Jacobi椭圆函数有理式的Fourier级数*

本文列出了手册[1]及文献[2]中未计算过的九十余个Jacobi椭圆函数sn(u,k),cn(u,k),dn(u,k)的有理函数的Fourier展式.对于用Melnikov方法研究可积系统在周期扰动下的次谐波分枝与浑沌性质,及其他工程物理中的计算问题,这些公式可供查阅应用.     

传动系统扭振的重频条件

借助于传递矩阵法研究了两轴系扭振的重频条件。必要条件为:存在节点啮合对(JEC);充要条件为:四个边界传递系数(f_B)等于零的个数不少于3个。给出了两轴系存在重频时的振型选择。多级轴系重频的必要条件与两轴系的必要条件相同,而如果所有的相邻JEC之间的传递系数(f_I)等于零时,频率重数等于独立的f_B为零的个数减1.若存在f_I≠0,可将它所对应的连接部分删除,从而把整个轴系的JEC分成内部不含f_I≠0的几组,该阶频率的总重数等于各组独立解个数之和。     

泛系方法论与幻方构造

论述了泛系方法论的精缩影模式及其对求解、建模、算法生成与理论建构的作用,同时用泛系方法提出并证明了:1递归构造n阶幻方(n≥5)的方法;2已知m阶幻方和n阶幻方(m,n≥3),求mn阶幻方的公式;3已知m阶幻方(m≥3),构造2m阶幻方的方法。     

二维RLW方程的Cauchy问题

通过椭圆积分求出了二维RLW方程椭圆余弦波解,并用先验估计方法证明了该方程Cauchy问题关于小x、y周期解的若干性质和解的唯一性、稳定性。     

一个新非线性可积晶格族和它们的可积辛映射

该文引入一个离散特征值问题,导出一族离散可积系,建立了它们的Hamilton结构,证明了它们Louville可积性.通过谱问题双非线性化,得到了一个可积辛映射与一族有限维完全可积系,最后给出了离散可积系统解的表示.     

一类代数系统及其应用

本文利用已有的loop代数$\widetilde{A}_{1}$构造出代数系统$X$,然后建立了一个新的等谱问题得到著名的Volterra lattice可积系,最后通过构造出的$X$的扩展代数系统$\widetilde{X}$得到已有的可积系的可积耦合系统.     

广义Pochhammer-Chree方程的显式精确孤波解

首先对广义Pochhammer-Chre方程(PC方程)u_tt-u_ttxx+ru_xxt-(a₁u+a₂u2+a₃u3)_xx=0(r≠0)(Ⅰ)的孤波解u(ξ)建立了公式∫_-∞+∞[u'(ξ)]2dξ=1/12rv(C₊-C_-)3[3a₃(C₊+C_-)+2a₂]。由此推知:广义PC方程(Ⅰ)不可能有钟状孤波解,只可能有扭状孤波解;而广义PC方程u_tt-u_ttxx-(a₁u+a₂u2+a₃u3)_xx=0(Ⅱ)可能既有钟状孤波解又有渐近值满足3a₃(C₊+C_-)+2a₂=0的扭状孤波解。进一步求出了广义PC方程(Ⅰ)的扭状孤波解,求出了广义PC方程(Ⅱ)的钟状孤波解和渐近值满足2a₃(C₊+C_-)+2a₂=0的扭状孤波解。最后给出了广义PC方程u_tt-u_ttxx-(a₁u+a₃u3+a₅u5)_xx=0(Ⅲ)的显式孤波解。     

Hamilton体系与辛正交系的完备性*

本文定义了一个Banach空间ZH,并证明了一类Hamilton体系的本征函数系(辛正交系)在ZH空间中具有完备性.还证明了如下结论ZH空间能连续嵌入到L₂[0,1]×L₂[0,1]但ZH≠L₂[0,1]×L₂[0,1].     

非水平分层区域Helmholtz边值问题的解析解

在(x,y,z)直角坐标系中,N个物性参数不同的区域D_j(j=0,1,…,N-1)充斥着整个空间,这些区域间的分界面是非水平的光滑曲面S_j,j+1下面的边值问题称为非水平分层区域Helmholtz边值问题:
?2H(j)+K_jH(j)=0(j=0,1,…,N-1)
(H(0)-H(1))S_0.1=δ(S)(δ(S):广义δ-函数)
(H(j)-H(j+1))S_j,j+1=0(j=1,…,N-2)本文给出了此问题的解析解.     

Bargmann系统与耦合Harry-Dym方程解的对合表示

在位势与特征函数确定的约束下,耦合 Harry-Dym 方程 Lax 对的空间部分非线性化为一个完全可积的系统{R~(2N),dpΛdq,H=1/2〈Λ~2q,q〉〈Λq,q〉~(-2)+1/2〈p,p〉-1/2α〈q,q〉},而时间部分的非线性化导出它的 N-对合系{F_m}.约束映射将相容系统(H)、(F_m)的对合解映成 m 阶耦合 Harry-Dym 方程的解.一个 Neumann 系统和定态 Harry-Dym 方程之间的关系被讨论.系统{R~(2N),dpΛdq,(?)=1/2〈p,p〉-1/2〈Λq,q〉~(-1)-1/2α〈q,q〉}证明是完全可积的.     

Weierstrass integrability of differential equations

The integrability problem consists of finding the class of functions a first integral of a given planar polynomial differential system must belong to. We recall the characterization of systems which admit an elementary or Liouvillian first integral. We define Weierstrass integrability and we determine some Weierstrass integrable systems which are Liouvillian integrable. Inside this new class of integrable systems there are non-Liouvillian integrable systems.     

A hierarchy of Liouville integrable lattice equations and its integrable coupling systems

A new discrete two-by-two matrix spectral problem with two potentials is introduced, followed by a hierarchy of integrable lattice equations obtained through discrete zero curvature equations. It is shown that the Hamiltonian structures of the resulting integrable lattice equations are established by virtue of the trace identity. Furthermore, based on a discrete four-by-four matrix spectral problem, the discrete integrable coupling systems of the resulting hierarchy are obtained. Then, with the variational identity, the Hamiltonian structures of the obtained integrable coupling systems are established. Finally, the resulting Hamiltonian systems are proved to be all Liouville integrable.     

An integrable coupling hierarchy of the Mkdv_integrable systems, its Hamiltonian structure and corresponding nonisospectral integrable hierarchy

A four-by-four matrix spectral problem is introduced, locality of solution of the related stationary zero curvature equation is proved. An integrable coupling hierarchy of the Mkdv_integrable systems is presented. The Hamiltonian structure of the resulting integrable coupling hierarchy is established by means of the variational identity. It is shown that the resulting integrable couplings are all Liouville integrable Hamiltonian systems. Ultimately, through the nonisospectral zero curvature representation, a nonisospectral integrable hierarchy associated with the resulting integrable couplings is constructed.     

Integrability and linearizability of the Lotka-Volterra systems

Integrability and linearizability of the Lotka-Volterra systems are studied. We prove sufficient conditions for integrable but not linearizable systems for any rational resonance ratio. We give new sufficient conditions for linearizable Lotka-Volterra systems. Sufficient conditions for integrable Lotka-Volterra systems with 3:−q resonance are given. In the particular cases of 3:−5 and 3:−4 resonances, necessary and sufficient conditions for integrable systems are given.     

Integrability,computation and applications

The study of integrable systems and the notion of integrability has been re-energized with the discovery that infinite-dimensional systems such as the Korteweg-de Vries equation are integrable. In this paper, the following novel aspects of integrability are described: (i) solutions of Darboux, Brioschi, Halphen-type systems and their relationships to monodromy problems and automorphic functions, (ii) computational chaos in integrable systems, (iii) we explain why we believe that homoclinic structures and homoclinic chaos associated with nonlinear integrable wave problems, will be observed in appropriate laboratory experiments.     

Integrable pseudopotentials related to generalized hypergeometric functions

We construct integrable pseudopotentials with an arbitrary number of fields in terms of generalized hypergeometric functions. These pseudopotentials yield some integrable (2 + 1)-dimensional hydrodynamic type systems. In two particular cases these systems are equivalent to integrable scalar 3-dimensional equations of second order. An interesting class of integrable (1 + 1)-dimensional hydrodynamic type systems is also generated by our pseudopotentials.     

The behaviour of cyclic variables in integrable systems

A general theorem on the behaviour of the angular variables of integrable dynamical systems as functions of time is established. Problems on the motion of the nodal line of a Kovalevskaya top and of a three- dimensional rigid body in a fluid are considered in integrable cases as examples. This range of topics is discussed for systems of a more general form obtained from completely integrable systems after changing the time.     

Integrable decomposition of a hierarchy of soliton equations and integrable coupling system by semidirect sums of Lie algebras

Staring from a new spectral problem, a hierarchy of the soliton equations is derived. It is shown that the associated hierarchies are infinite-dimensional integrable Hamiltonian systems. By the procedure of nonlinearization of the Lax pairs, the integrable decomposition of the whole soliton hierarchy is given. Further, we construct two integrable coupling systems for the hierarchy by the conception of semidirect sums of Lie algebras.     

Infinitesimally stable and unstable singularities of 2-degrees of freedom completely integrable systems

In this article we give a list of 10 rank zero and 6 rank one singularities of 2-degrees of freedom completely integrable systems. Among such singularities, 14 are the singularities that satisfy a non-vanishing condition on the quadratic part, the remaining 2 are rank 1 singularities that play a role in the geometry of completely integrable systems with fractional monodromy. We describe which of them are stable and which are unstable under infinitesimal completely integrable deformations of the system.