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1.
Let k and r be fixed integers such that 1 < r < k. Any positive integer n of the form n = akb, where b is r-free, is called a (k, r)-integer. In this paper we prove that if Qk,r(x) denotes the number of (k, r)-integers ≤ x, then Qk,r(x) = xζ(k)ζ(r) + Δk,r(x), where Δk,r(x) = O(x1rexp [?Blog35x (log log x)?15]), B being a positive constant depending on r and the O-estimate is uniform in k. On the assumption of the Riemann hypothesis, we improve the above order estimate of Δk,r(x) and prove that
1x1αδk,r(t)dt=0(x1kω(x))or0(x3/(4r+1)ω(x))
, according as k ≤ (4r + 1)3 or k > (4r + 1)3, where ω(x) = exp [B log x(log log x)?1].  相似文献   

2.
3.
Let k be an odd positive integer. Davenport and Lewis have shown that the equations
a1x1k+…+anxnk=0
with integer coefficients, have a nontrivial solution in integers x1,…, xN provided that
N?[36klog6k]
Here it is shown that for any ? > 0 and k > k0(?) the equations have a nontrivial solution provided that
N?8log 2+?k log k.
  相似文献   

4.
Let f(z), an analytic function with radius of convergence R (0 < R < ∞) be represented by the gap series ∑k = 0ckzλk. Set M(r) = max¦z¦ = r ¦f(z)¦, m(r) = maxk ? 0{¦ ck ¦ rλk}, v(r) = maxk ¦ ¦ ck ¦ rλk = m(r)} and define the growth constants ?, λ, T, t by
?λ=lim supr→R inf{log[Rr /(R?r)]?1log+log+M(r)}
, and if 0 < ? < ∞,
Tt=lim supr→R inf{[Rr /(R?r)]??log+M(r)}
. Then, assuming 0 < t < T < ∞, we obtain a decomposition theorem for f(z).  相似文献   

5.
Let Lu be the integral operator defined by (Lk?)(x, y) = ∝ s ∝ ?(x′, y′)(eik??) dx′ dy′, (x, y) ? S where S is the interior of a smooth, closed Jordan curve in the plane, k is a complex number with Re k ? 0, Im k ? 0, and ?2 = (x ?x′)2 + (y ? y′)2. We define q(x, y) = [dist((x, y), ?S)]12, (x, y) ? S; L2(q, S) = {? : ∝ s ∝ ¦ ?(x, y)¦2 q(x, y) dx dy < ∞}; W21(q, S) = {? : ? ? L2(q, S), ???x, ?f?y ? L2(q, S)}, where in the definition of W21(q, S) the derivatives are taken in the sense of distributions. We prove that Lk is a continuous 1-l mapping of L2(q, S) onto W21(q, S).  相似文献   

6.
Let
F(x) = k=onnkAkxk
An ≠ 0,
and
G(x) = k=onnkBkxk
Bn ≠ 0,
be polynomials with real zeros satisfying An?1 = Bn?1 = 0, and let
H(x) = k=on-2nkAkBkxk.
Using the recently proved validity of the van der Waerden conjecture on permanents, some results on the real zeros of H(x) are obtained. These results are related to classical results on composite polynomials.  相似文献   

7.
The approximate solution of the finite moment problem μk = ∫01xk?1?(x) dx, k = 1, 2, 3, …, is considered. This problem is related to the problem of finding a best polynomial least squares approximation to a given function ?(x) in [0,1]. The connection with Laplace transform inversion is emphasized, and a set of special square matrices with integral elements is introduced, which has an intimate relation to the above two problems. These matrices are the well-known inverses of finite segments of the infinite Hilbert matrix.  相似文献   

8.
It is known that the classical orthogonal polynomials satisfy inequalities of the form Un2(x) ? Un + 1(x) Un ? 1(x) > 0 when x lies in the spectral interval. These are called Turan inequalities. In this paper we will prove a generalized Turan inequality for ultraspherical and Laguerre polynomials. Specifically if Pnλ(x) and Lnα(x) are the ultraspherical and Laguerre polynomials and Fnλ(x) = Pnλ(x)Pnλ(1), Gnα(x) = Lnα(x)Lnα(0), then Fnα(x) Fnβ(x) ? Fn + 1α(x) Fn ? 1β(x) > 0, ? 1 < x < 1, ?12 < α ? β ? α + 1 and Gnα(x) Gnβ(x) ? Gn + 1α(x) Gn ? 1β(x) > 0, x > 0, 0 < α ? β ? α + 1. We also prove the inequality (n + 1) Fnα(x) Fnβ(x) ? nFn + 1α(x) Fn ? 1β(x) > An[Fnα(x)]2, ?1 < x < 1, ?12 < α ? β < α + 1, where An is a positive constant depending on α and β.  相似文献   

9.
Let Z(Sn;?(x)) denote the polynomial obtained from the cycle index of the symmetric group Z(Sn) by replacing each variable si by f(x1). Let f(x) have a Taylor series with radius of convergence ? of the form f(x)=xk + ak+1xk+1 + ak+2xk+2+? with every a1?0. Finally, let 0<x<1 and let x??. We prove that
limn→∞Z(Sn;?(x))xkn = Πi=1k(1?xi)?ak+1
This limit is used to estimate the probability (for n and p both large) that a point chosen at random from a random p-point tree has degree n + 1. These limiting probabilities are independent of p and decrease geometrically in n, contrasting with the labeled limiting probabilities of 1n!e.In order to prove the main theorem, an appealing generalization of the principle of inclusion and exclusion is presented.  相似文献   

10.
It is shown that if A?Ωn?{Jn} satisfies
nkσk(A)?(n?k+1)2 σk?1(A)
(k=1,2,…,n)
, where σk(A) denotes the sum of all kth order subpermanent of A, then Per[λJn+(1?λ)A] is strictly decreasing in the interval 0<λ<1.  相似文献   

11.
We prove global well-posedness results for small initial data in Hs(R),s>sk, and in B?sk,12(R), sk=1/2?1/k, for the generalized Benjamin–Ono equation ?tu+H?2xu+?x(uk+1)=0,k?4. We also consider the cases k=2,3. To cite this article: L. Molinet, F. Ribaud, C. R. Acad. Sci. Paris, Ser. I 337 (2003).  相似文献   

12.
In this paper we are constructing a recurrence relation of the form
i=0rωi(k)mk+i{λ} [f] = ω(k)
for integrals (called modified moments)
mk{λ}[f]df=?11 f(x)Ck(λ)(x)dx (k = 0,1,…)
in which Ck(λ) is the k-th Gegenbauer polynomial of order λ(λ > ?12), and f is a function satisfying the differential equation
i=0n Pi(x)f(i)(x) = p(x) (?1?x?1)
of order n, where p0, p1, …, pn ? 0 are polynomials, and mkλ[p] is known for every k. We give three methods of construction of such a recurrence relation. The first of them (called Method I) is optimum in a certain sense.  相似文献   

13.
Let u(x, t) be the solution of utt ? Δxu = 0 with initial conditions u(x, 0) = g(x) and ut(x, 0) = ?;(x). Consider the linear operator T: ?; → u(x, t). (Here g = 0.) We prove for t fixed the following result. Theorem 1: T is bounded in Lp if and only if ¦ p?1 ? 2?1 ¦ = (n ? 1)?1and ∥ T?; ∥LαP = ∥?;∥LPwith α = 1 ?(n ? 1) ¦ p?1 ? 2?1 ¦. Theorem 2: If the coefficients are variables in C and constant outside of some compact set we get: (a) If n = 2k the result holds for ¦ p?1 ? 2?1 ¦ < (n ? 1)?1. (b) If n = 2k ? 1, the result is valid for ¦ p?1 ? 2?1 ¦ ? (n ? 1). This result are sharp in the sense that for p such that ¦ p?1 ? 2?1 ¦ > (n ? 1)?1 we prove the existence of ?; ? LP in such a way that T?; ? LP. Several applications are given, one of them is to the study of the Klein-Gordon equation, the other to the completion of the study of the family of multipliers m(ξ) = ψ(ξ) ei¦ξ¦ ¦ ξ ¦ ?b and finally we get that the convolution against the kernel K(x) = ?(x)(1 ? ¦ x ¦)?1 is bounded in H1.  相似文献   

14.
Author index     
A matrix T=(tik) is introduced, the coefficients of which are defined by kik:= (ik(ik)!)Σx?Snai(x)k, i, k?N={1, 2, 3,…,}, where ai(x) denotes the s the number of i cycles in the element x of the symmetric group Sn. It is shown that these numbers are natural numbers, that they are easy to evaluate, and that they serve very well in order to formulate an infinite number of characterizations of multiply transitive subgroups of symmetric groups in terms of the cycle structure of their elements.  相似文献   

15.
16.
Let θ(k, p) be the least s such that the congruence x1k + … + xsk ≡ 0(mod p) has a nontrivial solution. Let θ(k) = {max θ(k, p)| p > 1 + 2k}. The purpose of this note is to prove the following conjecture of S. Chowla: θ(k) = O(k12+?).  相似文献   

17.
In two party elections with popular vote ratio pq, 12≤p=1 ?q, a theoretical model suggests replacing the so-called MacMahon cube law approximation (pq)3, for the ratio PQ of candidates elected, by the ratio ?k(p)?k(q) of the two half sums in the binomial expansion of (p+q)2k+1 for some k. This ratio is nearly (pq)3 when k = 6. The success probability gk(p)=(pa(pa+qa) for the power law (pq)a?PQ is shown to so closely approximate ?k(p)=Σ0k(r2k+1)p2k+1?rqr, if we choose a = ak=(2k+1)!4kk!k!, that 1≤?k(p)gk(p)≤1.01884086 for k≥1 if12≤p≤1. Computationally, we avoid large binomial coefficients in computing ?k(p) for k>22 by expressing 2?k(p)?1 as the sum (p?q) Σ0k(4pq)sas(2s+1), whose terms decrease by the factors (4pq)(1?12s). Setting K = 4k+3, we compute ak for the large k using a continued fraction πak2=K+12(2K+32(2K+52(2K+…))) derived from the ratio of π to the finite Wallis product approximation.  相似文献   

18.
For parabolic initial boundary value problems various results such as limt ↓ 0{(?ut6x)(0, t)(?uα?x)(0, t)} = 1, where u satisfies ?u?t = a(u)(?2u?x2), 0 < x < 1, 0 < t ? T, u(x, 0) = 0, u(0, t) = |1(t), 0 < t ? T, u(1, t) = |2(t), 0 < t ? T, uαsatisfies (?uα?t) = α(?2uα?x2), 0 < x < 1, 0 < t ? T, uα(x, 0) = 0, uα(0, t) = |1(t), 0 < t ? T, uα(1, t) = |2(t), 0 < t ? T, and α = a(0), are demonstrated via the maximum principle and potential theoretic estimates.  相似文献   

19.
Given a set S of positive integers let ZkS(t) denote the number of k-tuples 〈m1, …, mk〉 for which mi ∈ S ? [1, t] and (m1, …, mk) = 1. Also let PkS(n) denote the probability that k integers, chosen at random from S ? [1, n], are relatively prime. It is shown that if P = {p1, …, pr} is a finite set of primes and S = {m : (m, p1pr) = 1}, then ZkS(t) = (td(S))k Πν?P(1 ? 1pk) + O(tk?1) if k ≥ 3 and Z2S(t) = (td(S))2 Πp?P(1 ? 1p2) + O(t log t) where d(S) denotes the natural density of S. From this result it follows immediately that PkS(n) → Πp?P(1 ? 1pk) = (ζ(k))?1 Πp∈P(1 ? 1pk)?1 as n → ∞. This result generalizes an earlier result of the author's where P = ? and S is then the whole set of positive integers. It is also shown that if S = {p1x1prxr : xi = 0, 1, 2,…}, then PkS(n) → 0 as n → ∞.  相似文献   

20.
Results on partition of energy and on energy decay are derived for solutions of the Cauchy problem ?u?t + ∑j = 1n Aj?u?xj = 0, u(0, x) = ?(x). Here the Aj's are constant, k × k Hermitian matrices, x = (x1,…, xn), t represents time, and u = u(t, x) is a k-vector. It is shown that the energy of Mu approaches a limit EM(?) as ¦ t ¦ → ∞, where M is an arbitrary matrix; that there exists a sufficiently large subspace of data ?, which is invariant under the solution group U0(t) and such that U0(t)? = 0 for ¦ x ¦ ? a ¦ t ¦ ? R, a and R depending on ? and that the local energy of nonstatic solutions decays as ¦ t ¦ → ∞. More refined results on energy decay are also given and the existence of wave operators is established, considering a perturbed equation E(x) ?u?t + ∑j = 1n Aj?u?xj = 0, where ¦ E(x) ? I ¦ = O(¦ x ¦?1 ? ?) at infinity.  相似文献   

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