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1.
X(Y) f -:X(Y)={fM(×): fX(Y)=f(x,.)YX< . =(0, ), M (×) — , ×, X, Y, Z— . X(Y) Z(×).  相似文献   

2.
Let be a ball in N, centered at zero, and letu be a minimizer of the nonconvex functional over one of the classesC M := {w W loc 1, () 0 w(x) M in,w concave} orE M := {w W loc 1,2 () 0 w(x) M in,w 0 inL()}of admissible functions. Thenu is not radial and not unique. Therefore one can further reduce the resistance of Newton's rotational body of minimal resistance through symmetry breaking.  相似文献   

3.
The first property is a refinement of earlier results of Ch. de la Vallée Poussin, M. Brelot, and A. F. Grishin. Let w=u–v with u, v superharmonic on a suitable harmonic space (for example an open subset of R n ), and let [w]=[u]–[v] denote the associated Riesz charge. If w0, and if E denotes the set of those points of at which the lim inf of w in thefine topology is 0, then the restriction of [w] to E is 0. Another property states that, if e denotes a polar subset of such that the fine lim inf of |w| at each point of e is finite, then the restriction of [w] to e is 0.  相似文献   

4.
Range of the posterior probability of an interval over the -contamination class ={=(1–)0+q:qQ} is derived. Here, 0 is the elicited prior which is assumed unimodal, is the amount of uncertainty in 0, andQ is the set of all probability densitiesq for which =(1–)0+q is unimodal with the same mode as that of 0. We show that the sup (resp. inf) of the posterior probability of an interval is attained by a prior which is equal to (1–)0 except in one interval (resp. two disjoint intervals) where it is constant.  相似文献   

5.
Numerical calculations are carried out in the hodograph plane to construct optimal critical airfoil shapes and the flow about them. These optimal airfoil shapes give the highest free-stream Mach numberM for a given thickness ratio and tail angle t (nonlifting) for which the flow is nowhere supersonic. A relationship betweenM and for various t is given. Analytical and numerical solutions to the same problem are found on the basis of transonic small-disturbance theory. These results provide a limiting case asM 1, 0 and agree well with the calculations of the full problem. Using a numerical method to calculate the flow about general (subsonic) airfoils, a comparison is made between the critical free-stream Mach numbers for some standard airfoil shapes and the optimal free stream Mach number of the corresponding and t . A significant increase in the critical free-stream Mach number is found for the optimal airfoils.  相似文献   

6.
The explicit solution of the equation u=f in a plane infinite angle, satisfying on one side of the angle a Neumann condition and on the other one the condition u/n + hu/r + u= (/r is the tangential derivative, C, 0), is constructed and estimated in weighted Sobolev spaces. The obtained estimates are sharp with respect to the differential order and are uniform with respect to . The construction of the solution reduces to the investigation of a finite difference equation in the complex plane, arising after a Mellin transform.Translated from Zapiski Nauchnykh Seminarov Leningradskogo Otdeleniya Matematicheskogo Instituta im. V. A. Steklova Akademii Nauk SSSR, Vol. 182, pp. 149–167, 1990.  相似文献   

7.
Let (n) be the number of all prime divisors ofn and (n) the number of distinct prime divisors ofn. We definev q (x)=|{nx(n)–(n)=q}|. In this paper, we give an asymptotic development ofv q (x); this improves on previous results.
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8.
In this paper we examine for which Witt classes ,..., n over a number field or a function fieldF there exist a finite extensionL/F and 2,..., n L* such thatT L/F ()=1 andTr L/F (i)=i fori=2,...n.  相似文献   

9.
Let G denote a semisimple group, a discrete subgroup, B=G/P the Poisson boundary. Regarding invariants of discrete subgroups we prove, in particular, the following:(1) For any -quasi-invariant measure on B, and any probablity measure on , the norm of the operator () on L 2(B,) is equal to (), where is the unitary representation in L 2(X,), and is the regular representation of .(2) In particular this estimate holds when is Lebesgue measure on B, a Patterson–Sullivan measure, or a -stationary measure, and implies explicit lower bounds for the displacement and Margulis number of (w.r.t. a finite generating set), the dimension of the conformal density, the -entropy of the measure, and Lyapunov exponents of .(3) In particular, when G=PSL2() and is free, the new lower bound of the displacement is somewhat smaller than the Culler–Shalen bound (which requires an additional assumption) and is greater than the standard ball-packing bound.We also prove that ()=G() for any amenable action of G and L 1(G), and conversely, give a spectral criterion for amenability of an action of G under certain natural dynamical conditions. In addition, we establish a uniform lower bound for the -entropy of any measure quasi-invariant under the action of a group with property T, and use this fact to construct an interesting class of actions of such groups, related to 'virtual' maximal parabolic subgroups. Most of the results hold in fact in greater generality, and apply for instance when G is any semi-simple algebraic group, or when is any word-hyperbolic group, acting on their Poisson boundary, for example.  相似文献   

10.
We study uniqueness property for the Cauchy problemxV(x), x(0)=, whereVR nR is a locally Lipschitz continuous, quasiconvex function (i.e. the sublevel sets {Vc} are convex) and V(x) is the generalized gradient ofV atx. We prove that if 0V(x) forV(x)b, then the set of initial data {V=b} yielding non uniqueness of solution in a geometric sense has (n–1)-dimensional Hausdorff measure zero in {V=b}.  相似文献   

11.
Let X = Y Z, Y Z = Ø, < be a topogenity on Y, a topology on X. A (<, )-extension is a topogenity < on X such that < ¦Y = <, (<) = . We establish some properties of (<, )-extensions and construct all of them in the case of a finite Z.  相似文献   

12.
13.
In engineering and economics often a certain vectorx of inputs or decisions must be chosen, subject to some constraints, such that the expected costs (or loss) arising from the deviation between the outputA() x of a stochastic linear systemxA()x and a desired stochastic target vectorb() are minimal. Hence, one has the following stochastic linear optimization problem minimizeF(x)=Eu(A()x b()) s.t.xD, (1) whereu is a convex loss function on m , (A(), b()) is a random (m,n + 1)-matrix, E denotes the expectation operator andD is a convex subset of n . Concrete problems of this type are e.g. stochastic linear programs with recourse, error minimization and optimal design problems, acid rain abatement methods, problems in scenario analysis and non-least square regression analysis.Solving (1), the loss functionu should be exactly known. However, in practice mostly there is some uncertainty in assigning appropriate penalty costs to the deviation between the outputA ()x and the targetb(). For finding in this situation solutions hedging against uncertainty a set of so-called efficient points of (1) is defined and a numerical procedure for determining these compromise solutions is derived. Several applications are discussed.  相似文献   

14.
Summary For a non-linear boundary value problem with a positive and increasing non-linearity there exists a critical value* of the parameter, beyond which there are no solutions. We give a minimax characterization of*.
Zusammenfassung In der Randwertaufgabe –u(x)=f(x, u(x)), u(a)=u(b)=0, seif positiv und wachsend im zweiten Argument. Dann gibt es einen Wert*, so dass keine Lösung existiert für>*. In dieser Arbeit wird* durch ein Minimaxprinzip charakterisiert. Der Beweis beruht auf der Anwendung von Ober- und Unterlösungen und monotonen Iterationen.
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15.
We show that for reasonable couples of Pisot number and , there is no measure simultaneously invariant by the two transformations of [0, 1], x {x} and x {x}, and Bernoulli (or weak Bernoulli) for one of the transformations.  相似文献   

16.
The behavior of the poles zn(), n=1,2,... of the scattering matrix of the operatorl u=–u(x), x , (u/n)+(x)u|=0 as 0 is considered. It is proved that |zn()–zn|=0((1/2)qn), where qn is the order of the pole of the scattering matrix for the operator 0u=–u, u/=0.Translated from Zapiski Nauchnykh Seminarov Leningradskogo Otdeleniya Matematicheskogo Instituta im. V. A. Steklova AN SSSR, Vol. 117, pp. 183–191, 1981.  相似文献   

17.
V.P. Fonf  C. Zanco 《Positivity》2004,8(3):269-281
For any subset A of the unit sphere of a Banach space X and for [0,2) the notion of -flatness is introduced as a measure of non-flatness of A. For any positive , construction of locally finite tilings of the unit sphere by -flat sets is carried out under suitable -renormings of X in a quite general context; moreover, a characterization of spaces having separable dual is provided in terms of the existence of such tilings. Finally, relationships between the possibility of getting such tilings of the unit sphere in the given norm and smoothness properties of the norm are discussed.  相似文献   

18.
Upper and lower bounds are obtained for the radius of-convexity, R, of the schlicht within ¦z¦< 1 functions g(z), g(0)=0, and g(0)=1, for values ranging from 0 to 0.313.... The exact value of R is determined for 0.313... < 1. The results constitute the solution to a problem recently posed by the Roumanianmathematician P. T. Mocanu [1].Translated from Matematicheskie Zametki, Vol. 11, No. 2, pp. 227–232, February, 1972.  相似文献   

19.
Summary A totally umbilical pseudo-Riemannian submanifold with the parallel mean curvature vector field is said to be an extrinsic sphere. A regular curve in a pseudo-Riemannian manifold is called a circle if it is an extrinsic sphere. LetM be ann-dimensional pseudo-Riemannian submanifold of index (0n) in a pseudo-Riemannian manifold with the metricg and the second fundamental formB. The following theorems are proved. For 0 = +1 or –1, 1 = +1, –1 or 0 (2–2 0+ 12n–2–2) and a positive constantk, every circlec inM withg(c, c) = 0 andg( c c, c c) = 1 k 2 is a circle in iffM is an extrinsic sphere. For 0 = +1 or –1 (–0n–), every geodesicc inM withg(c, c) = 0 is a circle in iffM is constant isotropic and B(x,x,x) = 0 for anyx T(M). In this theorem, assume, moreover, that 1n–1 and the first normal space is definite or zero at every point. Then we can prove thatM is an extrinsic sphere. When = 0 orn, this fact does not hold in general.  相似文献   

20.
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   

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