一个产生Jaulent-Miodek方程的无反射位势的五次Hamilton系统

在Jaulent-Miodek方程的无反射位势与平方特征函数的关系(u,v)~T=f(ψ)所确定的约束下,孤子方程的Lax对被非线性化成一个五次系统和一个非线性演化方程,而前者的解簇是由后者所确定的S-流的不变集。此外,f把五次系统的解映到某个驻定的Jaulent-Miodek方程的解。     

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.     

变形的非线性Schrdinger方程的反散射解法的Zakhallov-Shabat方程

c_(a)(0)和r(ξ,0)为常量.对(2)中的ξ取ξ_m,ξ-i∈,-in+∈,其中ξ_m为第一象限的常数,ξ,η为正实数,∈为无限小正量,就得到决定ψ_1,ψ_2的完备方程组. MNLS方程(1)的解可以表为(7)式中(8)(9)这里R_1为(3)中的R的上分量,R_2为R的下分量,R_1(0,x)=R_1(ξ,x)|t=0,R_2(0,x)=[dR_2(ξ,x)/dξ]ξ=0。当r(ξ’)=r(iη’)=0时,即无反射的情况,方程(2)已由我们最近用亚纯变换矩阵方法首次导出,它的多孤子解的显式也得出了.     

Levi族的Lax组非线性化

文[1]研究Levi族的Lax表示.今进一步讨论其Lax组的非线性化.设λ_1…,λ_N是Levi特征值问题的N个不同的特征值,那么φ_j(?)(φ_(1j),φ_(2j))~T是相应于特征值λ_j的特征函数,j=1,…,N.(?)=(?)/(?)x,q、r为势函数,x在所论区间Ω内变化. 浓缩(1)为向量形式:     

非线性椭圆障碍问题很弱解的全局可积性

本文研究一类非线性椭圆方程的K_(ψ,θ)~r(Ω)-障碍问题很弱解u的全局可积性,其中u的可积指数r满足max{1,p-1}r p n.令θ_*=max{θ,ψ},若θ_*∈W~(1,q)(Ω),q r,则上述问题的很弱解u具有全局可积性,这里r充分接近p.     

E^n中P维与q维平面间的夹角公式

本文将柯西不等式进一步推广为[α_1β,…,α_mβ][α_iα_j]~(-1)[α_1β,…,α_mβ]~T+(|α∧|β~2)/(|α|~2)≤β~2其中β=b_1∧…∧b_q,q≤p≤n,α_i 是从 p 个向量α_1,…,α_p 中任取 q 个作成的 q 重向量,m=c_p~q.接着给出了 n 维欧氏空间 E~n 中 p 维与 q 维平面间的夹角公式:cos~2θ=[α_1β,…,α_mθ][α_iα_j]~(-1)[α_1β,…,α_mβ]~T/β~2用它导出了 n-1维球面型空间 S_(n-1,1)中关于单形(顶点 P_n 到对面上)的高 h_n 的公式.     

双曲型守恒律组的一类差分格式及其熵条件

其中u(x,t)=(u_1(x,t),…,u_m(x,t))~T,f(u(x,t))=(f_1(u(x,t)),…,f_m(u(x,t)))~T,f的Jacobian记为 A(u)=?f(u)/?u,具有m个实特征值λ_1(u)≤λ_2(u)≤… ≤λ_m(u)以及完备的古特征向量系{γ_k(u)}_k~m=1.对区域R~+={(x,t)|x∈(-∞,+∞),t∈     

非线性脉冲微分方程边值问题正解的存在性

考虑如下非线性脉冲微分方程两点边值问题{-x'(t)=x~q,t∈(0,1),t≠1/2,△x|_(t=1/2)=β_1x(1/2),△x'|_(t=1/2)=-β_2x(1/2),x(0)=x(1)=0,其中参数0β_2β_1.当q∈(-∞,1)\{0}时,利用上下解方法研究非线性脉冲边值问题正解的存在性.     

On the Necessary and Sufficient Condition of Existence of Solution to Cauchy problem of a Class of Degenerate Equation

In this paper, we discuss the existence of the solution to the Cauchy problem: L_p~ku≡u_(xx)-x~(2k)u_(tt) Px~(k-1)u_t=f(x,t),t≥0, (1) (A_k) u(x,0)=ψ_1(x), u_t(x,0)=ψ_2(x), (2)where κ=2i 1, i=0,1,2,…,P R=(-∞, ∞), ψ_1(x),ψ_2(x)∈C~∞(R), f(x,t) ∈C~∞(R_2~ ),R_2~ ={(x, t)∈R~2|t≥0}.If κ=1, the uniqueness and existence of solution to the Cauchy problem(A_κ) was entirely solved by [1-3], if κ>1, A. Menikoff proved that the C~∞     

亚纯函数的级的估计

设f(z)为一亚纯函数,其级p< ∞。re~(iω_1),re~(iω_2),…,re~(iω_q)(r≥0)为q条射线,其中0≤ω_1<ω_2<…<ω_q<2π,q≥1。本文证明了若方程:f(z)=0,f(z)=∞,f~((l))(z)=1(l≥0,f~((0))≡f)的根均分布在包含上述q条射线的q个窄形区域中,又δ(0,f) δ(∞,f) δ(1,f~((l))>0,则     

1-Soliton solution and conservation laws for the Jaulent-Miodekequation with power law nonlinearity

This paper obtains the 1-soliton solution of the Jaulent-Miodek equation with power law nonlinearity. The solitary wave ansatz is used to obtain the soliton solution to this equation. Subsequently, the conserved quantities are computed using the invariance and multiplier approach based on the well known result that the Euler-Lagrange operator annihilates the total divergence.     

用试探方程法求Jaulent-Miodek方程的新的精确行波解

利用试探方程法将Jaulent-Miodek方程约化为初等积分的形式,进而求出了该方程的精确行波解,其中包括椭圆函数双周期解和有理函数解等新解.     

一个特征值问题的非线性化及其生成的经典可积系统

Under the Bargmann constrained condition, the spatial part of a new Lax pairof the higher order MkdV equation is nonlinearized to be a completely integrable system(R^2N,dp∧dq, H0=1/2F0)(F0=〈Aq,p〉 〈Ap, p〉 〈p,q〉^2). While the nonlinearization of the time part leads to its N-involutive system (Fm).     

A Half—Power Trace Formulas for the Generalized Jaulent—Miodek Equation

A new dispersive relation is found and a half-pow tormulas for the generalizeMiodek equation under the deeaying conditions at infinity are obtained.     

Jaulent-Miodek方程组和长水波近似方程组的新精确解

首先,利用直接代数法给出了一类非线性方程的四组显式精确解的公式.进而,很方便地得到了Jaulent-Miodek方程组和长水波近似方程组的若干新精确解.     

On the Involutive Solutions of Solition Hierarchy

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Super Jaulent-Miodek hierarchy and its super Hamiltonian structure,conservation laws and its self-consistent sources

A super Jaulent-Miodek hierarchy and its super Hamiltonian structures are constructed by means of a kind of Lie super algebras and super trace identity. Moreover, the self-consistent sources of the super Jaulent-Miodek hierarchy is presented based on the theory of self-consistent sources. Further- more, the infinite conservation laws of the super Jaulent-Miodek hierarchy are also obtained. It is worth noting that as even variables are boson variables, odd variables are fermi variables in the spectral problem, the commutator is different from the ordinary one.     

微分变换法求解二维非线性Volterra积分微分方程

为了解决二维非线性Volterra积分微分方程的求解问题,本文给出微分变换法.利用该方法将方程中的微分部分和积分部分进行变换,这样简化了原方程,进而得到非线性代数方程组,从而将原问题转换为求解非线性代数方程组的解,使得计算更简便.文中最后数值算例说明了该方法的可行性和有效性.     

The integrability and parametric representation of a hierarchy of soliton equations

In this paper after having obtained the Lax pair of a hierarchy of soliton equations,we discuss the parametric representation for finite-band solutions of the stationary solitonequation, and prove it can be represented as a Hamiltonian system which is integrable inLiouville sense. The nonconfocal involutive integral representations {Fm} are obtained also.In the condition of finite-band solutions of the soliton equation, the time and space can bedevided inio two Hamiltonian systems, so the fi…     

Convergence of the Neumann Series in BEM for the Neumann Problem of the Stokes System

A weak solution of the Neumann problem for the Stokes system in Sobolev space is studied in a bounded Lipschitz domain with connected boundary. A solution is looked for in the form of a hydrodynamical single layer potential. It leads to an integral equation on the boundary of the domain. Necessary and sufficient conditions for the solvability of the problem are given. Moreover, it is shown that we can obtain a solution of this integral equation using the successive approximation method. Then the consequences for the direct boundary integral equation method are treated. A solution of the Neumann problem for the Stokes system is the sum of the hydrodynamical single layer potential corresponding to the boundary condition and the hydrodynamical double layer potential corresponding to the trace of the velocity part of the solution. Using boundary behavior of potentials we get an integral equation on the boundary of the domain where the trace of the velocity part of the solution is unknown. It is shown that we can obtain a solution of this integral equation using the successive approximation method.