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。     

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.     

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…     

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     

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.     

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...     

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…     

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…     

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.     

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.     

ON THE CONVERGENCE OF IMPLICIT DIFFERENCE SCHEMES FOR HYPERBOLIC CONSERVATION LAWS

1. IntroductionWe are are interested in the fOllowing Cauchy problem for scalar conservation lawswhere the initial data uo E BV(R) and the flux function f 6 C'(n).It is well known that this problem may not always have a smooth global solution even ifthe i…     

ON ENTROPY CONDITIONS OF HIGH RESOLUTION SCHEMES FOR SCALAR CONSERVATION LAWS

1. IntroductionLet us consider the Cauchy problems for nonlinear hroerbolic scalar cO~ion laws:where the function f(u) E C'(R) and the hatal data ho E BV(R). As is well lmown, thisProblem in general does not ~ smooth solution, so that weak solution in the sense ofdistributions must be considered. Moreover, an elitropy condition must be added in order toensure the ~s of the weak solutions.The research of numerical methods for solving the equation (1.1) has been developed rapidlyin this deca…     

李群的余切丛上的两种辛群胚结构

本文研究了李群的余切丛上的辛群胚结构.利用李代数胚的对偶丛上有自然诱导的泊松结构,.构造出了同一余切丛上的不同的辛群胚结构,推广了辛群胚的性质.     

A ESTIMATE OF THE RATE OF ENTROPY DISSIPATION OF HIGH RESOLUTION MUSCL TYPE GODUNOV SCHEMES

1.IntroductionLetusconsidertheCauchyproblemsfornonlinearhyperbolicscalarconservationlaws:wheref:W~WisLipschitzcontinuousfunctions,andtheinitialdata"o(x)isagivenfunctioninLI(R)nLoo(R).Asitiswell--known,thisproblemingeneraldoesnotadmitsmoothsolution,so...     

A NUMERICAL BOUNDARY EIGENVALUE PROBLEM FOR ELASTIC CRACKS IN FREE AND HALF SPACE

We present in this paper a numerical method for hypersingular boundary integral equations.This method was developed for planar crack problems:additional edge si...     

TWO-GRID DISCRETIZATION SCHEMES OF THE NONCONFORMING FEM FOR EIGENVALUE PROBLEMS

This paper extends the two-grid discretization scheme of the conforming finite elements proposed by Xu and Zhou （Math. Comput., 70 （2001）, pp.17-25） to the nonconforming finite elements for eigenvalue problems. In particular, two two-grid discretization schemes based on Rayleigh quotient technique are proposed. By using these new schemes, the solution of an eigenvalue problem on a fine mesh is reduced to that on a much coarser mesh together with the solution of a linear algebraic system on the fine mesh. The resulting solution still maintains an asymptotically optimal accuracy. Comparing with the two-grid discretization scheme of the conforming finite elements, the main advantages of our new schemes are twofold when the mesh size is small enough. First, the lower bounds of the exact eigenvalues in our two-grid discretization schemes can be obtained. Second, the first eigenvalue given by the new schemes has much better accuracy than that obtained by solving the eigenvalue problems on the fine mesh directly.