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1.
Let e(x, y, ) be the spectral function and the unit spectral projection operator, with respect to the Laplace–Beltrami operator on a closed Riemannian manifold M. We generalize the one-term asymptotic expansion of e(x, x, ) by Hörmander (Acta Math. 88 (1968), 341–370) to that of x y e(x,y,)| x=y for any multiindices , in a sufficiently small geodesic normal coordinate chart of M. Moreover, we extend the sharp (L 2,L p) (2 p) estimates of by Sogge (J. Funct. Anal. 77 (1988), 123–134; London Math. Soc. Lecture Note Ser. 137, Cambridge University Press, Cambridge, 1989; Vol. 1, pp. 416–422) to the sharp (L 2, Sobolev L p) estimates of .  相似文献   

2.
We estimate the kinematic measure of one convex domain moving to another under the groupG of rigid motions in n . We first estimate the kinematic formula for the total scalar curvature D 0gD 1 Rdv of then–2 dimensional intersection submanifold D 0gD 1. Then we use Chern and Yen's kinematic fundamental formula and our integral inequality to obtain a sufficient condition for one convex domain to contain another in n (4). Forn=4, we directly obtain another sufficient condition in 4.  相似文献   

3.
The problem of solving the one-dimensional heat equation /t - 2/x2 = f(x, t) subject to given initial and nonlocal conditions is considered. It is solved in the Laplace transform domain by taking the Laplace transform of the unknown function with respect to time t. The physical solution is recovered with the help of a numerical technique for inverting the Laplace transform.AMS Subject Classification (1991): 35K20.  相似文献   

4.
Let K be a field of characteristic 2 and letV be a vector space of dimension 2m over K. Let f be a non-degenerate alternating bilinear form defined on V × V. The symplectic group Sp(2m, K) acts on the exterior powers k V for 0 k. 2m There is a contraction map defined on the exterior algebra , which commutes with the Sp(2m, K) action and satisfies 2 = 0 and ( k V) k–1 V We prove that ( k V)= ker k–1 V except when k=m+2. In the exceptional case, ( m+2 V) has codimension 2m in ker m V and we show that the quotient module ker m V/ m+2 V is a spin module for Sp(2m,K). When K is algebraically closed, we show that this spin module occurs with multiplicity 1 in m V and multiplicity 0 in all other components of V.  相似文献   

5.
Summary A functionf C (), is called monotone on if for anyx, y the relation x – y + s impliesf(x)f(y). Given a domain with a continuous boundary and given any monotone functionf on we are concerned with the existence and regularity ofmonotone extensions i.e., of functionsF which are monotone on all of and agree withf on . In particular, we show that there is no linear mapping that is capable of producing a monotone extension to arbitrarily given monotone boundary data. Three nonlinear methods for constructing monotone extensions are then presented. Two of these constructions, however, have the common drawback that regardless of how smooth the boundary data may be, the resulting extensions will, in general, only be Lipschitz continuous. This leads us to consider a third and more involved monotonicity preserving extension scheme to prove that, when is the unit square [0, 1]2 in 2, strictly monotone analytic boundary data admit a monotone analytic extension.Research supported by NSF Grant 8922154Research supported by DARPA: AFOSR #90-0323  相似文献   

6.
Reiterated homogenization is studied for divergence structure parabolic problems of the form u /t–div (a(x,x/,x/2,t,t/ k)u )=f. It is shown that under standard assumptions on the function a(x, y 1,y 2,t,) the sequence {u } of solutions converges weakly in L 2 (0,T; H 0 1 ()) to the solution u of the homogenized problem u/t– div(b(x,t)u)=f.This revised version was published online in April 2005 with a corrected missing date string.  相似文献   

7.
Summary We say that the discD()R 2, of radius , located around the origin isp-covered in timeT by a Wiener processW(·) if for anyzD() there exists a 0tT such thatW(t) is a point of the disc of radiusp, located aroundz. The supremum of those 's (0) is studied for which,D() isp-covered inT.  相似文献   

8.
Summary This paper is concerned with the rate of convergence to zero of theL pmetrics np1p, constructed out of differences between distribution functions, for departure from normality for normed sums of independent and identically distributed random variables with zero mean and unit variance. It is shown that the np are, under broad conditions, asymptotically equivalent in the strong sense that, for 1p, p, np/np is universally bounded away from zero and infinity asn.  相似文献   

9.
We consider generalized ruled surfaces in euclidean n-space n with k-dimensional generators and central ruled surface of dimension k–m+1 (O < m < k). Every orthogonal trajectoryy of the generators of defines a principal ruled surface y with generators totally orthogonal to the generators of . In each generator of y there exists an ellipsoid — called the indicatrix of the distribution parameters — which is defined by the distribution parameters of the tangent spaces to or y. Formulars will be given for the distribution parameters of and y .

Herrn Prof. Dr. H.R. Müller zum 70. Geburtstag  相似文献   

10.
LetX be the solution of the SDE:dX t = (X t)dB t +b(X t)dt, with andb C b (R) such that >0 for some constant , andB a real Brownian motion. Let be the law ofX onE=C([0, 1],R) andk E* – {0}, whereE* is the topological dual space ofE. Consider the classical form: k (u, v)=u / kv / kd, whereu andv are smooth functions onE. We prove that, if k is closable for anyk in a dense subset ofE* and if the smooth functions are contained in the domain of the generator of the closure of k , must be a constant function.  相似文献   

11.
Summary A characterization of compact sets in Lp (0, T; B) is given, where 1P and B is a Banach space. For the existence of solutions in nonlinear boundary value problems by the compactness method, the point is to obtain compactness in a space Lp (0,T; B) from estimates with values in some spaces X, Y or B where XBY with compact imbedding XB. Using the present characterization for this kind of situations, sufficient conditions for compactness are given with optimal parameters. As an example, it is proved that if {fn} is bounded in Lq(0,T; B) and in L loc 1 (0, T; X) and if {fn/t} is bounded in L loc 1 (0, T; Y) then {fn} is relatively compact in Lp(0,T; B), p相似文献   

12.
In this paper we consider lattice points in domains bounded by algebraic curves of the formx n+yn=Rn fulfilling the additional condition where and are fixed positive real numbers. The number of these lattice points is estimated for largeR and it appears that for rational or badly approximable and the error term in the final result can be made smaller (at least forn3) than it is best possible when counting the lattice points without the additional condition indicated above.  相似文献   

13.
Let {S n} be a random walk, generated by i.i.d. increments X i which drifts weakly to in the sense that as n . Suppose k0, k1, and E|X 1|1\k = if k>1. Then we show that the probability that S. crosses the curve nan K before it crosses the curve nan k tends to 1 as a . This intuitively plausible result is not true for k = 1, however, and for 1/2 <k<1, the converse results are not true in general, either. More general boundaries g(n) than g(n) = n k are also considered, and we also prove similar results for first passages out of regions like { (n, y): n1, |y| (a + n) k } as a .  相似文献   

14.
Zusammenfassung Eine neuentwickelte Methode für untere Schranken und das Rayleigh-Ritzverfahren für obere Schranken werden von den Verfassern dazu angewandt, die Eigenfrequenzen der Schwingungen von dünnen gleichförmigen, rechteckigen Platten mit freien Rändern abzuschätzen. Die Anwendbarkeit des Verfahrens für untere Schranken wird hervorgehoben, und es werden Berechnungen für eine Symmetrieklasse von rechteckigen sowie für eine Unterklasse von quadratischen Platten angegeben. Die dadurch entstehenden Schranken führen zu einer Verbesserung bisher veröffentlichter Resultate und weisen auf die Brauchbarkeit der Methode für untere Schranken hin.
Nomenclature The following symbols are not defined in the text 2 Laplacian differential operator (= 2/x 2 + 2/y 2) - 4 Biharmonic differential operator (= 4/x 4 + 2 4/x 2 y 2 + 4/y 4) - u Generic name for displacement functions - Generic name for eigenvalues - a,b Plate side lengths - Circular frequency of free vibration - Mass density of plate material - h Plate thickness - D Plate flexural rigidity - First variation - d Element of surface area - ij Kronecker's delta - {} Matrix or vector of the included elements The research reported in this article has been sponsored by the Department of the Navy under Contract NOw-62-0604-c with the Bureau of Naval Weapons.  相似文献   

15.
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   

16.
Let G be a graph with order p, size q and component number . For each i between p – and q, let be the family of spanning i-edge subgraphs of G with exactly components. For an integer-valued graphical invariant if H H is an adjacent edge transformation (AET) implies |(H)-(H')|1 then is said to be continuous with respect to AET. Similarly define the continuity of with respect to simple edge transformation (SET). Let M j() and m j() be the invariants defined by . It is proved that both M p–() and m p–(;) interpolate over , if is continuous with respect to AET, and that M j() and m j() interpolate over , if is continuous with respect to SET. In this way a lot of known interpolation results, including a theorem due to Schuster etc., are generalized.  相似文献   

17.
A computer-assisted proof is given of Minkowski's conjecture on the critical determinant of the region xp+yp<1 in the cases 1.03p 1.9745, p2.40, p2.577.Translated from Zapiski Nauchnykh Seminarov Leningradskogo Otdeleniya Matematicheskogo Instituta im. V. A. Steklova AN SSSR, Vol. 71, pp. 163–180, 1977.  相似文献   

18.
We give a general criterion for the intrinsic ultracontractivity of Dirichlet Laplacians – D on domainsD ofR d d 3, based on the Lieb's formula. It applies to various classes of domains (e.g. John, Hölder andL p-averaging domains) and gives new conditions for intrinsic ultracontractivity in terms of the Minkowski dimension of the boundary D. In particular, isotropic self-similar fractals and domains satisfying a c-covering condition are considered.  相似文献   

19.
Résumé Nous considérons l'équation différentielle stochastique réfléchie à valeur dansR 2 associée à l'opérateur différentiel dégénéré (1/2)2/x 2+x/y. On étudie alors le phénomène d'excursion autour du point origine. En particulier, on peut identifier la loi de l'inverse du temps local comme un subordinateur stable d'ordre 1/4 et en donner une formule du type temps d'occupation. Ceci permet alors d'étudier le comportement de la loi du processus au voisinage du point origine pour préciser, dans ce cas particulier, des résultats obtenus par Krée (1985) grâce à des méthodes analytiques.
Summary We consider theR 2-valued reflected stochastic differential equation associated with the degenerated differential operator (1/2)2/x 2+x/y. We study the excursion phenomenon around the point (0, 0). We are able to identify the law of the inverse of the local time as a stable subordinator with order 1/4 and to give for it an occupation time formula. These facts enable us to study the behavior of the law of the process near the point (0, 0) and to refine, in our case, results obtained by Krée (1985) by means of analytical methods.
  相似文献   

20.
Hieber  Matthias  Schrohe  Elmar 《Positivity》1999,3(3):259-272
Let {T p:q 1 p q 2} be a family of consistent C 0 semigroups on L p(), with q 1,q 2 [1,) and open. We show that certain commutator conditions on T p and on the resolvent of its generator A p ensure the p independence of the spectrum of A p for p [q 1,q 2.Applications include the case of Petrovskij correct systems with Hölder continuous coefficients, Schrödinger operators, and certain elliptic operators in divergence form with real, but not necessarily symmetric, or complex coefficients.  相似文献   

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