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1)  solitary-wave-like solutions
类孤立波解
1.
By using two extended Riccati equations and Mathematica software,the author obtains exact solutions to the Variable Coefficient Burgers Equation with forced term outside and Witham-Broer-Kaup equation,including many kinds of solitary-wave-like solutions,like periodical solutions and solitary wave solutions with variable speed,many of which are found for the first time.
借助两个推广形式的Riccati方程组和Mathematica软件,求出了具外力项变系数Burgers方程和Witham- Broer-Kaup方程的一些精确解,包括各种类孤立波解、类周期解和变速孤立波解,其中许多解是新的。
2.
Including many kinds of solitary-wave-like solutions and like-periodical solutions,many solutions are new.
基于齐次平衡原则和分离变量法的思想,通过两个推广的Riccati方程组和Mathematica软件,求出了变系数(2+1)维Broer-kaup方程的一些精确解,包括各种类孤立波解、类周期解,其中许多解是新的。
2)  solitary wave solutions
孤立波解
1.
Periodic wave solutions and solitary wave solutions to (2+1)-dimensional KdV equation;
(2+1)维KdV方程的周期波解和孤立波解
2.
Exact solitary wave solutions of the coupled K d V equations;
一个耦合KdV方程组的精确孤立波解
3.
New solitary wave solutions for (n+1) dimensional Klein-Gordon-Schrdinger equations;
(n+1)维Klein-Gordon-Schrdinger方程组新的孤立波解
3)  Solitary wave solution
孤立波解
1.
Compacton solution and solitary wave solution for a class of nonlinear intensity Boussinesq equation;
一类非线性强度Boussinesq方程的Compacton解和孤立波解
2.
Exact solitary wave solutions for the Gross-Piteavskii equation with time-dependent linear potential;
含时线性势Gross-Piteavskii方程的孤立波解
3.
The solitary wave solutions with varying velocity for the (3+1)-dimensional variable-coefficients ZK equation;
变系数(3+1)维ZK方程的变速孤立波解
4)  solitary solution
孤立波解
1.
New periodic and solitary solution for the generalized fifth KdV equation;
广义五阶KdV方程的新的周期波解与孤立波解
2.
Envelope periodic and solitary solutions of Davey-Stewartson equation
Davey-Stewartson方程组的包络周期解和孤立波解
3.
The result of reductions gives rise to abundant solutions: Compacton solutions, peakon solutions,kink solutions, and bell-shaped solitary solutions.
在3种规则的要求下得到了广义Camassa-Holm方程的对称性约化,特别研究了C(m,1,1)的对称性约化,约化的结果得到了丰富的解:紧孤立波解(Compacton),尖峰孤立波解(peakon),扭结解和光滑的钟型孤立波解。
5)  soliton solution
孤立波解
1.
For example SK equation,using simple equation and Painleve test,we get many solutions of SK equation,including soliton solutions and some periods solutions.
利用已知精确解的简单方程求解高阶非线性发展方程,以SK方程为例,利用简单方程和Painleve截断展开法,求出该方程的多组行波解,包括孤立波解和类孤立波解,以及若干周期函数解,这种方法还可以用来求解其他高阶非线性发展方程。
2.
Some new elliptic periodic solutions and soliton solution of variable coefficient KdV-MKdV equation with three arbitrary functions by are found Jacobi elliptic function expansion method.
运用Jacobi椭圆函数展开法求得了具有3个任意函数的变系数KdV_MKdV方程的新椭圆周期解及孤立波解。
6)  solitary wave-like solution
类孤波解
1.
New solitary wave-like solution and analytic solution of generalized KdV equation with variable coefficients;
变系数广义KdV方程新的类孤波解和解析解
2.
New solitary wave-like solution and exact solution of variable coefficient KP equation;
变系数KP方程新的类孤波解和解析解
3.
These solutions degenerate to solitary wave-like solutions at a certain limit.
 将Jacobi椭圆正弦函数展开法与Jacobi椭圆余弦函数展开法引入到变系数KdV方程组的求解中,得到了三组类周期波解· 这些解析解在一定条件下退化为类孤波解·
补充资料:别解四类
【别解四类】
 (术语)今于四类之别解中,示地狱界与人界及佛界三种之相。先言地狱界之十如是,相如是者恶人显后堕地狱之前相,凡夫虽不知,而佛菩萨之目,则能见之也。性如是者,专习恶之人其习状如生成,改变为难也。体如是者:“摧折粗恶色心以为体质。”即堕于地狱为狱卒所责之荒恶身心体是也。私记二本云:“问:体者即指受报身。与报何异?答:阴身为体。苦乐为报。”力如是者:“地狱有登刀上剑之用。”即于地狱有上剑山上刃林裂破身体之力用也。作如是者:“构造经营。”谓于身口意之三业造恶也。私记云:“作是造业与因何别?答:构造为作,约外约色,习因为因,约内约心。”因如是者:“恶习因也。”谓于过去习恶也。缘如是者作恶之缘助也。果如是者,谓过去所习之恶事,受地狱之身亦能起也。报如是者:“铜柱铁床之苦。”谓于地狱攀登铜柱。坐热铁床也。本末究竟等者,相如是,报如是,皆为空谛故谓为等。又恶之果报在本之性相中,本之性相,在恶之果报中则为假谛等,又地狱之理体与佛果无异,则皆为中道法界,是中道之等也。次明人界之十如,则相如是者:“相表清升。”谓对于四恶趣之沉沦,格别清净,有上升之相也。性如是者:“性觉白法。”谓清白之善法,成为其性也。体如是者:“体是安乐身心。”谓与三途等苦报相违,安稳快乐之身心也。力如是者:“堪任善器。”谓堪于勤善之器也。作如是者:“造止行二善。”谓作止恶行善之二善也。因如是者:“因是白业。”谓成就清白之善因也。缘如是者:“作善我我所。”谓我思能作善也,此为白善之缘。果如是者:“任运修善心生。”谓依前来习善之习用,而自然生善心也,报如是者:“自然爱乐。”谓自然受人果之快乐也。本末究竟如前地狱界。次明佛界之十如,则“佛界十法者。皆约中道分别也。”言佛界之十如其体皆为中道也。此虽为一中道,而因义理相违,故分为十如。相如是者为缘因佛性,是外修万行也。性如是者为了因佛性,是内生真智也。体如是者为正因佛性,是真如法界也。力如是者,谓初发菩提心,超二乘上为力。是发菩提心也。作如是者四弘誓愿也。因如是者智慧庄严也。缘如是者福德庄严也。果如是者一念相应大觉朗然之无上正觉也。报如是者大般涅槃三德秘藏也。本末究竟等者三谛法界之体等也。
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