JAMPJournal of Applied Mathematics and Physics2327-4352Scientific Research Publishing10.4236/jamp.2016.410195JAMP-71554ArticlesPhysics&Mathematics The Pfaffian Technique: A (2 + 1)-Dimensional Korteweg de Vries Equation LixiaoZhai1JunxiaoZhao1School of Mathematical Sciences, University of Chinese Academy of Sciences, Beijing, China13102016041019301935September 13, 2016Accepted: October 23, October 27, 2016© Copyright 2014 by authors and Scientific Research Publishing Inc. 2014This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/

The (2 + 1)-dimensional Korteweg de Vries (KdV) equation, which was first derived by Boiti et al., has been studied by various distinct methods. It is known that this (2 + 1)-dimensional KdV equation has rich solutions, such as multi-soliton solutions and dromion solutions. In the present article, a unified representation of its N-soliton solution is given by means of pfaffian. We’ll show that this (2 + 1)-dimensional KdV equation is nothing but the Plücker identity when its τ-function is given by pfaffian.

The (2 + 1)-Dimensional Korteweg de Vries Equation Hirota Bilinear Method Pfaffian Plücker Identity
1. Introduction

The solitary wave, so-called because it often occurs as a single entity and is localized, was first observed by J. Scott Russell on the Edinburgh-Glasgow Canal in 1834. It is known that many nonlinear evolution equations have soliton solutions, such as the Korteweg de Vries equation, the Sin-Gordon equation, the nonlinear Schrödinger equation, the Kadomtsev-Petviashvili equation, the Davey-Stewartson equation, etc. In order to study the property of nonlinear evolution equations, methods are developed to derive solitary wave solution or soliton solution to nonlinear evolution equations. Some of the most important methods are the inverse scattering transformation (IST)  method, the bilinear method  -  , symmetry reduction method  , the Bäcklund or Darboux transformation method  and so on. Having soliton solutions is one of the basic integrable properties of nonlinear evolution equations.

In this paper, we are interested in the general expression of N-soliton solution to the (2 + 1)-dimensional KdV equation,

which was first derived by Boiti et al. by using the idea of the weak Lax pair  . This system can also be obtained from the inner parameter-dependent symmetry constraint of the KP equation  . Recently, the dromion solutions and some exact solutions are studied by Lou and Wazwaz respectively  -  . While as for the uniformed ex- pression of its N-soliton solution is unknown yet.

In this article, we’ll study the N-soliton solution to the (2 + 1)-dimensional KdV system (1). A compact form of the N-soliton solution to Equation (1) is obtained by means of pfaffian technique, which is given in section 2. Conclusion and further discussions are given in section 3.

2. N-Soliton Solution to the (2 + 1)-Dimensional KdV Equation

Given a nonlinear evolution equation, if it has 3-soliton solution, then this equation is of great possibility of having N-soliton () solution. Pfaffian technique is one of the methods that can help us to determine whether the evolution equation has multi- soliton solutions or not. In this section, we first review some properties of pfaffian.

2.1. Pfaffian

Pfaffians are antisymmetric functions with respect to its independent variables

An n-th order pfaffian can be defined inductively by the expansion rule 

where denotes the absence of letter j. For example, when n = 2, we have

There are various kinds of pfaffian identities. In this article, we just introduce the so-called Plüker relation for pfaffians 

which we are going to use. Hereafter, we let denote pfaffian

for simplicity.

2.2. N-Soliton Solutions

The Hirota form of the (2 + 1)-dimensional KdV system (1) is

which is obtained by the dependent variable transformations

Here the Hirota bilinear operator is defined by

with n and m are arbitrary nonnegative integers.

In  , the 3-soliton solution to the (2 + 1)-dimensional KdV system (3) is obtained

where

via the perturbation method. It claims that the N-soliton solutions for can also be obtained by using perturbation method, but the explicit expression of the multi- soliton solution is not given.

In this article, we’ll study the the multi-soliton solution to Equation (3) using the pfaffian technique   . A compact form of the N-soliton solution is given in terms of N-th order pfaffian.

Proposition 1. If the t-function f of the (2 + 1)-dimensional KdV system (3) is given by the pfaffian function

whose entries, for, are defined by

then this particular pfaffian function (6) gives an N-soliton solutions to the (2 + 1)-di- mensional KdV system (3).

Proof. In the following, we will prove that the pfaffian function (6) satisfies the (2 + 1)-dimensional KdV Equation (3). By defining “differential operators” ()

we obtain the following differential formulae

In order to find the pfaffian expression for the differential functions with derivative of variable y, we need to define another letter 

Then we have

Substituting formulae (9) and (11) into the right hand side of Equation (3), we obtain nothing but the Plücker relation for pfaffians (2)

where denotes. Therefore the pfaffian function (6) solves the (2 + 1)-dimensional KdV system (3).

Note that in order to derive the differential formulae of the pfaffian function (6), we have to define another extra letter besides the “differential operators”. The multi-soliton solution to the nonlinear (2 + 1)-dimensional KdV system (1) can be obtained by substituting pfaffian function (6) into the dependent variable transfor- mation (4) directly.

3. Conclusion

In this article, a compact form of the multi-soliton solution to the (2 + 1)-dimensional KdV system is given via the pfaffian technique. As one can see, the key point of the proof is to derive suitable expressions of the differential formulae of pfaffian t-function f. It is worth pointing out that the method used in this article is different as the one for the proof of the BKP equation, which the differential formulae of the pfaffian t-fun- ction depend only on the “differential operators”.

Acknowledgements

We thank the editor and the referee for their comments. This research work is supported by the National Science Foundation of China (Grant Numbers 11271362, 11271266 and 11501510) and a President’s Grant from the University of Chinese Academy of Sciences. These supports are greatly appreciated.

Cite this paper

Zhai, L.X. and Zhao, J.X. (2016) The Pfaffian Technique: A (2 + 1)-Dimensional Korteweg de Vries Equation. Journal of Applied Mathema- tics and Physics, 4, 1930-1935. http://dx.doi.org/10.4236/jamp.2016.410195

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