三维不可压Navier-Stokes方程关于速度场单分量在各向异性临界空间中的正则性准则 献给杨乐教授80华诞

给定初始涡度场ω_0属于L~(3/2)∩L~2,本文证明若三维不可压Navier-Stokes方程的Fujita-Kato解在有限时刻T~?处发生爆破,则对任意p∈[4,∞], q_1∈[1, 2],μ 0, q_2∈[2,(1/p+μ)~(-1)],κ∈[1,∞],以及任意单位向量e,(v(t)|e)_(R~3)的■范数等于无穷.     

若干图的广义Mycielski图的边色数

设图G(V,E)为简单图,V(Mn(G))={v01,v02,…,v0p;v11,v12,…,v1p;…,vn1,vn2,…,vnp}EMn(G))=E(G)∪vijv(i+1)kv0 jv0k∈E(G),1 j,k p,i=0,1,…,n-1称Mn(G)为G的n串广义M ycielsk i图,其中n为自然数,V(G)={v01,v02,…,v0p}.本文得到了路、圈、扇、轮、星图的广义M ycielsk i图的边色数.     

一类N维非线性波动方程的Cauchy问题

证明下列非线性波动方程的Cauchy问题v_(tt)-α△v_(tt)-Δv=g(v)-αΔg(v),x∈R~N,t>0,(1)v(x,0)=v_0(x),v_t(x,0)=v_1(x),x∈R~N(2)在空间C~2([0,∞);H~s(R~N))(s>N/2)中存在唯一整体广义解v和在空间C~2([0,∞);H~s(R~N))(s>2+N/2N)中存在唯一整体古典解v,即u∈C~2([0,∞);C_B~2(R~N)).还证明Cauchy问题(1),(2)在C~3([0,∞);W~(m,p)(R~N)∩L~∞(R~N))(m≥0,1≤p≤∞)中有唯一整体广义解v和在C~3([0,∞);W~(m,p)(R~N)∩L~∞(R~N))(m>2+N/P)中有唯一整体古典解v,即v∈C~3([0,∞);C~2(R~N)∩L~∞(R~N)).     

关于“具人工粘性项的2守恒律组的有限差分格式”一文的注记

In [ 2 ], D.Hoff analyzes an implicit finite difference scheme for the mixed initial -value Dirichlet problem for a system of two conservation laws with artif ficial viscosity . The system is a model for isentropic flow in one space dimen-sion .However, in [2], there is an additional condition on the state function p(v),(?)For polytropic gas, p(v) = k²v^-γ, where k>0 and 1<γ≤3,the condition (*) is equivalent to 1<γ<2. In the present note, we remove the restriction(*),so that the main results of [2] still hold for the general state function p(v) with p′(v)<0, p″(v)>0.     

M.Riesz定理的注记

设u(z)是单位圆内的实值调和函数 ,若 p_平均Mp(r ,u) =12π∫2π0｜u(reiθ) ｜pdθ1 p <∞ ,则称u(z) ∈hp( 1

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轮图的广义Mycielski图的邻强边色数

设图 G(V,E)为简单图 ,V(Mn(G) ) |{ v0 1,v0 2 ,… ,v0 p;v11,v12 ,… ,v1p,… ,vn1,vn2 ,… ,vnp}E(Mn(G) ) =E(G)∪ { vijv(i+ 1) k|v0 jv0 k ∈ E(G) ,1≤ j,k≤ p ,i =0 ,1,… ,n - 1}称 Mn(G)为 G的 n广义 Mycielski图 ,n为自然数 .本文得到了轮的广义 Mycielski图的临强边色数 .     

一类Boussinesq方程的整体解的存在性与不存在性

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The Aysmptotic Behavior of Solution to a Class of Inhomogeneons Systems of Gas Dynamics

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半导体器件数值模拟的块中心差分法

此处(1.1)～(1.3)分别是电位势方程,电子浓度(e)和空穴浓度(p)方程,其中α是由介电常数和电子电荷决定的正常数,N(x)表示掺杂分布,r,r_p是正常数,μ(x),μ_p(x)表示迁移率,R(e,p)=(ep—1)/(e+p+2)表示电子和空穴的产生复合率,△是拉普拉斯算子,是梯度算子,v是区域Ω边界Ω的外法线方向,p_0(x),e_0(x)是已知的初始浓度函数。     

Cohomology of the moduli of parabolic vector bundles

The purpose of this paper is to compute the Betti numbers of the moduli space ofparabolic vector bundles on a curve (see Seshadri [7], [8] and Mehta & Seshadri [4]), in the case where every semi-stable parabolic bundle is necessarily stable. We do this by generalizing the method of Atiyah and Bott [1] in the case of moduli of ordinary vector bundles. Recall that (see Seshadri [7]) the underlying topological space of the moduli of parabolic vector bundles is the space of equivalence classes of certain unitary representations of a discrete subgroup Γ which is a lattice in PSL (2,R). (The lattice Γ need not necessarily be co-compact). While the structure of the proof is essentially the same as that of Atiyah and Bott, there are some difficulties of a technical nature in the parabolic case. For instance the Harder-Narasimhan stratification has to be further refined in order to get the connected strata. These connected strata turn out to have different codimensions even when they are part of the same Harder-Narasimhan strata. If in addition to ‘stable = semistable’ the rank and degree are coprime, then the moduli space turns out to be torsion-free in its cohomology. The arrangement of the paper is as follows. In § 1 we prove the necessary basic results about algebraic families of parabolic bundles. These are generalizations of the corresponding results proved by Shatz [9]. Following this, in § 2 we generalize the analytical part of the argument of Atiyah and Bott (§ 14 of [1]). Finally in § 3 we show how to obtain an inductive formula for the Betti numbers of the moduli space. We illustrate our method by computing explicitly the Betti numbers in the special case of rank = 2, and one parabolic point.     

Levinson定理证明的一些简化

<正> (一)1974年,Levinson N.证明了他的关于Riemann ζ-函数在直线σ=1/2上的零点个数的著名定理:对充分大的T有     

一维绝热流动中初等波的相互作用

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On Campedelli branch loci

We construct new degree ten plane curves having six [3, 3] points that do not belong to a conic and degree ten plane curves with five [3, 3] points and a quadruple point, having the six singularities that again do not lie on a conic. In the second family we find an irriducible curve.

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Sunto Si costruiscono nuove curve piane di ordine dieci dotate di sei punti [3, 3] che non giacciono su una conica e curve di ordine dieci dotate di cinque punti [3, 3] e di un punto quadruplo ancora non giacenti su una conica. Nella seconda famiglia si è presentata una curva irriducibile.

     

Character tables of commutative hecke algebras associated with exceptional weyl groups

The purpose of this paper is to calculate all the character tables of Hecke algebras associated with exceptional Weyl groups and their maximal parabolic subgroups when they are commutative. In the case when Weyl groups are of classical type, they are already known in [D.1] and [D.2]. In §1, we discuss the structure of Hecke algebras and in §2, we calculate all the character tables of these commutative Hecke algebras associated with exceptional Weyl groups.     

Shape control of curve design by weighted rational spline

Controlling the convexity and the strain energy of the interpolating curve can be carried out by controlling the second-order derivative of the interpolating function. In [1], the rational cubic spline with linear denominator has been used to constrain the convexity and the strain energy of the interpolating curves, but it does not work in some case. This paper deals with the weighted rational cubic spline with linear denominator for this kind of constraint, the sufficient and necessary condition for controlling the convexity and strain energy of the interpolating curves are derived, and a numerical example is given.     

关于三次Bézier曲线的凸性

苏步青在[1]中研究了Bezier曲线的仿射不变量与Bezier多边形之间的关系,并利用这些不变量对三次Bezier曲线不存在拐点和二重点的条件进行了讨论,但所得条件还不是充分必要条件.为了弥补[1]中这个不足之处,我们在这里给出一个补充,从而完善了这套条件.为了节省篇幅,我们沿用[1]中的记号而不再另外说明.     

Special Pair of Dual Parametric Nonlinear Optimization Problems with Common Set of Optimal Points

On the base of a given strictly convex function defined on the Euclidean space E n ( n S 2) we can-without the assumption that it is differentiable - introduce some manifolds in topologic sense. Such manifolds are sets of all optimal points of a certain parametric non-linear optimization problem. This paper presents above all certain generalization of some results of [F. No ? i ) ka and L. Grygarová (1991). Some topological questions connected with strictly convex functions. Optimization , 22 , 177-191. Akademie Verlag, Berlin] and [L. Grygarová (1988). Über Lösungsmengen spezieller konvexer parametrischer Optimierungsaufgaben . Optimization 19 , 215-228. Akademie Verlag Berlin], under less strict assumptions. The main results are presented in Sections 3 and 4, in Section 3 the geometrical characterization of the set of optimal points of a certain parametric minimization problem is presented; in Section 4 we study a maximization non-linear parametric problem assigned to it. It seems that it is a certain pair of parametric optimization problems with the same set of their optimal points, so that this pair of problems can be denoted as a pair of dual parametric non-linear optimization problems. This paper presents, most of all in Section 2, a number of interesting geometric facts about strictly convex functions. From the point of view of non-smooth analysis the present article is a certain complement to Chapter 4.3 of the book [B. Bank, J. Guddat, D. Klatte, B. Kummer and K. Tammer (1982). Nonlinear Parametric Optimization . Akademie Verlag, Berlin] where a convex parametric minimization problem is considered under more general and stronger conditions (but without any assumptions concerning strict convexity and without geometrical aspects).     

Remarks on time map for quasilinear equations

We present two different generalizations of R. Schaaf's (1990) [18] time map formula to quasilinear equations, including the case of p-Laplacian. We give conditions for monotonicity and for convexity of the time map, which imply uniqueness or multiplicity results for the corresponding Dirichlet boundary value problem. Our time map formulas can be also used for effective computations of the global solution curves.