共查询到18条相似文献,搜索用时 156 毫秒
1.
利用推广的齐次平衡方法,研究了(2+1)维BroerKaup方程的局域相干结构.首先根据领头项分析,给出了这个模型的一个变换,并把它变换成一个线性化的方程,然后由具有两个任意函数的种子解构造出它的一个精确解,发现(2+1)维BroerKaup方程存在相当丰富的局域相干结构.合适的选择这些任意函数,一些特殊型的多dromion解,多lump解,振荡型dromion解,圆锥曲线孤子解,运动和静止呼吸子解和似瞬子解被得到.孤子解不仅可以存在于直线孤子的交叉点上,也可以存在于曲线孤子的交叉点或最临近点上.呼吸子在幅度和形状上都进行了呼吸.本方法直接而简单,可推广应用一大类(2+1)维非线性物理模型.
关键词:
浙江师范大学非线性物理研究室
金华321004 浙江海洋学院物理系
舟山316004 相似文献
2.
势形式破裂孤子方程的dromion孤子解结构 总被引:3,自引:3,他引:0
使用改进的齐次平衡方法,研究了破裂孤子方程的孤子解结构,发现它具有单孤子解,单曲线孤子解,单dromion孤子解,多dromion孤子解。 相似文献
3.
从可积模型的双线性形式出发,可以得到关于方程场变量或某种势所存在的所有方向都是指数局域的dromion解或除一个方向外指数衰减的“Solitoff”解.以(1+1)维和(2+1)维KdV类型方程为例,对孤子(dromions或“Solitoff”)间的相互作用进行了详细的研究,发现孤子间的相互作用规律与方程的维数和类型无关.只要方程的多孤子解形式符合Hirota标准形式(所有耦合系数均不为零),孤子之间的碰撞是弹性的,否则就是非弹性的
关键词:
可积模型
孤子相互作用
双线性方法 相似文献
4.
用分离变量法研究了新(2+1)维非线性演化方程的相干孤子结构.由于Bcklund变换和变量分离步骤中引入了作为种子解的任意函数,得到了新(2+1)维非线性演化方程丰富的孤子解.合适地选择任意函数,孤子解可以是solitoffs,dromions,dromion格子,呼吸子和瞬子.呼吸子不仅在幅度、形状,各峰间距离,甚至在峰的数目上都进行了呼吸.
关键词:
新(2+1)维非线性演化方程
分离变量法
孤子结构 相似文献
5.
利用分离变量法,研究了(2+1)维非线性薛定谔(NLS)方程的局域结构.由于在B?cklund变换和变量分离步骤中引入了作为种子解的任意函数,得到了NLS方程丰富的局域结构.合适地选择任意函数,局域解可以是dromion,环孤子,呼吸子和瞬子.dromion解不仅可以存在于直线孤子的交叉点上,也可以存在于曲线孤子的最近邻点上.呼吸子在幅度和形状上都进行了呼吸
关键词:
非线性薛定谔方程
分离变量法
孤子结构 相似文献
6.
7.
8.
利用分离变量法得到了2+1维Nizhnik-Novikov-Veselov方程包含三个任意函数的精确解.合 适地选择任意函数,该精确解可以是描述所有方向指数局域的dromion相互作用,三个方向 指数局域的‘Solitoff’和dromion相互作用以及线孤子和y周期孤子相互作用的解.对dromi on相互作用从解析和几何两个角度进行了详细地探讨,揭示了一些新的相互作用规律.
关键词:
dromions相互作用
NNV方程
分离变量法 相似文献
9.
从(2+1)维双线性形式的非局域Bussinesq(NLBQ)方程和KP方程的隐线孤子解出发,可以找到与某种势所相应的各方向都指数衰减的dromion解.利用图形分析的方法,对这些dromion之间的相互作用进行了详细的研究.发现这两种模型中的dromion间的相互作用只引起位相漂移,不引起形状和速度的变化,也不引起旋转.即dromion间的相互作用是弹性的,没有能量、动量和角动量的交换.
关键词: 相似文献
10.
借助Mathematica符号计算软件,利用拓展的F/G展开法和变量分离法,得到(2+1)维耗散长波方程的精确解.通过选择适当的函数,获得(2+1)维耗散长波方程的亮暗dromion解和周期孤波解. 相似文献
11.
A SIMPLE SOLITON SOLUTION METHOD FOR THE (2+1) DIMENSIONAL LONG DISPERSIVE WAVE EQUATIONS 总被引:1,自引:0,他引:1 下载免费PDF全文
A simple and direct method is presented to solve the (2+1) dimensional long dispersive wave equation. We introduced a variable dependent transformation in order to convert this equation into the simple forms, which are three coupled linear and bilinear partial differential equations, and give the single and double soliton solutions and the (1, N) dromion solution. 相似文献
12.
Zhang Jiefang 《International Journal of Theoretical Physics》1999,38(8):2253-2258
Hirota's bilinear form of the (2 +1)-dimensional breaking-soliton equations introduced byBogyovlenskii is deduced in a straightforward manner andused to construct wave-type solutions for the fieldvariables. The peculiar localization behavior of thesystem by the generating dromion for the composite fieldvariable qr is also brought out and is generalized to(1, N, 1) dromions. 相似文献
13.
The abundant generalized dromion structures for the (2+1)-dimensional KdV equation are obtained using the homogeneous balance method. We give not only the general curve soliton which is finite on a curved line and localized apart from the curve, find but also the dromion solutions which can be driven by two perpendicular line soliton and by two non-perpendicular line soliton and by one line soliton and one curve line soliton. Various types of multi-dromion solutions can be constituted by selecting different arbitrary functions of y. The (1+N) dromion obtained by Radha et al. is only a very special case of our results. 相似文献
14.
YANZhen-Ya 《理论物理通讯》2002,37(3):269-276
We have found two types of important exact solutions,compacton solutions,which are solitary waves with the property that after colliding with their own kind,they re-emerge with the same coherent shape very much as the solitons do during a completely elastic interaction,in the (1 1)D,(1 2)D and even (1 3)D models,and dromion solutions (exponentially decaying solutions in all direction) in many (1 2)D and (1 3)D models.In this paper,symmetry reductions in (1 2)D are considered for the break soliton-type equation with fully nonlinear dispersion (called BS(m,n) equation)ut b(u^m)xxy 4b(u^n δx^-1uy)x=0,which is a generalized model of (1 2)D break soliton equation ut buxxy 4buuy 4buxδx^-1uy=0,by using the extended direct reduction method.As a result,six types of symmetry reductions are obtained.Starting from the reduction equations and some simple transformations,we obtain the solitary wavke solutions of BS(1,n) equations,compacton solutions of BS(m,m-1) equations and the compacton-like solution of the potential form (called PBS(3,2)) ωxt b(ux^m)xxy 4b(ωx^nωy)x=0.In addition,we show that the variable ∫^x uy dx admits dromion solutions rather than the field u itself in BS(1,n) equation. 相似文献
15.
16.
Using extended homogenous balance method, we obtain Bäcklund transformation (BT) and a linear partial differential equation of higher-order Broer-Kaup (HBK) system. As a result, multisoliton and single soliton and other exact solutions of (2+1)-dimensional HBK system are given. By analyzing single soliton solution, we get some dromion solutions. 相似文献
17.
Oscillating Solitons for (2+1)-Dimensional Nonlinear Models 总被引:1,自引:0,他引:1
Using extended homogeneous balance method and variable separation hypothesis,we found new variableseparation solutions with three arbitrary functions of the (2 1)-dimensional dispersive long-wave equations.Based on derived solutions,we revealed abundant oscillating solitons such as dromion,multi-dromion,solitoff,solitary waves,and so on,by selecting appropriate functions. 相似文献