The New Infinite Sequence Solutions of Multiple Sine-Gordon Equations

By the function transformation and the first integral of the ordinary differential equations, the problem of solving the solutions of the double sine-Gordon equation and the treble sine-Gordon equation is researched, and the new solutions are obtained. First, the problem of solving the solutions of the double sine-Gordon equation and the treble sine-Gordon equation is changed to the problem of solving the solutions of the nonlinear ordinary differential equation. Second, with the help of the Bäcklund transformation and the nonlinear superposition formula of solutions of the first kind of elliptic equation and the Riccati equation, the new infinite sequence soliton-like solutions of two kinds of sine-Gordon equations are constructed.


Introduction
Refs. [1]- [3] studied the problem of solving the solutions of the double sine-Gordon equation, and a finite number of new solutions consisting of Jacobi elliptic function, hyperbolic function and trigonometric function are obtained.
where p and λ are constants.
Refs. [4] [5] obtained the new solutions consisting of Jacobi elliptic function, hyperbolic function and trigonometric function of the treble sine-Gordon equation.
In this paper, by the function transformation and the first integral of the ordinary differential equations, the problem of solving the solutions of the double sine-Gordon equation and the treble sine-Gordon equation is changed to the problem of solving the solutions of the nonlinear ordinary differential equation.Based on these, with the help of the Bäcklund transformation and the nonlinear superposition formula of solutions of the first kind of elliptic equation and the Riccati equation, the new infinite sequence soliton-like solutions of two kinds of sine-Gordon equations are constructed, which are consisting of Riemann θ function, Jacobi elliptic function, hyperbolic function, trigonometric function and rational function.

Some Kinds of New Conclusions of Nonlinear Ordinary Differential Equation
The relative conclusions of the Bäcklund transformation of some kinds of ordinary differential equations introduced as follows are very important in constructing the new solutions of the two kinds of sine-Gordon equations.
, 2 According to the relative conclusions of the Riccati Equation [6] and the fitting Bäcklund transformation (4), the solutions of the ordinary differential Equation (3) ( ) are obtained.Theorem 2.2 There is the following fitting Bäcklund transformation between the ordinary differential Equation (3) and the first kind of elliptic Equation (6).
Then we put forward the fitting Bäcklund transformation between the ordinary differential Equation (3) and the first kind of elliptic Equation ( 6) in some cases.
the following Bäcklund transformation between the ordinary differential Equation (3) and the first kind of elliptic Equation (6).
− there is the following Bäcklund transformation between the ordinary differential Equation (3) and the first kind of elliptic Equation (6).
there is the following Bäcklund transformation between the ordinary differential Equation (3) and the first kind of elliptic Equation (6).( ) ( ) Here , P Q and R are arbitrary constants not equal to zero., A B and C are determined by the first kind of elliptic Equation (6).

Theorem 2.3 If ( )
y ξ is the solution that are not the constants of the first kind of elliptic Equation (6), then the following ( ) y ξ is also the solution of the first kind of elliptic Equation (6).
Here 0 , , M L W and H are arbitrary constants that are not all zero.Theorem 2. 4 The first kind of elliptic Equation ( 6) has the following some kinds of solutions.Case 1.The Riemann θ function new solutions [7] of the first kind of elliptic equation When , the first kind of elliptic Equation ( 6) has the following solution.
( ) ( ) ( ) where ( ) The Jacobi elliptic function new solutions of the first kind of elliptic equation According to the periodicity of the Jacobi elliptic function, some kinds of new solutions of the first kind of elliptic equation are obtained, some new solutions [6] [8] [9] are listed here.When ( ) ( ) . .
, the first kind of elliptic Equation ( 6) has the following solutions. .
, the first kind of elliptic Equation ( 6) has the following solutions.

The New Infinite Sequence Solutions of the Treble Sine-Gordon Equations
Substituting the functional transformation ( ) ( ) ( ) ( ) (where µ and ω are undetermined constants) into the Equation (2) yields the following ordinary differential equation By the functional transformation, the ordinary differential Equation ( 33) is changed to the ordinary differential Equations (34) Then by the functional transformation (35), the ordinary differential Equations ( 34) is changed to the ordinary differential Equations (36) ( )( ) We can obtain the first integral of the ordinary differential Equations (36) as follows where 0 C is an arbitrary constant.Substituting the first integral (37) into the first equation of the ordinary differential Equations (36) yields the following ordinary differential equation where With the help of the relative conclusions of some kinds of ordinary differential equations introduced in Part 2, the new infinite sequence solutions of the treble sine-Gordon equations are constructed

To Construct the New Infinite Sequence Solutions
When C 0 = 0 When 0 0 C = , the ordinary differential Equations ( 38) is changed to the following the ordinary differential equation.
where ( ) y τ is determined by the first kind of elliptic Equation (6).A, B and C are the coefficients of the first kind of elliptic Equation ( 6), and − .P, Q and R are arbitrary constants that are not all zero.
If the ( ) 0 y τ of the superposition Formula (40) are taken as the Solutions (15)-( 17) of the first kind of elliptic Equation ( 6), then the Riemann θ function type new infinite sequence solutions of the treble sine-Gordon equations are obtained.
If the ( ) 0 y τ of the superposition Formula (40) are taken as the Solutions ( 18)-(30) of the first kind of elliptic Equation ( 6), then the Jacobi elliptic function type new infinite sequence smooth-type soliton-like and tight-soliton solutions of the treble sine-Gordon equations are obtained.
where ( ) 0 y τ is determined by the first kind of elliptic Equation (6).A, B and C are the coefficients of the first kind of elliptic Equation (15), and − .P, Q and R are arbitrary constants that are not all zero.
If the ( ) 0 y τ of the superposition Formula (41) is taken as the Solution (31), then the trigonometric function type new infinite sequence solutions of the treble sine-Gordon equations are obtained.
If the ( ) 0 y τ of the superposition Formula (41) is taken as the Solution (32), then the hyperbolic function type new infinite sequence solutions of the treble sine-Gordon equations are obtained.

To Construct the
where p and r are arbitrary constants that are not all zero. ) where M is an arbitrary constants that is not zero.
( ) 0 v τ is determined by the first kind of elliptic Equation (46).

The New Infinite Sequence Solutions of the Double Sine-Gordon Equations
Substituting the functional transformation ( ) ( ) ( ) ( ) (where µ and ω are undetermined constants) into Equation (1) yields the following ordinary differential equation By the functional transformation, the ordinary differential Equation ( 48) is changed to the following two ordinary differential equations The two ordinary differential equations have the following first integral ( ) ( ) where 0 C is an integral constant.Substituting the first integral into the first equation of the ordinary differential Equations ( 49) and (50) severally yields the following two ordinary differential equation

Conclusion
By the auxiliary equation method, many kinds of smooth type soliton, tense type soliton and peak soliton and so on new solutions of the nonlinear evolution equations have been obtained [1]- [14].In this paper, by the function transformation and the first integral of the ordinary differential equations, the new infinite sequence soliton-like solutions consisting of the Riemann θ function, Jacobi elliptic function, hyperbolic function, trigonometric function and rational function of the double sine-Gordon equation and the treble sine-Gordon equation are obtained.These solutions conclude many kinds of smooth type soliton, tense type soliton and peak soliton and so on new solutions.Refs.[1]- [5] didn't obtain the new tense type soliton and peak soliton solutions of the double sine-Gordon equation and the treble sine-Gordon equation.
following Bäcklund transformation between the ordinary differential Equation (3) and the first kind of elliptic Equation(6).
= , the first kind of elliptic Equation (6) has the following solutions.

Case 3 .
The other new solutions of the first kind of elliptic equation When 2 first kind of elliptic Equation (6) has the following solutions.

1 .
The new infinite sequence smooth-type soliton-like solutions When the coefficients of the ordinary differential Equation (39case 2. of theorem 2.2, with the help of the following superposition formula, the new infinite sequence smooth-type soliton-like solutions of the treble sine-Gordon equations are obtained, which are consisting of Riemann θ function, Jacobi elliptic function and hyperbolic function.

If 1 k
= in the Jacobi elliptic function type solutions of the treble sine-Gordon equations, then the hyperbolic function type new infinite sequence solutions are obtained.Case 2. The new infinite sequence peak-type soliton solutions When Case 2. of the Theorem 2.2, with the help of the following superposition formula, the new infinite sequence peak soliton-like solutions of the treble sine-Gordon equations are obtained, which are consisting of hyperbolic function and trigonometric function.

(
The ordinary differential Equations (38) is changed to the following the ordinary differential equation when

3 H
τ are the solutions of the Riccati Equation (44).

3. 1 . 3 .
To Construct the New Infinite Sequence Solutions When C ordinary differential Equations (38) is changed to the following the ordinary differential equation.
C = , the ordinary differential Equations (53) is changed to the following the ordinary differential equation.
By the method to construct the new infinite sequence solutions of the treble sine-Gordon equation, we can also obtain the new infinite sequence solutions of the double sine-Gordon equation (not given here).