利用Hirota双线性法求解一类非线性发展方程

利用hirota双线性法和Hopf-Cole变换,得到(3+1)维广义KP方程、广义(3+1)维浅水波方程、(1+1)维Boussinesq方程、(2+1)维Nizhnik方程的精确解,并做出一部分解的图形,进一步研究解的结构和性质.实践证明,方法对于研究非线性发展方程具有十分重要的作用.     

一类非线性数学物理方程的精确解

利用改进的辅助方程法,分别获得(1+1)维Benjiamin Ono方程、Phi-4方程、(3+1)维YTSF方程、foam drainage方程的精确解,进一步扩大了解的范围,丰富了解的结构.实践证明,利用这种辅助方程法对于研究非线性数学物理方程具有十分重要的作用.     

两类非线性发展方程的新的显式解

应用指数函数法,得到了(1+1)维Sinh-Gordon方程、(2+1)维Boiti-Leon-Manna-Pempinelli(BLMP)方程的一些新的显式解.     

几个非线性发展方程的精确解

应用改进F/G展开法求得(2+1)维BBM方程、(1+1)维Benjiamin Ono方程、广义(2+1)维ZK-MEW方程的精确解,这些解包括双曲函数解、三角函数解.当对双曲函数解中的参数取特殊值时,可得到孤立波解:当对三角函数解中的参数取特殊值时,可得到周期波函数解.实践表明,F/G展开法在非线性发展方程中具有广泛的应用.     

应用改进的Kudryashov法求非线性方程的精确解

利用Kudryashov法分别得到(1+1)维Benjiamin Ono方程、(2+1)维AKNS方程、分数阶生物群体模型方程的精确解.实践证明,这种方法简洁方便,对于研究非线性发展方程具有十分重要的意义.     

关于不定方程3x(x+1)(x+2)(x+3)=10y(y+1)(y+2)(y+3)

通过利用pell方程、递归序列、平方剩余、Legendre符号、同余关系等初等证明方法,并利用Mathematica软件对Legendre符号等进行计算,证明了方程3x(x+1)(x+2)(x+3)=10y(y+1)(y+2)(y+3)共有16组整数解,并且无正整数解.     

关于丟番图方程x(x+1)(x+2)(x+3)=27y(y+1)(y+2)(y+3)

先后运用了pell方程、勒让德符号,同余关系,递归序列、二次平方剩余,分类讨论的有关方法,并通过使用数学软件Mathematica进行计算,证明了以下结论:不定方程x(x+1)(x+2)(x+3)=27y(y+1)(y+2)(y+3)没有正整数解,并找出了该方程的全部16组整数解.     

用Hirota双线性方法构造一种(3+1)维高维孤子方程的多孤子解

通过两种方法构造了一种(3+1)维高维孤子方程的孤子解.第一种方法是利用对数函数变换,将其化成双线性形式的方程,在用级数扰动法求解双线性方程的单孤子解、双孤子解和N-孤子解.第二种方法是用广义有理多项式与试探法相结合,构造了(3+1)维高维孤子方程的怪波解.     

(2+1)维耦合MKP型方程的分解及其显式解

利用(2+1)维耦合MKP型方程与它分解后的(1+1)维DNLS方程之间的关系,用达布变换的方法求出(1+1)维DNLS方程的显式解,进而得到(2+1)维耦合MKP型方程的显式解.     

指数Diophantine方程4~x+b~y=(b+4)~2

本文研究了指数Diophantine方程4~x+b~y=(b+4)~2的解.设b1是给定的正奇数,运用有关指数Diophantine方程的已知结果以及有关Pell方程的Stormer定理的推广,证明了方程4~x+b~y=(b+4)~2仅有正整数解(x,y,z)=(1,1,1).     

Backlund Transformation and Exact Solution to Kadomtsev-Petviashvili Equation with Variable Coefficients

By using the homogeneous balance principle, we derive a Backlund transformation (BT) to (3+1)-dimensionaI Kadomtsev-Petviashvili (K-P) equation with variable coefficients if the variable coefficients are linearly dependent. Based on the BT, the exact solution of the (3+1)-dimensional K-P equation is given. By the same method, we derive a BT and the solution to (2+1)-dimensional K-P equation. The variable coefficients can change the amplitude of solitary wave, but cannot change the form of solitary wave.     

The Hirota Method and Soliton Solutions to the Multidimensional Nonlinear Schrodinger Equation

Using the Hirota method, we obtain a 1-soliton solution to the (3+1)-dimensional nonlinear Schrodinger equation.     

Lump Solutions, Lump-soliton Interaction Phenomena and Breather-soliton Solutions to a (3+1)-dimensional Boiti-Leon-Manna-Pempinelli-like Equation

The (3+1)-dimensional Boiti-Leon-Manna-Pempinelli-like equation (BLMP-like equation) is introduced by the generalized bilinear operators $D_{p}$ associated with $p=3$. The lump solutions, lump-soliton interaction phenomena and breather-soliton solutions are discussed to the (3+1)-dimensional BLMP-like equation based on the generalized bilinear method with symbolic computation system Mathematica. In order to observe the behavior of those solutions, we fix the value of $z$, then give the 3D-graphs of some solutions at different times. We find a lump solution moved in oblique direction; a lump-soliton interaction phenomenon is appeared and disappeared along with the time. We also see a kink-breather soliton moved in oblique direction.     

A new note on exact complex travelling wave solutions for (2+1)-dimensional B-type Kadomtsev-Petviashvili equation

Exact solutions of the (2+1)-dimensional Kadomtsev-Petviashvili by Zhang [Huiqun Zhang, A note on exact complex travelling wave solutions for (2+1)-dimensional B-type Kadomtsev-Petviashvili equation, Appl. Math. Comput. 216 (2010) 2771-2777] are considered. To look for “new types of exact solutions travelling wave solutions” of equation Zhang has used the G′/G-expansion method. We demonstrate that there is the general solution for the reduction by Zhang from the (2+1)-dimensional Kadomtsev-Petviashvili equation and all solutions by Zhang are found as partial cases from the general solution.     

一个2+1维变形Boussinesq方程的N孤子解

研究了一个2＋1维变形Boussinesq非线性发展方程：utt-uxx-uyy-3（u^2）xx-uxxxx=0,运用Hirota双线性方法得到它的N孤子解.     

Deformation and (3+1)-dimensional integrable model

A suitable and effective deformation relation is derived by using the Miura transformation. In the light of this relation, the (2+1)-dimensional linear heat conductive equation is deformed to a (3+1)-dimensional model. It is proved by standard singularity structure analysis that the (3+1)-dimensional nonlinear equation obtained here is Painlevé integrable.     

Jacobi Elliptic Function Solutions and Traveling Wave Solutions of the (2 + 1)-Dimensional Gardner-KP Equation

The fully integrable KP equation is one of the models that describes the evolution of nonlinear waves, the expansion of the well-known KdV equation, where the impacts of surface tension and viscosity are negligible. This paper uses the Modified Extended Direct Algebraic (MEDA) method to build fresh exact, periodic, trigonometric, hyperbolic, rational, triangular and soliton alternatives for the (2 + 1)-dimensional Gardner KP equation. These solutions that we discover in this article will help us understand the phenomena of the (2 + 1)-dimensional Gardner KP equation. Comparing the study in this paper and existing work, we find more exact solutions with soliton and periodic structures and the rational function solution in this paper is more general than the rational solution in existing literature. Most of the Jacobi elliptic function solutions and the mixed Jacobi elliptic function solutions to the (2 + 1)-dimensional Gardner KP equation discovered in this paper, to the best of our highest understanding are not seen in any existing paper until now.     

（3＋1）维带有源项的反应扩散方程的不变集和精确解

讨论了（3＋1）维带有源项的反应扩散方程ut=A1（u）uxx＋A2（u）uyy＋A3（u）uzz＋B1（u）ux^2;＋B2（u）uy^2＋B3（u）uz^2＋Q（u）．通过构建函数不变集的思想方法．得到了上述方程的几个新精确解．该方法也可以用来解N＋1维反应扩散方程．     

A quest for the integrable equation in 3+1 dimensions

The L and T operators of the Korteweg-de Vries equation are modified to seek a (3+1)-dimensional integrable equation. However, the Lax equation in this case is eventually reduced to a (2+1)-dimensional equation. We also propose other modified equations and their Lax pairs. A similar attempt is made to derive a higher-dimensional Harry Dym (HD) equation. As a result, a new (2+1)-dimensional HD equation is presented. Translated from Teoreticheskaya i Matematicheskaya Fizika, Vol. 122, No. 2, pp. 305–309, February, 2000.     

Exact Solutions for (3+1)-Dimensional Wick-Type Stochastic KP Equation

In the paper, the (3+1)-dimensional Wick-type stochastic KP equation is considered. And the exact solutions for (3+1)-dimensional Wick-type stochastic KP equation are obtained via homogeneous balance principle and Hermite transformation.