. Assume that satisfies (3) and . Let
Using the first expression of (3), a direct calculation gives the following equations:
Substituting (9) and (10) into the following equation:
and comparing the coefficients of , , and , we obtain the following:
Equation (13) implies the following:
Substituting (15) into (14) and integrating it once, we have the following:
where is a constant of integration. Through direct calculations, we arrive at the following:
Using (17) and , a simple reduction shows that (16) gives rise to the following:
Similarly, we consider the following equation: where Seeing (3), (8), and (9), a direct calculation shows that (19) gives the following: which together with (17) implies the following:
This means that both of the Lax pairs (3) and (11) and (19) have the same form; that is, they lead to the same equation (5). Therefore, original solutions , of the generalized SK equation (5) are mapped into its new ones , by the Darboux transformation (8).
3. Explicit Solutions of the Generalized Sawada-Kotera Equation
(I) We choose a trivial solution , of (5). Then (3) with is reduced to the following: Let . We can see that (23) has a general solution: where , are constants and Using the Darboux transformation (8), we get an explicit solution of (5)
Case 2. When , (28) has a general solution:
where , are constants and
Using the Darboux transformation (8), we get an explicit solution of (5):
(III) We choose another trivial solution , of (5). Then (3) with is reduced to the following:
Case 1. For , a direct calculation gives a general solution of (34): where , are constants and . Using the Darboux transformation (8), we get a soliton solution of the generalized SK equation (5) : Plots of the solutions are given in Figures 3 and 4.
This work was supported by National Natural Science Foundation of China (no. 11171312) and Henan Natural Science Foundation of Basic Research (no. 102300410214).
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