利用伪辛空间中的迷向点集构作结合方案

令Ｆｑ是ｑ个元的有限域，其中ｑ是一个２的方幂。在本文我们假设δ＝１或２。     

欧拉方程的Velicity表示和辛积分

1．引言在过去的十年中,oseledets,Sakdeer,Buttke以一个Buttke称为velicity的新变量独立地给出了不可压缩欧拉方程的新形式．本文的目的是分析velicity方程的类型：证明线性化的方程形成退化的一阶双典型拟微分系统,特征线是粒子路线．2．Velicity的描述首先概括Buttke的工作．参见Buttke＊．本文的定义与间相同．定义为Velicity为任意向量场M,它与速度场相关一个标量函数的梯度,即M二u＋W·因为u是不可压缩,所以V·。＝0可以通过求散度从M解得。7·M一凸吟所以有of二凸一‘｛7·M｝,u＝M－7凸一‘｛7·M｝．连续的velicity…     

变分与无限维系统的高精度辛格式

1.引 言 冯康和他的研究小组提出的生成函数法[1]系统地解决了象二体问题这样地有限维Hamil-ton系统辛算法的构造问题,该方法也可以自然地推广到无限维Hamilton系统[2].首先在空间方向进行离散,例如采用差分或谱离散,得到有限维Hamilton系统,然后再采用生成函数法离散该系统.这样得到的辛格式是整个一层的格式,对于研究格式的局部性质如多辛性质[3],局部能量守恒性质[5]就相当困难.     

四阶杆振动方程的两类高精度辛格式

In this paper, we present two classes of symplectic schemes with high order accuracy for solving four-order rod vibration equation utt uxxxx=0 via the third type generating function method. First, the equation of four order rod vibration is written into the canonical Hamilton system; second, overcoming successfully the essential difficult on the calculus of high order variations derivative, we get the semi-discretization with arbitrary order of accuracy in time direction for the PDEs by the third type generating function method. Furthermore the discretization of the related modified equation of original equation is obtained. Finally, arbitrary order accuracy symplectic schemes are obtained. Numerical results are also presented to show the effectiveness of the scheme, high order accuracy and properties of excellent long-time numerical behavior.     

带约束动力学辛算法的符号计算

首先对带约束动力学中的辛算法作了改进,利用吴消元法求解多项式类型Euler-Lagrange方程.在辛算法的基础上,根据线性方程组理论和相容条件提出了一个求解约束的新算法.新算法的推导过程比辛算法严格,而且计算也比辛算法简单,并且多项式类型的Euler-Lagrange仍可以用吴消元法求解.另外,对于某些非多项式类型的Euler-Lagrange方程,可以先化为多项式类型,再用吴消元法求解.利用符号计算软件,上述算法都可以在计算机上实现.     

用Hyperbolic函数构造Schrodinger方程的辛格式

本文利用Ｈｙｐｅｒｂｏｌｉｃ函数ｓｉｎｈ（ｘ）和ｔａｎｈ（ｘ）构造了Ｓｃｈｒｏｄｉｎｓｅｒ方程的任意阶的辛格式并讨论了它们的稳定性．     

Lp空间中重分算法的收敛性

§ 1　IntroductionThe nontrivial solution of the following refinement equation = αa(α)( 2 .-α) ( 1 )is called refinable.The sequence a is called the refinementmask.When the mask a is finite-ly supported on Zand αa(α) =2 ,itis well known thatthe refinementequation( 1 ) hasa unique compactly supported distribution solution satisfies^( 0 ) =1 ,where^denotes theFourier transform of.This solution is called the normalized solution of( 1 ) .In order to study the solution of the equ…     

A NOTE ON THE CONSTRUCTION OF SYMPLECTIC SCHEMES FOR SPLITABLE HAMILTONIAN H = H~((1)) H~((2)) H~((3))

For a hamiltonian systemwhere J = [ 2: ], It, is n x n identity matrix, H f R2n - R is a smooth function andl It, O I t It, is n x n identity matrix, H f R2n - R is a smooth function and7 is the gradiellt operator, the 8ymplectic difference schemes should…     

辛三代数的Frattini子代数

本文研究了辛三代数的Frattini子代数和基本辛三代数的问题.利用Frattini子代数和基本辛三代数的性质,得到了辛三代数的非嵌入定理,从而推广了李三系中关于Frattini子系的结果.     

利用伪辛空间中2维全迷向子空间构作结合方案与PBIB设计

取有限域Ｆｑ上２×２＋２维伪辛空间中２维全迷向子空间作为处理，构作了具有４个结合类和２个结合类的结合方案与ＰＢＩＢ设计，并且计算了它们的参数     

EQUIVALENCE OF SEMI-LAGRANGIAN AND LAGRANGE-GALERKIN SCHEMES UNDER CONSTANT ADVECTION SPEED

We compare in this paper two major implementations of large time-step schemes for advection equations, i.e., Semi-Lagrangian and Lagrange-Galerkin techniques. We show that SL schemes are equivalent to exact LG schemes via a suitable definition of the basis functions. In this paper, this equivalence will be proved assuming some simplifying hypoteses, mainly constant advection speed, uniform space grid, symmetry and translation invariance of the cardinal basis functions for interpolation. As a byproduct of this equivalence, we obtain a simpler proof of stability for SL schemes in the constant-coefficient case.     

A NOTE ON CONSTRUCTION OF HIGHER-ORDER SYMPLECTIC SCHEMES FROM LOWER-ORDER ONE VIAFORMAL ENERGIES

1.IntroductionFirstofall,let'srecallthedefinitionsofsymplecticschemes,revertibleschemes,andFeng'swayofconstructionofsymplecticmethodsviageneratingfunctions.Aswell-known,thephaseflow{g',tER}ofanyHamiltoniansystem(whereJ~I--i:n1,H:RZn-- RIisasmoothfunc...     

利用射影平面中的二次曲线构作结合方案

设C是射影平面H=PG(2,Fq)中的一条二次曲线.把H看作射影空间PG(3,Fq)的无穷远超平面,那么H在PG(3,Fq)中的补空间是仿射空间X=AG(3,Fq).我们把H上的点集划分为2个或3个子集的并.设a≠b∈X.若线ab与H的交点属于第i个集合,定义a和b属于第i个结合类.我们证明上述构作是结合方案.最后,把H的某一点集作为处理集,构作出结合方案.     

SYMPLECTIC SCHEMES FOR QUASILINEAR WAVE EQUATIONS OF KLEIN-GORDON AND SINE-GORDON TYPE

1. IntroductionThere has been much discussion recently aboat deswi symplectic numrical schemesfor both finite and idste dimensional Hamilonian systems ([1] - [8]). A dass of syInPlecticsMes for linear wav equations has been sUggested [1], and numerical exPerimellt8 for tlieseschemes have been conducted [8, 9]. Results shOw that the syInPlectic method8 are inhereotlyfree from arttheial dissipatinn and all kinds of nonHtalltoulan pollutions, and are thu8 Of highquality and resolution.In thi…     

ASYMPTOTIC DECAY TOWARD RAREFACTION WAVE FOR A HYPERBOLIC-ELLIPTIC COUPLED SYSTEM ON HALF SPACE

We consider the asymptotic behavior of solutions to a model of hyperbolicelliptic coupled system on the half-line R＋ = （0, ∞）,with the Dirichlet boundary condition u（0, t） = 0. S. Kawashima and Y. Tanaka [Kyushu J. Math., 58（2004）, 211-250] have shown that the solution to the corresponding Cauchy problem behaviors like rarefaction waves and obtained its convergence rate when u_ u＋. Our main concern in this paper is the boundary effect. In the case of null-Dirichlet boundary condition on u, asymptotic behavior of the solution （u, q） is proved to be rarefaction wave as t tends to infinity. Its convergence rate is also obtained by the standard L2-energy method and Ll-estimate. It decays much lower than that of the corresponding Cauchy problem.     

A HIERARCHY OF INTEGRABLE LATTICE SOLITON EQUMIONS AND ITS INTEGRABLE SYMPLECTIC MAP

1TheLatticeSolitonHierarchyDenoteEf(n)-f(n 1),nEZ,andwritef(n)=f,f(n k)=E*f.Considerthediscrete3x3matrixspectralproblem:whereajb,carethreepotentials,Aisaconstantspectralparameter.Theadjointrepresentationequationof(1)iswhereeachentryVj=Kj(B(A),C(A),D(A))0fthe3x3matrixVisaLaurentexpansionofA:Then(2)isequivaentt0'therecursi0nrelations:,Theaboverecursionequationscanbesolvedsuccessivelyt0deducethefollowingresults:Wedefine{Dj}bythefollowingrelation:From(3)we0btainKGj-1=JGj,Gj=(Aj,Bj,Cj…     

特殊二阶微分方程的线性自治系统的辛多步法

１．引言１９世纪Ｈａｍｉｌｔｏｎ提出经典力学的一种基本的方程形式．记Ｐ＝Ｍｑ表示动量,ｑ表示位移,于是动能Ｔ＝１／２（ｐ,Ｍ－１　ｐ）,并将总能量Ｈ＝Ｔ＋Ｖ位能）表示为ｐ,ｑ的函数：于是经典力学的标准形式－Ｎｅｗｔｏｎ形式称为Ｈａｍｉｌｔｏｎ正则方程．（１．１）是ＺＩ维相空间或称辛空间中的相变量（ＰＩ,...,Ｐ。,ｑｌ;...,ｑｎ）'的一阶微分方程组．其中ｑ-（ｑｌ,...;ｑｒｔ）'是位置向量,ｄｑ,、Ｉ。。。。。ｑ＝ｉ＝（ｑｌ,...,ｑｈ）'是速度向量,ｄｔ'"""。'。'。。。ｌ、。。ｄ"ｑ,...．、,-,-…     

VON NEUMANN STABILITY ANALYSIS OF SYMPLECTIC INTEGRATORS APPLIED TO HAMILTONIAN PDEs

Symplectic integration of separable Hamiltonian ordinary and partial differential equations is discussed. A von Neumann analysis is performed to achieve general linear stability criteria for symplectic methods applied to a restricted class of Hamiltonian PDEs. In this treatment, the symplectic step is performed prior to the spatial step, as opposed to the standard approach of spatially discretising the PDE to form a system of Hamiltonian ODEs to which a symplectic integrator can be applied. In this way stability criteria are achieved by considering the spectra of linearised Hamiltonian PDEs rather than spatial step size.     

复二维空间形式中曲率椭圆是圆的辛临界曲面（英文）

本文研究了复二维空间形式中曲率椭圆是圆的辛临界曲面.利用活动标架法,获得了这类曲面是极小曲面的结果,丰富了辛临界曲面的内容.     

辛RK型方法的形式能量

引言 自从冯康先生创立哈密尔顿系统的辛算法后,为数众多且多种多样的保结构算法已经被提了出来［１－４］．哈密尔顿系统的能量Ｈ（ｚ）也是系统的不变量,但一般情况下,没有任何一个辛格式能够保持所有原始哈密尔顿能量［５,６］．另一方面,任何辛格式都保持一个形式哈密尔顿能量,它随格式本身的精度逼近原始哈密尔顿能量．关于形式能量的计算有多种途径,如冯康先生通过生成函数的微积分技巧在理论上得到了构造有生成函数确定的辛差分格式的形式能量的完整方法．Ｙｏｓｈ［１１］利用 Ｌｉｅ级数的 ＢＣＨ公式确定了可分哈密尔顿系…