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1.
Let Im(v) denote the set of integers k for which a pair of m-cycle systems of Kv, exist, on the same vertex set, having k common cycles. Let Jm(v) = {0, 1, 2,…, tv ?2, tv} where tv = v(v ? 1)/2m. In this article, if 2mn + x is an admissible order of an m-cycle system, we investigate when Im(2mn + x) = Jm(2mn + x), for both m even and m odd. Results include Jm(2mn + 1) = Im(2mn + 1) for all n > 1 if m is even, and for all n > 2 if n is odd. Moreover, the intersection problem for even cycle systems is completely solved for an equivalence class x (mod 2m) once it is solved for the smallest in that equivalence class and for K2m+1. For odd cycle systems, results are similar, although generally the two smallest values in each equivalence class need to be solved. We also completely solve the intersection problem for m = 4, 6, 7, 8, and 9. (The cased m = 5 was done by C-M. K. Fu in 1987.) © 1993 John Wiley & Sons, Inc.  相似文献   

2.
We derive leading terms in the expansion of ratios of the formB n+α(nβ)/Bn(nβ) for largen, whereB n(x) is any one of the Bessel functionsJ n(x), Yn(x), Hn(x),I n(x) andK n(x).  相似文献   

3.
Some monotonicity results are given for the remainder terms in the asymptotic expansion for x → ∞ of the function Jv(x)Jv+n(x) + Yv(x Yv+n(x), v ε R, n ε Z.  相似文献   

4.
The inverse scattering method is used to determine the distribution limit as ? → 0 of the solution u(x, t, ?) of the initial value problem. Ut ? 6uux + ?2uxxx = 0, u(x, 0) = v(x), where v(x) is a positive bump which decays sufficiently fast as x x→±α. The case v(x) ? 0 has been solved by Peter D. Lax and C. David Levermore [8], [9], [10]. The computation of the distribution limit of u(x, t, ?) as ? → 0 is reduced to a quadratic maximization problem, which is then solved.  相似文献   

5.
该文证明:和如下耦合色散系统相联系的初值问题的充分光滑的解$(u,v)=(u(x,t),v(x,t))$, 如果在两个时刻有半线支集那么它们全为零. {∂ tu+∂3x u+∂ x(up vp+1)=0, ∂ tv+∂3x v+∂x(up+1vp)=0,x∈R,t≥ 0  相似文献   

6.
This paper is concerned with the following periodic Hamiltonian elliptic system
{l-Du+V(x)u=g(x,v) in  \mathbbRN,-Dv+V(x)v=f(x,u) in  \mathbbRN,u(x)? 0 and v(x)?0 as  |x|?¥,\left \{\begin{array}{l}-\Delta u+V(x)u=g(x,v)\, {\rm in }\,\mathbb{R}^N,\\-\Delta v+V(x)v=f(x,u)\, {\rm in }\, \mathbb{R}^N,\\ u(x)\to 0\, {\rm and}\,v(x)\to0\, {\rm as }\,|x|\to\infty,\end{array}\right.  相似文献   

7.
For an integer i, a graph is called an Li-graph if, for each triple of vertices u, v, w with d(u, v) = 2 and w (element of) N(u) (intersection) N(v), d(u) + d(v) ≥ | N(u) (union) N(v) (union) N(w)| —i. Asratian and Khachatrian proved that connected Lo-graphs of order at least 3 are hamiltonian, thus improving Ore's Theorem. All K1,3-free graphs are L1-graphs, whence recognizing hamiltonian L1-graphs is an NP-complete problem. The following results about L1-graphs, unifying known results of Ore-type and known results on K1,3-free graphs, are obtained. Set K = lcub;G|Kp,p+1 (contained within) G (contained within) Kp V Kp+1 for some ρ ≥ } (v denotes join). If G is a 2-connected L1-graph, then G is 1-tough unless G (element of) K. Furthermore, if G is as connected L1-graph of order at least 3 such that |N(u) (intersection) N(v)| ≥ 2 for every pair of vertices u, v with d(u, v) = 2, then G is hamiltonian unless G ϵ K, and every pair of vertices x, y with d(x, y) ≥ 3 is connected by a Hamilton path. This result implies that of Asratian and Khachatrian. Finally, if G is a connected L1-graph of even order, then G has a perfect matching. © 1996 John Wiley & Sons, Inc.  相似文献   

8.
We study the p-system with viscosity given by vt ? ux = 0, ut + p(v)x = (k(v)ux)x + f(∫ vdx, t), with the initial and the boundary conditions (v(x, 0), u(x,0)) = (v0, u0(x)), u(0,t) = u(X,t) = 0. To describe the motion of the fluid more realistically, many equations of state, namely the function p(v) have been proposed. In this paper, we adopt Planck's equation, which is defined only for v > b(> 0) and not a monotonic function of v, and prove the global existence of the smooth solution. The essential point of the proof is to obtain the bound of v of the form b < h(T) ? v(x, t) ? H(T) < ∞ for some constants h(T) and H(T).  相似文献   

9.
We study the large–time behavior of the second moment (energy) for the flow of a gas in a N-dimensional porous medium with initial density v0(x) 0. The density v(x, t) satisfies the nonlinear degenerate parabolic equation vt = vm where m > 1 is a physical constant. Assuming that for some > 0, we prove that E(t) behaves asymptotically, as t , like the energy EB(t) of the Barenblatt-Pattle solution B(|x|, t). This is shown by proving that E(t)/EB(t) converges to 1 at the (optimal) rate t–2/(N(m-1)+2). A simple corollary of this result is a central limit theorem for the scaled solution E(t)N/2v(E(t)1/2x, t).  相似文献   

10.
Bounds uniform in the real argument and the index for the functionsa ν (x)=xI′ ν (x)/I′ ν (x) andb ν (x)=xK′ ν (x)/K ν (x), as well as for the modified Bessel functionsI ν(x) andK ν(x), are established in the quadrantx>0, ν≥0, except for some neighborhoods of the pointx=0, ν=0. Translated fromMatematicheskie Zametki, Vol. 65, No. 5, pp. 681–692, May, 1999.  相似文献   

11.
12.
Let (K, v) be a perfect rank one valued field and let ([`(Kv)],[`(v)]){(\overline{K_{v}},\overline{v})} be the canonical valued field obtained from (K, v) by the unique extension of the valuation [(v)\tilde]{\widetilde{v}} of K v , the completion of K relative to v, to a fixed algebraic closure [`(Kv)]{\overline{K_{v}}} of K v . Let [`(K)]{\overline{K}} be the algebraic closure of K in [`(Kv)]{\overline {K_{v}}}. An algebraic extension L of K, L ì [`(K)]{L\subset\overline{K}}, is said to be a v-adic maximal extension, if [`(v)] | L{\overline{v}\mid_{L}} is the only extension of v to L and L is maximal with this property. In this paper we describe some basic properties of such extensions and we consider them in connection with the v-adic spectral norm on [`(K)]{\overline{K}} and with the absolute Galois groups Gal([`(K)]/K){(\overline{K}/K)} and Gal([`(Kv)] /Kv){(\overline{K_{v}} /K_{v})}. Some other auxiliary results are given, which may be useful for other purposes.  相似文献   

13.
Convergence results for interpolatory product rules for evaluating Cauchy principal value integrals of the form f ?1 1 v(x)f(x)/x ? λ dx wherev is an admissible weight function have been extended to integrals of the form f ?1 1 k(x)f(x)/x ? λ dx wherek is an arbitrary integrable function subject to certain conditions. Further, whereas the above convergence results were shown when the interpolation points were the Gauss points with respect to some admissible weight functionw, they are now shown to hold when the interpolation points are Radau or Lobatto points with respect tow.  相似文献   

14.
This paper considers the solution of the problem: inff[y, x(y)] s.t.y [y, x(y)] E k , wherex(y) solves: minF(x, y) s.t.x R(x, y) E n . In order to obtain local solutions, a first-order algorithm, which uses {dx(y)/dy} for solving a special case of the implicitly definedy-problem, is given. The derivative is obtained from {dx(y, r)/dy}, wherer is a penalty function parameter and {x(y, r)} are approximations to the solution of thex-problem given by a sequential minimization algorithm. Conditions are stated under whichx(y, r) and {dx(y, r)/dy} exist. The computation of {dx(y, r)/dy} requires the availability of y F(x, y) and the partial derivatives of the other functions defining the setR(x, y) with respect to the parametersy.Research sponsored by National Science Foundation Grant ECS-8709795 and Office of Naval Research Contract N00014-89-J-1537. We thank the referees for constructive comments on an earlier version of this paper.  相似文献   

15.
In this paper, in the setting of sequential spaces, we consider the value functions vS and vI defined by vS(x)=supyK(x)f(x,y) and vI(x)=infyK(x)f(x,y), and we introduce sufficient conditions on the value functions and on the data, weaker than upper semicontinuity, which guarantee the existence of maximum for such functions. Various examples illustrate the results and the connections with previous results.  相似文献   

16.
For a monomial ideal IS = K[x 1...,x n ], we show that sdepth(S/I) ≥ ng(I), where g(I) is the number of the minimal monomial generators of I. If I =νI′, where νS is a monomial, then we see that sdepth(S/I) = sdepth(S/I′). We prove that if I is a monomial ideal IS minimally generated by three monomials, then I and S/I satisfy the Stanley conjecture. Given a saturated monomial ideal IK[x 1,x 2,x 3] we show that sdepth(I) = 2. As a consequence, sdepth(I) ≥ sdepth(K[x 1,x 2,x 3]//I) +1 for any monomial ideal in IK[x 1,x 2,x 3].  相似文献   

17.
This paper gives conditions ensuring the existence for an initial value (x 0,v 0) of a solution to the second order differential inclusionx″(t) ∈F[x(t),x′(t)],x(0)=x 0,x′(0)=v 0 such thatx(t)K for allt whereK is a nonempty given subset ofR n .   相似文献   

18.
The main results in this paper are, the characterization of all the σfinite positive measures μ and v, for which K(L1(μ, L1(v)) proximinal in K(L1(μ, L1(v)) all the a-finite positive measures fi and v, for which K(L(μ), L(v)) is proximinal in L(Lμ)), Lv(v)) and all the compact Hausdorff spaces Q, for which K(C(Q), L(μ)) is proximinal in L(C(Q), :(μ))  相似文献   

19.
We present various new inequalities involving the logarithmic mean L(x,y)=(x-y)/(logx-logy) L(x,y)=(x-y)/(\log{x}-\log{y}) , the identric mean I(x,y)=(1/e)(xx/yy)1/(x-y) I(x,y)=(1/e)(x^x/y^y)^{1/(x-y)} , and the classical arithmetic and geometric means, A(x,y)=(x+y)/2 A(x,y)=(x+y)/2 and G(x,y)=?{xy} G(x,y)=\sqrt{xy} . In particular, we prove the following conjecture, which was published in 1986 in this journal. If Mr(x,y) = (xr/2+yr/2)1/r(r 1 0) M_r(x,y)= (x^r/2+y^r/2)^{1/r}(r\neq{0}) denotes the power mean of order r, then $ M_c(x,y)<\frac{1}{2}(L(x,y)+I(x,y)) {(x,y>0,\, x\neq{y})} $ M_c(x,y)<\frac{1}{2}(L(x,y)+I(x,y)) {(x,y>0,\, x\neq{y})} with the best possible parameter c=(log2)/(1+log2) c=(\log{2})/(1+\log{2}) .  相似文献   

20.
We present a class of functions gK(w), K ≥ 2, for which the recursive sequences wn + 1 = gK(wn) converge to N1/v with relative error . Newton's method results when K = 2. The coefficients of the gK(w) form a triangle, which is Pascal's for v = 2. In this case, if w1 = x1/y1, where x1, y1 is the first positive solution of Pell's equation x2 ? Ny2 = 1, then wn + 1 = xn + 1/yn + 1 is the Knpth or 2Knpth convergent of the continued fraction for , its period p being even or odd.  相似文献   

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