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1.
Necessary conditions are obtained for the existence of a 2 – (v, k, ) design, for which the block intersection sizess 1,s 2, ...,s n satisfys 1 s 2 ... s n s (mod 2 e ), wheree is odd. These conditions are obtained by combining restrictions on the Smith Normal Form of the incidence matrix of the design with some well known properties of self-orthogonal binary codes with all weights divisible by 4.Research done at AT&T Bell Laboratories.  相似文献   

2.
Vakarchuk  S. B. 《Mathematical Notes》2002,72(5-6):615-619
In the Hardy space H p, (p1, 0< 1, H p,1 H p) we develop best linear approximation methods (previously studied by Taikov and Ainulloev) for the classes W(r,,) of analytic functions on the unit disk and calculate the exact values of linear, Gelfand, and informational n-widths of these classes.  相似文献   

3.
Let 1, 2, ... be a sequence of i.i.d. random variables with positive mean and finite variance and letr(b), b0, be real numbers tending to 0 asb . Definings n=1+...+n andS n=Sn(b)=sn+r(b)n, the stopping time =(b)=inf {n>/1:Sn >b} whereb=b(b) , will be considered with special regard to the excess over the boundaryR b=s+r(b)–b. It turns out that the limiting distribution ofR b is the same as in the caser(b)0 for allb. Proving this, Blackwell's renewal theorem and its integral version have to be established first in the above stated situation. Finally, an expansion ofE to vanishing terms asb will be provided and applied to some examples arising in economics.
Zusammenfassung Seien 1, 2, ... unabhängige identisch verteilte Zufallsgrößen mit positivem Erwartungswert und endlicher Varianz sowier(b), b0, reelle Zahlen mitr(b)0 für b. Sei ferners 1, s2, ... der zugehörige Summenprozeß,S n= Sn(b)=sn+r(b)n fürn1 und =(b)=inf {n1: Sn>b, wobeib=b(b) fürb . Es wird gezeigt, daß die asymptotische Verteilung des ExzessesR b=s +r(b)b mit der im Fallr(·)0 übereinstimmt. Dazu werden sowohl das Blackwellsche Erneuerungstheorem als auch seine Integralversion in der vorher beschriebenen parameterabhängigen Situation geeignet formuliert und bewiesen. Als Folgerung ergibt sich dann eine asymptotische Entwicklung vonE(b) fürb bis zu Termen o(1). Anh- and einiger Beispiele aus dem ökonomischen Bereich wird schließlich noch aufgezeigt, wo Approximationen fürE(b) von Interesse sein können.
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4.
Résumé Soit (V )0 une résolvante définie sur un espace mesurable telle que le noyau initial est borné; on trouve une condition nécéssaire et suffisante pour qu'un noyau borné U possède une résolvante (U )0 telle que U V pour tout 0. On donne plusieurs applications de ce résultat.  相似文献   

5.
Let a convex bodyAE n be covered bys smaller homothetic copies with coefficients 1, ..., s , respectively. It is conjectured that 1 + ...+ s n. This conjecture is confirmed in two cases:n is arbitrary ands=n+1;s is arbitrary andn=2.  相似文献   

6.
Summary For differential operatorsM of second order (as defined in (1.1)) we describe a method to prove Range-Domain implications—Muu and an algorithm to construct these functions , , , . This method has been especially developed for application to non-inverse-positive differential operators. For example, for non-negativea 2 and for given functions = we require =C 0[0, 1] C 2([0, 1]–T) whereT is some finite set), (M) (t)(t), (t[0, 1]–T) and certain additional conditions for eachtT. Such Range-Domain implications can be used to obtain a numerical error estimation for the solution of a boundary value problemMu=r; further, we use them to guarantee the existence of a solution of nonlinear boundary value problems between the bounds- and .  相似文献   

7.
Flow disturbances produced by the slow relative motion of an impermeable body in a large, rapidly rotating vessel are studied as an asymptotic theory for an inviscid, incompressible fluid at a small Rossby number (u c /L1). The axial distance between the vessel wallsH is assumed to be so much larger than the body scaleL that the reduced height H/L is of unit order or greater. This flow admits a columnar structure near the body and an outer nonlinear structure of the inertial-wave type far above the forcing region, at distances along the rotation-axis (z=0(L/)). The inner boundary condition for the outer problem is provided by transferring the impermeable surface condition through the columnar structure; the outer solution in turn determines the vorticity and the solution of the columnar inner region.For thin obstacles or shallow ground topography (1), the outer solution is governed by an equation comparable to a linear one for inertial waves. The linear solutions obtained for steady transverse motion in an infinite domain () shows that, in this case, surface (perturbation) velocities are orthogonal to those in an irrotational (non-rotating) flow over the same ground topography. In the far field, i.e., ( z/L l) disturbances are confined mainly behind a wedge-shaped caustic front downstream of the rotation axis , wherein their amplitudes are comparable to , in general accord with Lighthill's result from group-velocity consideration. The field behind the caustic supports, however, lee waves extending far downstream with diminishing strength. Their wave lengths belong to orderLz/x, and therefore these waves should appear to be densely packed in the wedge-shaped region. The question on tilting of the Taylor column is delineated; the structure of the caustic zone and its upstream flow behavior are also analyzed.
Zusammenfassung Die Strömung um einen Körper, der sich langsam in einem grossen, rotierenden Behälter bewegt, wird untersucht mit einer asymptotischen Theorie für eine reibungsfreie, inkompressible Flüssigkeit bei einer kleinen Rossby-Zahl, d.h. u c /L1. Der axiale AbstandH zwischen den Gefässwänden wird als soviel grösser als die Körperabmessung angenommen, dass für die reduzierte Höhe =H/L 0(1) gilt. Diese Strömung erlaubt eine säulenähnliche Struktur (Taylor column) in Körpernähe und eine äussere, nichtlineare Struktur vom Wellentyp für Höhenz=0(L/) über dem Köper. Die innere Randbedingung für das äussere Problem wird erhalten, indem die Bedingung an der Wand durch die Säule verschoben wird. Die äussere Lösung bestimmt ihrerseits die Rotation und damit die Lösung im inneren, säulenartigen Bereich.Wenn Körper oder Bodenform flach sind (1), so wird die Aussenlösung durch eine Gleichung bestimmt, welche vergleichbar ist mit einer linearen Gleichung für Trägheitswellen. Lineare Lösungen werden für gleichförmige Bewegung von der Achse weg in einem unbegrenzten Bereich ) gegeben. Sie zeigen, dass die Oberflächenstromlinien orthogonal zu den Stromlinien sind, die bei rotationsfreier (nichtdrehender) Strömung über der gleichen Bodenform entstehen. Im Fernfeld ( z/L l) sind Störungen hauptsächlich auf ein keilförmiges Gebiet stromabwärts von der Rotationsachse ( ) begrenzt. In diesem Gebiet geht ihre Amplitude mit , in Uebereinstimmung mit Lighthill's Resultat, das mit der Gruppengeschwindigkeit hergeleitet wurde. Im keiförmigen Gebiet bestehen drei Familien von Lee-Wellen, welche sich mit unveränderter Stärke weit stromabwärts erstrecken. Ihre Wellenlängen gehören zur OrdnungLx/z, weshalb die Wellen im keilförmigen Bereich dicht gepackt erscheinen. Die Frage der Neigung der Taylor Säule behandelt und die Struktur des Randes vom keilförmigen Bereich wird analysiert.


This work is dedicated to Professor Nicholas Rott on the occasion of his sixtieth birthday.  相似文献   

8.
In this paper, it is shown that a necessary and sufficient condition for the existence of aC k-factorization ofK m,n is (i)m = n 0 (mod 2), (ii)k 0 (mod 2),k 4 and (iii) 2n 0 (modk) with precisely one exception, namely m =n = k = 6.  相似文献   

9.
Let s 0 and let + s be the set of functions x defined on a finite interval I and such that, for all collections of s + 1 pairwise different points t 0,..., t s I, the corresponding divided differences [x; t 0,...,t s ] of order s are nonnegative. Let + s B p + s B p, 1 p where B p is a unit ball in the space L p, and let + s L q + s L q, 1 q . For every s 3 and 1 q p , we determine the exact orders of the shape-preserving Kolmogorov widths {x - y} \right\ L_q , $$]]>, where M n is the collection of all affine linear manifolds M n in L q such that dim M n n and M n + s L q .Translated from Ukrainskyi Matematychnyi Zhurnal, Vol. 56, No. 7, pp. 901–926, July, 2004.  相似文献   

10.
We consider a sequence of Dirichlet problems for a nonlinear divergent operator A: W m 1( s ) [W m 1( s )]* in a sequence of perforated domains s . Under a certain condition imposed on the local capacity of the set \ s , we prove the following principle of compensated compactness: , where r s(x) and z s(x) are sequences weakly convergent in W m 1() and such that r s(x) is an analog of a corrector for a homogenization problem and z s(x) is an arbitrary sequence from whose weak limit is equal to zero.  相似文献   

11.
In this paper, it is shown that a necessary and sufficient condition for the existence of aP 3-factorization ofK m n is (i)mn 0(mod 3) and (ii) (m – 1)n 0(mod 4).  相似文献   

12.
The essence of this article lies in a demonstration of the fact that for some random search methods (r.s.m.) of global optimization, the number of the objective function evaluations required to reach a given accuracy may have very slow (logarithmic) growth to infinity as the accuracy tends to zero. Several inequalities of this kind are derived for some typical Markovian monotone r.s.m. in metric spaces including thed-dimensional Euclidean space d and its compact subsets. In the compact case, one of the main results may be briefly outlined as a constructive theorem of existence: if is a first moment of approaching a good subset of-neighbourhood ofx 0=arg maxf by some random search sequence (r.s.s.), then we may choose parameters of this r.s.s. in such a way that E c(f) In2 . Certainly, some restrictions on metric space and functionf are required.  相似文献   

13.
Weak L 2 -solutions u of the Schrödinger equation, –u + q(x) u – u = f(x) in L 2 , are represented by a Fourier series using spherical harmonics in order to prove the following strong maximum and anti-maximum principles in (N 2): Let 1 denote the positive eigenfunction associated with the principal eigenvalue 1 of the Schrödinger operator . Assume that the potential q(x) is radially symmetric and grows fast enough near infinity, and f is a `sufficiently smooth' perturbation of a radially symmetric function, f 0 and 0 f / C const a.e. in . Then u is 1-positive for - < < 1 (i.e., u c 1 with c const > 0) and 1-negative for 1 < < 1 + (i.e., u –c1 with c const > 0), where > 0 is a number depending on f. The constant c > 0 depends on both and f.  相似文献   

14.
We consider depth first search (DFS for short) trees in a class of random digraphs: am-out model. Let i be thei th vertex encountered by DFS andL(i, m, n) be the height of i in the corresponding DFS tree. We show that ifi/n asn, then there exists a constanta(,m), to be defined later, such thatL(i, m, n)/n converges in probability toa(,m) asn. We also obtain results concerning the number of vertices and the number of leaves in a DFS tree.  相似文献   

15.
For an odd prime powerq the infinite field GF(q 2 )= n0 GF (q 2n ) is explicitly presented by a sequence (f n)1 ofN-polynomials. This means that, for a suitably chosen initial polynomialf 1, the defining polynomialsf nGF(q)[x] of degrees2 n are constructed by iteration of the transformation of variablexx+1/x and have linearly independent roots over GF(q). In addition, the sequences are trace-compatible in the sense that the relative traces map the corresponding roots onto each other. In this first paper the caseq1 (mod 4) is considered and the caseq3 (mod 4) will be dealt with in a second paper. This specific construction solves a problem raised by A. Scheerhorn in [11].  相似文献   

16.
In this note we consider a reaction-diffusion problem which describes a simple model chemical reaction scheme for quadratic autocatalysis with linear decay. We show that withk>1 (wherek is a parameter measuring the relative strength of the decay step to the autocatalytic step) the dimensionless unreacting state 1, 0 is globally asymptotically stable, with 1+0(t –1/2) and 0(t –1/2 e (k–1)t) ast-. Here and are the concentrations of the reactant and the autocatalyst respectively, andt is time. The casek<1 has been considered in detail by Merkin et al. [1].  相似文献   

17.
The proximity is investigated of the solution of Cauchy's problem for the equation u t +((u))x= u xx ((u) > 0) to the solution of Cauchy's problem for the equation ut+ ((u))x= 0, when the solution of the latter problem has a finite number of lines of discontinuity in the strip 0 t T. It is proved that, everywhere outside a fixed neighborhood of the lines of discontinuity, we have |u–u| C, where the constant C is independent of. Similar inequalities are derived for the first derivatives of u–u.Translated from Matematicheskie Zametki, Vol. 8, No. 3, pp. 309–320, September, 1970.In conclusion we express our gratitude to L. A. Chudov for his valuable advice concerning this work.  相似文献   

18.
Spaces called rectangular spaces were introduced in [5] as incidence spaces (P,G) whose set of linesG is equipped with an equivalence relation and whose set of point pairs P2 is equipped with a congruence relation , such that a number of compatibility conditions are satisfied. In this paper we consider isomorphisms, automorphisms, and motions on the rectangular spaces treated in [5]. By an isomorphism of two rectangular spaces (P,G, , ) and (P,G, , ) we mean a bijection of the point setP onto P which maps parallel lines onto parallel lines and congruent points onto congruent points. In the following, we consider only rectangular spaces of characteristic 2 or of dimension two. According to [5] these spaces can be embedded into euclidean spaces. In case (P,G, , ) is a finite dimensional rectangular space, then every congruence preserving bijection ofP onto P is in fact an isomorphism from (P,G, , ) onto (P,G, , ) (see (2.4)). We then concern ourselves with the extension of isomorphisms. Our most important result is the theorem which states that any isomorphism of two rectangular spaces can be uniquely extended to an isomorphism of the associated euclidean spaces (see (3.2)). As a consequence the automorphisms of a rectangular space (P,G, , ) are precisely the restrictions (onP) of the automorphisms of the associated euclidean space which fixP as a whole (see (3.3)). Finally we consider the motions of a rectangular space (P,G, , ). By a motion of(P. G,, ) we mean a bijection ofP which maps lines onto lines, preserves parallelism and satisfies the condition((x), (y)) (x,y) for allx, y P. We show that every motion of a rectangular space can be extended to a motion of the associated euclidean space (see (4.2)). Thus the motions of a rectangular space (P,G, , ) are seen to be the restrictions of the motions of the associated euclidean space which mapP into itself (see (4.3)). This yields an explicit representation of the motions of any rectangular plane (see (4.4)).

Herrn Professor Burau zum 85. Geburtstag gewidmet  相似文献   

19.
We construct an asymptotic formula for a sum function for a (), where a () is the sum of the ath powers of the norms of divisors of the Gaussian integer on an arithmetic progression 0 (mod ) and in a narrow sector 1 arg < 2. For this purpose, we use a representation of a (n) in the form of a series in the Ramanujan sums.  相似文献   

20.
Summary We study integral functionals of the formF(u, )= f(u)dx, defined foru C1(;R k), R n . The functionf is assumed to be polyconvex and to satisfy the inequalityf(A) c0¦(A)¦ for a suitable constant c0 > 0, where (A) is then-vector whose components are the determinants of all minors of thek×n matrixA. We prove thatF is lower semicontinuous onC 1(;R k) with respect to the strong topology ofL 1(;R k). Then we consider the relaxed functional , defined as the greatest lower semicontinuous functional onL 1(;R k ) which is less than or equal toF on C1(;R k). For everyu BV(;R k) we prove that (u,) f(u)dx+c0¦Dsu¦(), whereDu=u dx+Dsu is the Lebesgue decomposition of the Radon measureDu. Moreover, under suitable growth conditions onf, we show that (u,)= f(u)dx for everyu W1,p(;R k), withp min{n,k}. We prove also that the functional (u, ) can not be represented by an inte- gral for an arbitrary functionu BVloc(R n;R k). In fact, two examples show that, in general, the set function (u, ) is not subadditive whenu BVloc(R n;R k), even ifu W loc 1,p (R n;R k) for everyp < min{n,k}. Finally, we examine in detail the properties of the functionsu BV(;R k) such that (u, )= f(u)dx, particularly in the model casef(A)=¦(A)¦.  相似文献   

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