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1.
The distributionF(x +, −r) Inx+ andF(x , −s) corresponding to the functionsx + −r lnx+ andx −s respectively are defined by the equations
(1) and
(2) whereH(x) denotes the Heaviside function. In this paper, using the concept of the neutrix limit due to J G van der Corput [1], we evaluate the non-commutative neutrix product of distributionsF(x +, −r) lnx+ andF(x , −s). The formulae for the neutrix productsF(x +, −r) lnx + ox −s, x+ −r lnx+ ox −s andx −s o F(x+, −r) lnx+ are also given forr, s = 1, 2, ...  相似文献   

2.
Let F be a distribution and let f be a locally summable function. The distribution F(f) is defined as the neutrix limit of the sequence {F n (f)}, where F n (x) = F(x) * δ n (x) and {δ n (x)} is a certain sequence of infinitely differentiable functions converging to the Dirac delta-function δ(x). The composition of the distributions x ?s ln m |x| and x r is proved to exist and be equal to r m x ?rs ln m |x| for r, s, m = 2, 3….  相似文献   

3.
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   

4.
A distribution functionF on the nonnegative real line is called subexponential if
whereF *n denotes then-fold Stieltjes convolution ofF with itself. In this paper, we consider the rate of convergence in the above definition and we discuss the asymptotic behavior ofR n (x) defined byR n (x)=1−F *n (x)−n(1−F(x)). Our results complement those previously obtained by several authors. In this paper, we define several new classes of functions related to regular variation andO-regular variation. As a typical result, in one of our theorems we show thatR n (x)=O(1)f(x)R(x), wheref(x) is the density ofF andR(x)=∫ 0 x (1−F(y))dy. We also discuss some applications. Published in Lietuvos Matematikos Rinkinys, Vol. 38, No. 1, pp. 1–18, January–March, 1998. Original article submitted April 24, 1996.  相似文献   

5.
Summary Let {X n },n=1,2,..., be a sequence of independent random variables distributed according to a distribution functionF(x) with finite variance,F n (x) be the empiric distribution function ofX 1,...,X n for eachn, andφ (n) * andφ * be optimum stratifications corresponding toF n (x) andF(x) respectively. It is shown in this paper thatφ (a) * tends almost surely toφ * under a suitable criterion. Institute of Statistical Mathematics  相似文献   

6.
Explicit inversion formulas are obtained for the hemispherical transform(FΜ)(x) = Μ{y ∃S n :x. y ≥ 0},xS n, whereS n is thendimensional unit sphere in ℝn+1,n ≥ 2, and Μ is a finite Borel measure onS n. If Μ is absolutely continuous with respect to Lebesgue measuredy onS n, i.e.,dΜ(y) =f(y)dy, we write(F f)(x) = ∫ x.y> 0 f(y)dy and consider the following cases: (a)fC (Sn); (b)f ∃ Lp(S n), 1 ≤ p < ∞; and (c)fC(Sn). In the case (a), our inversion formulas involve a certain polynomial of the Laplace-Beltrami operator. In the remaining cases, the relevant wavelet transforms are employed. The range ofF is characterized and the action in the scale of Sobolev spacesL p γ (Sn) is studied. For zonalf ∃ L1(S 2), the hemispherical transformF f was inverted explicitly by P. Funk (1916); we reproduce his argument in higher dimensions. Partially sponsored by the Edmund Landau Center for Research in Mathematical Analysis, supported by the Minerva Foundation (Germany).  相似文献   

7.
We consider the computation of the Cauchy principal value integral by quadrature formulae Q n F [f] of compound type, which are obtained by replacing f by a piecewise defined function Fn[f]. The behaviour of the constants ki, n in the estimates [R n F [f]] |⩽K i,n f (i) (where R n F [f] is the quadrature error) is determined for fixed i and n→∞, which means that not only the order, but also the coefficient of the main term of ki, n is determined. The behaviour of these error constants ki, n is compared with the corresponding ones obtained for the method of subtraction of the singularity. As it turns out, these error constants have, in general, the same asymptotic behaviour.  相似文献   

8.
Summary In this paper we determine all orthogonal polynomials Un(x) such that Un(x)=x1/2 F 2n+1 (x 1/2 ) and where f(t), u(t) have Taylor series expansions. Supported in part by N. S. F. grant GP-1593.  相似文献   

9.
Let an≥0 and F(u)∈C [0,1], Sikkema constructed polynomials: , ifα n ≡0, then Bn (0, F, x) are Bernstein polynomials. Let , we constructe new polynomials in this paper: Q n (k) (α n ,f(t))=d k /dx k B n+k (α n ,F k (u),x), which are called Sikkema-Kantorovic polynomials of order k. Ifα n ≡0, k=1, then Qn (1) (0, f(t), x) are Kantorovič polynomials Pn(f). Ifα n =0, k=2, then Qn (2), (0, f(t), x) are Kantorovič polynomials of second order (see Nagel). The main result is: Theorem 2. Let 1≤p≤∞, in order that for every f∈LP [0, 1], , it is sufficient and necessary that , § 1. Let f(t) de a continuous function on [a, b], i. e., f∈C [a, b], we define[1–2],[8–10]: . As usual, for the space Lp [a,b](1≤p<∞), we have and L[a, b]=l1[a, b]. Letα n ⩾0and F(u)∈C[0,1],Sikkema-Bernstein polynomials [3] [4]. The author expresses his thanks to Professor M. W. Müller of Dortmund University at West Germany for his supports.  相似文献   

10.
Let A⊆N={0,1,2,...} and β be an n-ary Boolean function. We call A a β-implicatively selector (β-IS) set if there exists an n-ary selector general recursive function f such that (∀x1,...,xn)(β(χ(x1),...,χ(xn))=1⟹f(x1,...,xn)∈A), where χ is the characteristic function of A. Let F(m), m≥1, be the family of all d m+1 * -IS sets, where , F(0)=N, and F(∞) is the class of all subsets in N. The basic result of the article says that the family of all β-IS sets coincides with one of F(m), m≥0, or F(∞), and, moreover, the inclusions F(0)⊂F(1)⊂...⊂F(∞) hold. Translated fromAlgebra i Logika, Vol. 35, No. 2, pp. 145–153, March–April, 1996.  相似文献   

11.
The non-commutative neutrix convolution product of the functions x r cos(x) and x s cos+(x) is evaluated. Further similar non-commutative neutrix convolution products are evaluated and deduced.  相似文献   

12.
For the Dirichlet series F(s) = ?n = 1 anexp{ sln } F(s) = \sum\nolimits_{n = 1}^\infty {{a_n}\exp \left\{ {s{\lambda_n}} \right\}} with abscissa of absolute convergence σ a =0, we establish conditions for (λ n ) and (a n ) under which lnM( s, F ) = TR( 1 + o(1) )exp{ rR
/ | s| } \ln M\left( {\sigma, F} \right) = {T_R}\left( {1 + o(1)} \right)\exp \left\{ {{{{{\varrho_R}}} \left/ {{\left| \sigma \right|}} \right.}} \right\} for σ ↑ 0, where M( s, F ) = sup{ | F( s+ it ) |:t ? \mathbbR } M\left( {\sigma, F} \right) = \sup \left\{ {\left| {F\left( {\sigma + it} \right)} \right|:t \in \mathbb{R}} \right\} and T R and ϱ R are positive constants.  相似文献   

13.
Let r, k, s be three integers such that , or We prove the following: Proposition. Let Y:={y i } i=1 s be a fixed collection of distinct points y i ∈ (-1,1) and Π (x):= (x-y 1 ). ... .(x-y s ). Let I:=[-1,1]. If f ∈ C (r) (I) and f'(x)Π(x) ≥ 0, x ∈ I, then for each integer n ≥ k+r-1 there is an algebraic polynomial P n =P n (x) of degree ≤ n such that P n '(x) Π (x) ≥ 0 and $$ \vert f(x)-P_n(x) \vert \le B\left(\frac{1}{n^2}+\frac{1}{n}\sqrt{1-x^2}\right)^r \omega_k \left(f^{(r)};\frac{1}{n^2}+\frac{1}{n}\sqrt{1-x^2}\right) \legno{(1)}$$ for all x∈ I, where ω k (f (r) ;t) is the modulus of smoothness of the k -th order of the function f (r) and B is a constant depending only on r , k , and Y. If s=1, the constant B does not depend on Y except in the case (r=1, k=3). In addition it is shown that (1) does not hold for r=1, k>3. March 20, 1995. Dates revised: March 11, 1996; December 20, 1996; and August 7, 1997.  相似文献   

14.
A distribution function F on the nonnegative real line is called subexponential if limx(1-F *n (x)/(1 - F(x)) = n for all n 2, where F *n denotes the nfold Stieltjes convolution of F with itself. In this paper, we consider the rate of convergence in the above definition and in its density analogue. Among others we discuss the asymptotic behavior of the remainder term R n (x) defined by R n (x) = 1 - F*n(x) - n(1 - F(x)) and of its density analogue rn (x) = -(Rn (x))'. Our results complement and complete those obtained by several authors. In an earlier paper, we obtained results of the form n(x) = O(1)f(x)R(x), where f is the density of F and R(x) = 0 x (1-F(y))dy. In this paper, among others we obtain asymptotic expressions of the form R n(x)= 2 n R2(x) + O(1)(-f'(x))R2(x) where f' is the derivative of f.  相似文献   

15.
The algebra of pseudodifferential operators with symbols inS 1,δ 0 , δ<1, is shown to be a spectrally invariant subalgebra of ℒ(b p,q s ) and ℒ(F p,q s ). The spectrum of each of these pseudodifferential operators acting onB p,q s orF p,q s is independent of the choice ofs, p, andq.  相似文献   

16.
Let f be an integrable function on the unit sphere Σ n−1 of R n (n⩾3) and let σ N δ be the Cesàro means of order σ of the Fourier-Laplace series of f. The special value λ:=n−2/2 of σ is known as the critical index. This paper proves that and where ω(f,t)p is the 1st-order modulus of continuity of f in Lp-metric which is defined in a way different than in the classical case of n=2. In Memory of Professor M. T. Cheng Project supported by the NSF of China under the grans # 19771009.  相似文献   

17.
Let g ≥ 2 be an integer, and let s(n) be the sum of the digits of n in basis g. Let f(n) be a complex valued function defined on positive integers, such that ?nx f(n)=o(x)\sum_{n\le x} f(n)=o(x) . We propose sufficient conditions on the function f to deduce the equality ?nx f(s(n))=o(x)\sum_{n\le x} f(s(n))=o(x) . Applications are given, for instance, on the equidistribution mod 1 of the sequence (s(n))α, where α is a positive real number.  相似文献   

18.
LetF(x) =F[x1,…,xn]∈ℤ[x1,…,xn] be a non-singular form of degree d≥2, and letN(F, X)=#{xεℤ n ;F(x)=0, |x|⩽X}, where . It was shown by Fujiwara [4] [Upper bounds for the number of lattice points on hypersurfaces,Number theory and combinatorics, Japan, 1984, (World Scientific Publishing Co., Singapore, 1985)] thatN(F, X)≪X n−2+2/n for any fixed formF. It is shown here that the exponent may be reduced ton - 2 + 2/(n + 1), forn ≥ 4, and ton - 3 + 15/(n + 5) forn ≥ 8 andd ≥ 3. It is conjectured that the exponentn - 2 + ε is admissable as soon asn ≥ 3. Thus the conjecture is established forn ≥ 10. The proof uses Deligne’s bounds for exponential sums and for the number of points on hypersurfaces over finite fields. However a composite modulus is used so that one can apply the ‘q-analogue’ of van der Corput’s AB process. Dedicated to the memory of Professor K G Ramanathan  相似文献   

19.
Chmielinski has proved in the paper [4] the superstability of the generalized orthogonality equation |〈f(x), f(y)〉| = |〈x,y〉|. In this paper, we will extend the result of Chmielinski by proving a theorem: LetD n be a suitable subset of ℝn. If a function f:D n → ℝn satisfies the inequality ∥〈f(x), f(y)〉| |〈x,y〉∥ ≤ φ(x,y) for an appropriate control function φ(x, y) and for allx, y ∈ D n, thenf satisfies the generalized orthogonality equation for anyx, y ∈ D n.  相似文献   

20.
The structure of the QFT expansion is studied in the framework of a new “invariant analytic” version of the perturbative QCD. Here, an invariant coupling constant α(Q 2 /Λ 2 ) = β 1 αs(Q 2 )/(4π) becomes a Q 2 -analytic invariant function α an (Q2/Λ 2 ) ≡A(x), which, by construction, is free of ghost singularities because it incorporates some nonperturbative structures. In the framework of the “analyticized” perturbation theory, an expansion for an observable F, instead of powers of the analytic invariant charge A(x), may contain specific functions An(x)=[an(x)] an , the “nth power of a(x) analyticized as a whole.” Functions A n>2(x) for small Q2Λ 2 oscillate, which results in weak loop and scheme dependences. Because of the analyticity requirement, the perturbation series for F(x) becomes an asymptotic expansion à la Erdélyi using a nonpower set {A n (x)}. The probable ambiguities of the invariant analyticization procedure and the possible inconsistency of some of its versions with the renormalization group structure are also discussed. Translated from Teoreticheskaya i Matematicheskaya Fizika, Vol. 119, No. 1, pp. 55–66, April, 1999.  相似文献   

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