首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 31 毫秒
1.
We show that a velocity field u satisfying the stationary Navier–Stokes equations on the entire plane must be constant under the growth condition lim sup |x|α |u(x)| < ∞ as |x| → ∞ for some α ∈ [0, 1/7). Bibliography: 10 titles.  相似文献   

2.
The real-valued Lambert W-functions considered here are w 0(y) and w  − 1(y), solutions of we w  = y, − 1/e < y < 0, with values respectively in ( − 1,0) and ( − ∞ , − 1). A study is made of the numerical evaluation to high precision of these functions and of the integrals ò1 [-w0(-xe-x)]a x-bx\int_1^\infty [-w_0(-xe^{-x})]^\alpha x^{-\beta}\d x, α > 0, β ∈ ℝ, and ò01 [-w-1(-x e-x)]a x-bx\int_0^1 [-w_{-1}(-x e^{-x})]^\alpha x^{-\beta}\d x, α > − 1, β < 1. For the latter we use known integral representations and their evaluation by nonstandard Gaussian quadrature, if α ≠ β, and explicit formulae involving the trigamma function, if α = β.  相似文献   

3.
 We prove that for every ε>0 and positive integer r, there exists Δ00(ε) such that if Δ>Δ0 and n>n(Δ,ε,r) then there exists a packing of K n with ⌊(n−1)/Δ⌋ graphs, each having maximum degree at most Δ and girth at least r, where at most εn 2 edges are unpacked. This result is used to prove the following: Let f be an assignment of real numbers to the edges of a graph G. Let α(G,f) denote the maximum length of a monotone simple path of G with respect to f. Let α(G) be the minimum of α(G,f), ranging over all possible assignments. Now let αΔ be the maximum of α(G) ranging over all graphs with maximum degree at most Δ. We prove that Δ+1≥αΔ≥Δ(1−o(1)). This extends some results of Graham and Kleitman [6] and of Calderbank et al. [4] who considered α(K n ). Received: March 15, 1999?Final version received: October 22, 1999  相似文献   

4.
For a given contractionT in a Banach spaceX and 0<α<1, we define the contractionT α j=1 a j T j , where {a j } are the coefficients in the power series expansion (1-t)α=1-Σ j=1 a j t j in the open unit disk, which satisfya j >0 anda j >0 and Σ j=1 a j =1. The operator calculus justifies the notation(I−T) α :=I−T α (e.g., (I−T 1/2)2=I−T). A vectory∈X is called an, α-fractional coboundary for T if there is anx∈X such that(I−T) α x=y, i.e.,y is a coboundary forT α . The fractional Poisson equation forT is the Poisson equation forT α . We show that if(I−T)X is not closed, then(I−T) α X strictly contains(I−T)X (but has the same closure). ForT mean ergodic, we obtain a series solution (converging in norm) to the fractional Poisson equation. We prove thaty∈X is an α-fractional coboundary if and only if Σ k=1 T k y/k 1-α converges in norm, and conclude that lim n ‖(1/n 1-α k=1 n T k y‖=0 for suchy. For a Dunford-Schwartz operatorT onL 1 of a probability space, we consider also a.e. convergence. We prove that iff∈(I−T) α L 1 for some 0<α<1, then the one-sided Hilbert transform Σ k=1 T k f/k converges a.e. For 1<p<∞, we prove that iff∈(I−T) α L p with α>1−1/p=1/q, then Σ k=1 T k f/k 1/p converges a.e., and thus (1/n 1/p ) Σ k=1 n T k f converges a.e. to zero. Whenf∈(I−T) 1/q L p (the case α=1/q), we prove that (1/n 1/p (logn)1/q k=1 n T k f converges a.e. to zero.  相似文献   

5.
We show that there is a function α(r) such that for each constantr≧3, almost everyr-regular graph onn vertices has a hole (vertex induced cycle) of size at least α(r)n asn→∞. We also show that there is a function β(c) such that forc>0 large enough,G n, p ,p=c/n almost surely has a hole of size at least β(c)n asn→∞.  相似文献   

6.
We use a piecewise-linear, discontinuous Galerkin method for the time discretization of a fractional diffusion equation involving a parameter in the range − 1 < α < 0. Our analysis shows that, for a time interval (0,T) and a spatial domain Ω, the error in L((0,T);L2(W))L_\infty\bigr((0,T);L_2(\Omega)\bigr) is of order k 2 + α , where k denotes the maximum time step. Since derivatives of the solution may be singular at t = 0, our result requires the use of non-uniform time steps. In the limiting case α = 0 we recover the known O(k 2) convergence for the classical diffusion (heat) equation. We also consider a fully-discrete scheme that employs standard (continuous) piecewise-linear finite elements in space, and show that the additional error is of order h 2log(1/k). Numerical experiments indicate that our O(k 2 + α ) error bound is pessimistic. In practice, we observe O(k 2) convergence even for α close to − 1.  相似文献   

7.
In this paper we prove Harnack inequality for nonnegative functions which are harmonic with respect to random walks in ℝ d . We give several examples when the scale invariant Harnack inequality does not hold. For any α ∈ (0,2) we also prove the Harnack inequality for nonnegative harmonic functions with respect to a symmetric Lévy process in ℝ d with a Lévy density given by $c|x|^{-d-\alpha}1_{\{|x|\leq 1\}}+j(|x|)1_{\{|x|>1\}}$c|x|^{-d-\alpha}1_{\{|x|\leq 1\}}+j(|x|)1_{\{|x|>1\}}, where 0 ≤ j(r) ≤ cr  − d − α , ∀ r > 1, for some constant c. Finally, we establish the Harnack inequality for nonnegative harmonic functions with respect to a subordinate Brownian motion with subordinator with Laplace exponent ϕ(λ) = λ α/2ℓ(λ), λ > 0, where ℓ is a slowly varying function at infinity and α ∈ (0,2).  相似文献   

8.
In accordance with the demands of the so-called local approach to inverse problems, the set of “waves” uf (·, T) is studied, where uf (x,t) is the solution of the initial boundary-value problem utt−Δu=0 in Ω×(0,T), u|t<0=0, u|∂Ω×(0,T)=f, and the (singular) control f runs over the class L2((0,T); H−m (∂Ω)) (m>0). The following result is established. Let ΩT={x ∈ Ω : dist(x, ∂Ω)<T)} be a subdomain of Ω ⊂ ℝn (diam Ω<∞) filled with waves by a final instant of time t=T, let T*=inf{T : ΩT=Ω} be the time of filling the whole domain Ω. We introduce the notation Dm=Dom((−Δ)m/2), where (−Δ) is the Laplace operator, Dom(−Δ)=H2(Ω)∩H 0 1 (Ω);D−m=(Dm)′;D−mT)={y∈D−m:supp y ⋐ ΩT. If T<T., then the reachable set R m T ={ut(·, T): f ∈ L2((0,T), H−m (∂Ω))} (∀m>0), which is dense in D−mT), does not contain the class C 0 T). Examples of a ∈ C 0 , a ∈ R m T , are presented. Translated fromZapiski Nauchnykh Seminarov POMI, Vol. 210, 1994, pp. 7–21. Translated by T. N. Surkova.  相似文献   

9.
Summary Let {X n}n≧1 be a sequence of independent, identically distributed random variables. If the distribution function (d.f.) ofM n=max (X 1,…,X n), suitably normalized with attraction coefficients {αn}n≧1n>0) and {b n}n≧1, converges to a non-degenerate d.f.G(x), asn→∞, it is of interest to study the rate of convergence to that limit law and if the convergence is slow, to find other d.f.'s which better approximate the d.f. of(M n−bn)/an thanG(x), for moderaten. We thus consider differences of the formF n(anx+bn)−G(x), whereG(x) is a type I d.f. of largest values, i.e.,G(x)≡Λ(x)=exp (-exp(−x)), and show that for a broad class of d.f.'sF in the domain of attraction of Λ, there is a penultimate form of approximation which is a type II [Ф α(x)=exp (−x−α), x>0] or a type III [Ψ α(x)= exp (−(−x)α), x<0] d.f. of largest values, much closer toF n(anx+bn) than the ultimate itself.  相似文献   

10.
Let ξt be a regenerative process and assume that, at each state x, the process can fail with intensity α(x). If the inter-regeneration times have a finite exponential moment orinf xα(x)>0, then α(ξt) tends to some limiting positive intensity as t→∞ (under mild additional restrictions). This fact is widely used in engineering because the limiting intensity can be employed in various calculations, say, in reliability theory. The paper contains a variety of examples showing that α(ξt) provided that inter-regeneration time has no exponential moment andinf x α(x)=0. The speed of convergence depends, in general, on both the tail of inter-regeneration time and α(x). Proceedings of the Seminar on Stability Problems for Stochastic Models, Hajdúszoboszló, Hungary, 1997, Part III.  相似文献   

11.
In this paper, we study the asymptotic behavior of the Laguerre polynomials as n→∞. Here α n is a sequence of negative numbers and −α n /n tends to a limit A>1 as n→∞. An asymptotic expansion is obtained, which is uniformly valid in the upper half plane ℂ+={z:Im z≥0}. A corresponding expansion is also given for the lower half plane ℂ={z:Im z≤0}. The two expansions hold, in particular, in regions containing the curve Γ in the complex plane, on which these polynomials are orthogonal. Our method is based on the Riemann-Hilbert approach introduced by Deift and Zhou. The work of R. Wong is partially supported by a grant from the Research Grants Council of the Hong Kong Special Administrative Region, China (Project No. CityU 102504).  相似文献   

12.
The paper continues the studies of the well-known class T of typically real functions f(z) in the disk U = {z:|z| < 1}. The region of values of the system {f(z 0), f(z 0), f(r 1), f(r 2),…, f(r n )} in the class T is investigated. Here, z 0 ∈ U, Im z 0 ≠ 0, 0 < r j  < 1 for j = 1,…, n, n ≥ 2. As a corollary, the region of values of f′(z 0) in the class of functions fT with fixed values f(z 0) and f(r j ) (j = 1,…, n) is determined. The proof is based on the criterion of solvability of the power problem of moments. Bibliography: 10 titles. Translated from Zapiski Nauchnykh Seminarov POMI, Vol. 357, 2008, pp. 33–45.  相似文献   

13.
Explicit formulas are obtained for the maximum possible values of the derivatives f (k)(x), x ∈ (−1, 1), k ∈ {0, 1, ..., r − 1}, for functions f that vanish together with their (absolutely continuous) derivatives of order up to ≤ r − 1 at the points ±1 and are such that $ \left\| {f^{\left( r \right)} } \right\|_{L_2 ( - 1,1)} \leqslant 1 $ \left\| {f^{\left( r \right)} } \right\|_{L_2 ( - 1,1)} \leqslant 1 . As a corollary, it is shown that the first eigenvalue λ 1,r of the operator (−D 2) r with these boundary conditions is $ \sqrt 2 $ \sqrt 2 (2r)! (1 + O(1/r)), r → ∞.  相似文献   

14.
Let φ be a convex l.s.c. function fromH (Hilbert) into ] - ∞, ∞ ] andD(φ)={uH; φ(u)<+∞}. It is proved that for everyu 0D(φ) the equation − (du/dt)(t ∈ ∂φ(u(t)),u(0)=u 0 has a solution satisfying ÷(du(t)/dt)÷ ≦(c 1/t)+c 2. The behavior ofu(t) in the neighborhood oft=0 andt=+∞ as well as the inhomogeneous equation (du(t)/dt)+∂φ(u(t)) ∈f(t) are then studied. Solutions of some nonlinear boundary value problems are given as applications.   相似文献   

15.
It is proved that there is a positive function Φ(∈) defined for sufficiently small ∈>0 such that lim∈→0 Φ(∈)=0 and for every integerk and everyk-dimensionalP 1+∈ spaceE, d(E, l k )<1+Φ(∈). Author was partially supported by N.S.F. Grant MCS 79-03042. An erratum to this article is available at .  相似文献   

16.
The class Σb is defined to consist of meromorphic univalent functionsH omitting a disc with the radiusb:H(z)=z+ Σ 0 A n z n ,z>1,H(b)>b ∈ (0, 1). By aid of FitzGerald inequalities the inverse coefficients of odd Σb-functions are maximized. The result extends the corresponding estimation, due to Netanyahu and Schober, fromb=0 to the whole interval (0, 1). The author wishes to express her gratitude to Professor O. Tammi for valuable discussions connected with the problem. This work was supported by a grant from the Finnish Ministry of Education.  相似文献   

17.
In this paper we establish some oscillation or nonoscillation criteria for the second order half-linear differential equation
where (i) r,cC([t 0, ∞), ℝ := (− ∞, ∞)) and r(t) > 0 on [t 0, ∞) for some t 0 ⩾ 0; (ii) Φ(u) = |u|p−2 u for some fixed number p > 1. We also generalize some results of Hille-Wintner, Leighton and Willet.  相似文献   

18.
Consider the retarded difference equationx n −x n−1 =F(−f(x n )+g(x n−k )), wherek is a positive integer,F,f,g:R→R are continuous,F andf are increasing onR, anduF(u)>0 for allu≠0. We show that whenf(y)≥g(y) (resp. f(y)≤g(y)) foryR, every solution of (*) tends to either a constant or −∞ (resp. ∞) asn→∞. Furthermore, iff(y)≡g(y) foryR, then every solution of (*) tends to a constant asn→∞. Project supported by NNSF (19601016) of China and NSF (97-37-42) of Hunan  相似文献   

19.
In this paper, we are concerned with the existence of positive solutions for a singular p-Laplacian differential equation
(φp(u'))'+β/r φp(u')-γ |u'|^p/u + g(r)=0,0〈r〈1,
subject to the Dirichlet boundary conditions: u(0) = u(1) =0, where φp(s) = |sl^P-2s,p 〉 2,β 〉0, γ〉(p-1)/p (β + 1), and g(r) ∈ C^1 [0, 1] with g(r) 〉 0 for all τ ∈ [0, 1]. We use the method of elliptic regularization, by carrying out two limit processes, to get a positive solution.  相似文献   

20.
In this paper, we get the exact values of average σ-B width and infinite dimensional σ-G width of Sobolev class Br p(R) in the metric Lp(R) (1≤p≤∞) and obtain the exact (σ∈N) and strong asymptotic (σ>1) results of infinite dimensional σ-G widths of Sobolev-Wiener class Wr pq (R) in the metric Lq(R) and its dual case Wr p(R) in the metric Lqp(R) (1≤q≤p≤∞). Supported by the National Natural Science Foundation of China (No. 19671012) and by the Doctoral Programme Foundation of Institution of Higher Education of National Education Committee of China.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号