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1.
In the middle of the 20th century Hardy obtained a condition which must be imposed on a formal power series f(x) with positive coefficients in order that the series f −1(x) = $ \sum\limits_{n = 0}^\infty {b_n x^n } $ \sum\limits_{n = 0}^\infty {b_n x^n } b n x n be such that b 0 > 0 and b n ≤ 0, n ≥ 1. In this paper we find conditions which must be imposed on a multidimensional series f(x 1, x 2, …, x m ) with positive coefficients in order that the series f −1(x 1, x 2, …, x m ) = $ \sum i_1 ,i_2 , \ldots ,i_m \geqslant 0^b i_1 ,i_2 , \ldots ,i_m ^{x_1^{i_1 } x_2^{i_2 } \ldots x_m^{i_m } } $ \sum i_1 ,i_2 , \ldots ,i_m \geqslant 0^b i_1 ,i_2 , \ldots ,i_m ^{x_1^{i_1 } x_2^{i_2 } \ldots x_m^{i_m } } satisfies the property b 0, …, 0 > 0, $ bi_1 ,i_2 , \ldots ,i_m $ bi_1 ,i_2 , \ldots ,i_m ≤ 0, i 12 + i 22 + … + i m 2 > 0, which is similar to the one-dimensional case.  相似文献   

2.
Summary In the paper we estimate a regressionm(x)=E {Y|X=x} from a sequence of independent observations (X 1,Y 1),…, (X n, Yn) of a pair (X, Y) of random variables. We examine an estimate of a type , whereN depends onn andϕ N is Dirichlet kernel and the kernel associated with the hermite series. Assuming, that E|Y|<∞ and |Y|≦γ≦∞, we give condition for to converge tom(x) at almost allx, provided thatX has a density. if the regression hass derivatives, then converges tom(x) as rapidly asO(nC−(2s−1)/4s) in probability andO(n −(2s−1)/4s logn) almost completely.  相似文献   

3.
Let ( Y,d,dl )\left( {\mathcal{Y},d,d\lambda } \right) be (ℝ n , |·|, μ), where |·| is the Euclidean distance, μ is a nonnegative Radon measure on ℝ n satisfying the polynomial growth condition, or the Gauss measure metric space (ℝ n , |·|, d λ ), or the space (S, d, ρ), where S ≡ ℝ n ⋉ ℝ+ is the (ax + b)-group, d is the left-invariant Riemannian metric and ρ is the right Haar measure on S with exponential growth. In this paper, the authors introduce and establish some properties of the atomic Hardy-type spaces { Xs ( Y ) }0 < s \leqslant ¥\left\{ {X_s \left( \mathcal{Y} \right)} \right\}_{0 < s \leqslant \infty } and the BMO-type spaces { BMO( Y, s ) }0 < s \leqslant ¥\left\{ {BMO\left( {\mathcal{Y}, s} \right)} \right\}_{0 < s \leqslant \infty }. Let H 1 ( Y )\left( \mathcal{Y} \right) be the known atomic Hardy space and L 01 ( Y )\left( \mathcal{Y} \right) the subspace of fL 1 ( Y )\left( \mathcal{Y} \right) with integral 0. The authors prove that the dual space of X s ( Y )\left( \mathcal{Y} \right) is BMO( Y,s )BMO\left( {\mathcal{Y},s} \right) when s ∈ (0,∞), X s ( Y )\left( \mathcal{Y} \right) = H 1 ( Y )\left( \mathcal{Y} \right) when s ∈ (0, 1], and X ( Y )\left( \mathcal{Y} \right) = L 01 ( Y )\left( \mathcal{Y} \right) (or L 1 ( Y )\left( \mathcal{Y} \right)). As applications, the authors show that if T is a linear operator bounded from H 1 ( Y )\left( \mathcal{Y} \right) to L 1 ( Y )\left( \mathcal{Y} \right) and from L 1 ( Y )\left( \mathcal{Y} \right) to L 1,∞ ( Y )\left( \mathcal{Y} \right), then for all r ∈ (1,∞) and s ∈ (r,∞], T is bounded from X r ( Y )\left( \mathcal{Y} \right) to the Lorentz space L 1,s ( Y )\left( \mathcal{Y} \right), which applies to the Calderón-Zygmund operator on (ℝ n , |·|, μ), the imaginary powers of the Ornstein-Uhlenbeck operator on (ℝ n , |·|, d γ ) and the spectral operator associated with the spectral multiplier on (S, d, ρ). All these results generalize the corresponding results of Sweezy, Abu-Shammala and Torchinsky on Euclidean spaces.  相似文献   

4.
LetX be a Borel subset of a separable Banach spaceE. Letμ be a non-atomic,σ-finite, Borel measure onX. LetGL 1 (X, Σ,μ) bem-dimensional. Theorem:There is an l ∈ E* and real numbers −∞=x 0<x 1<x 2<…<x n<x n+1=∞with nm, such that for all g ∈ G,   相似文献   

5.
Let Hk\mathcal{H}_{k} denote the set {n∣2|n, n\not o 1 (mod p)n\not\equiv 1\ (\mathrm{mod}\ p) ∀ p>2 with p−1|k}. We prove that when X\frac1120(1-\frac12k) +e\leqq H\leqq XX^{\frac{11}{20}\left(1-\frac{1}{2k}\right) +\varepsilon}\leqq H\leqq X, almost all integers n ? \allowbreak Hk ?(X, X+H]n\in\allowbreak {\mathcal{H}_{k} \cap (X, X+H]} can be represented as the sum of a prime and a k-th power of prime for k≧3. Moreover, when X\frac1120(1-\frac1k) +e\leqq H\leqq XX^{\frac{11}{20}\left(1-\frac{1}{k}\right) +\varepsilon}\leqq H\leqq X, almost all integers n∈(X,X+H] can be represented as the sum of a prime and a k-th power of integer for k≧3.  相似文献   

6.
LetX andY denote two complex Banach spaces and letB(Y, X) denote the algebra of all bounded linear operators fromY toX. ForAB(X) n ,BB(Y) n , the elementary operator acting onB(Y, X) is defined by . In this paper we obtain the formulae of the spectrum and the essential spectrum of Δ(A, B) by using spectral mapping theorems. Forn=1, we prove thatS p (L A ,R B )=σ(A)×σ(B) and .  相似文献   

7.
James East 《Semigroup Forum》2010,81(2):357-379
The (full) transformation semigroup Tn\mathcal{T}_{n} is the semigroup of all functions from the finite set {1,…,n} to itself, under the operation of composition. The symmetric group Sn í Tn{\mathcal{S}_{n}\subseteq \mathcal{T}_{n}} is the group of all permutations on {1,…,n} and is the group of units of Tn\mathcal{T}_{n}. The complement Tn\Sn\mathcal{T}_{n}\setminus \mathcal{S}_{n} is a subsemigroup (indeed an ideal) of Tn\mathcal{T}_{n}. In this article we give a presentation, in terms of generators and relations, for Tn\Sn\mathcal{T}_{n}\setminus \mathcal{S}_{n}, the so-called singular part of Tn\mathcal{T}_{n}.  相似文献   

8.
Let {S n , n=0, 1, 2, …} be a random walk (S n being thenth partial sum of a sequence of independent, identically distributed, random variables) with values inE d , thed-dimensional integer lattice. Letf n =Prob {S 1 ≠ 0, …,S n −1 ≠ 0,S n =0 |S 0=0}. The random walk is said to be transient if and strongly transient if . LetR n =cardinality of the set {S 0,S 1, …,S n }. It is shown that for a strongly transient random walk with p<1, the distribution of [R n np]/σ √n converges to the normal distribution with mean 0 and variance 1 asn tends to infinity, where σ is an appropriate positive constant. The other main result concerns the “capacity” of {S 0, …,S n }. For a finite setA inE d , let C(A xA ) Prob {S n A, n≧1 |S 0=x} be the capacity ofA. A strong law forC{S 0, …,S n } is proved for a transient random walk, and some related questions are also considered. This research was partially supported by the National Science Foundation.  相似文献   

9.
We describe the set of parameters γ for which there exists a decomposition of the operator γI H in a sum of n self-adjoint operators with spectra from the sets M 1, …, M n, M i = 0, 1, …, k i, for n ≥ 4 and, in some cases, for n = 3. __________ Translated from Ukrains’kyi Matematychnyi Zhurnal, Vol. 60, No. 4, pp. 470–477, April, 2008.  相似文献   

10.
For a family of compact Riemann surfaces Xt of genus g > 1, parameterized by the Schottky space we define a natural basis of which varies holomorphically with t and generalizes the basis of normalized abelian differentials of the first kind for n  =  1. We introduce a holomorphic function F(n) on which generalizes the classical product for n  =  1 and g  =  1. We prove the holomorphic factorization formula
where det'Δ n is the zeta-function regularized determinant of the Laplace operator Δn in the hyperbolic metric acting on n-differentials, Nn is the Gram matrix of the natural basis with respect to the inner product given by the hyperbolic metric, S is the classical Liouville action –a K?hler potential of the Weil–Petersson metric on – and cg,n is a constant depending only on g and n. The factorization formula reduces to Kronecker’s first limit formula when n  =  1 and g  =  1, and to Zograf’s factorization formula for n  =  1 and g  >  1. Received: April 2005. Accepted: October 2005  相似文献   

11.
Fix any n≥1. Let X 1,…,X n be independent random variables such that S n =X 1+⋅⋅⋅+X n , and let S*n=sup1 £ knSkS^{*}_{n}=\sup_{1\le k\le n}S_{k} . We construct upper and lower bounds for s y and sy*s_{y}^{*} , the upper \frac1y\frac{1}{y} th quantiles of S n and S*nS^{*}_{n} , respectively. Our approximations rely on a computable quantity Q y and an explicit universal constant γ y , the latter depending only on y, for which we prove that
${l}\displaystyle s_y\le s_y^*\le Q_y\quad\mbox{for }y>1,\\[4pt]\displaystyle \gamma_{3y/16}Q_{3y/16}-Q_1\le s_y^*\quad\mbox{for }y>\frac{32}{3},$\begin{array}{l}\displaystyle s_y\le s_y^*\le Q_y\quad\mbox{for }y>1,\\[4pt]\displaystyle \gamma_{3y/16}Q_{3y/16}-Q_1\le s_y^*\quad\mbox{for }y>\frac{32}{3},\end{array}  相似文献   

12.
LetK be a field, charK=0 andM n (K) the algebra ofn×n matrices overK. If λ=(λ1,…,λ m ) andμ=(μ 1,…,μ m ) are partitions ofn 2 let wherex 1,…,x n 2,y 1,…,y n 2 are noncommuting indeterminates andS n 2 is the symmetric group of degreen 2. The polynomialsF λ, μ , when evaluated inM n (K), take central values and we study the problem of classifying those partitions λ,μ for whichF λ, μ is a central polynomial (not a polynomial identity) forM n (K). We give a formula that allows us to evaluateF λ, μ inM(K) in general and we prove that if λ andμ are not both derived in a suitable way from the partition δ=(1, 3,…, 2n−3, 2n−1), thenF λ, μ is a polynomial identity forM n (K). As an application, we exhibit a new class of central polynomials forM n (K). In memory of Shimshon Amitsur Research supported by a grant from MURST of Italy.  相似文献   

13.
Let f(n) be a strongly additive complex-valued arithmetic function. Under mild conditions on f, we prove the following weighted strong law of large numbers: if X,X 1,X 2, … is any sequence of integrable i.i.d. random variables, then
$ \mathop {\lim }\limits_{N \to \infty } \frac{{\sum\nolimits_{n = 1}^N {f(n)X_n } }} {{\sum\nolimits_{n = 1}^N {f(n)} }} = \mathbb{E}Xa.s. $ \mathop {\lim }\limits_{N \to \infty } \frac{{\sum\nolimits_{n = 1}^N {f(n)X_n } }} {{\sum\nolimits_{n = 1}^N {f(n)} }} = \mathbb{E}Xa.s.   相似文献   

14.
We consider a new Sobolev type function space called the space with multiweighted derivatives $ W_{p,\bar \alpha }^n $ W_{p,\bar \alpha }^n , where $ \bar \alpha $ \bar \alpha = (α 0, α 1,…, α n ), α i ∈ ℝ, i = 0, 1,…, n, and $ \left\| f \right\|W_{p,\bar \alpha }^n = \left\| {D_{\bar \alpha }^n f} \right\|_p + \sum\limits_{i = 0}^{n - 1} {\left| {D_{\bar \alpha }^i f(1)} \right|} $ \left\| f \right\|W_{p,\bar \alpha }^n = \left\| {D_{\bar \alpha }^n f} \right\|_p + \sum\limits_{i = 0}^{n - 1} {\left| {D_{\bar \alpha }^i f(1)} \right|} ,
$ D_{\bar \alpha }^0 f(t) = t^{\alpha _0 } f(t),D_{\bar \alpha }^i f(t) = t^{\alpha _i } \frac{d} {{dt}}D_{\bar \alpha }^{i - 1} f(t),i = 1,2,...,n $ D_{\bar \alpha }^0 f(t) = t^{\alpha _0 } f(t),D_{\bar \alpha }^i f(t) = t^{\alpha _i } \frac{d} {{dt}}D_{\bar \alpha }^{i - 1} f(t),i = 1,2,...,n   相似文献   

15.
In this paper, the sharp estimates of all homogeneous expansions for f are established, where f(z) = (f 1(z), f 2(z), …, f n (z))′ is a k-fold symmetric quasi-convex mapping defined on the unit polydisk in ℂ n and
$ \begin{gathered} \frac{{D^{tk + 1} + f_p \left( 0 \right)\left( {z^{tk + 1} } \right)}} {{\left( {tk + 1} \right)!}} = \sum\limits_{l_1 ,l_2 ,...,l_{tk + 1} = 1}^n {\left| {apl_1 l_2 ...l_{tk + 1} } \right|e^{i\tfrac{{\theta pl_1 + \theta pl_2 + ... + \theta pl_{tk + 1} }} {{tk + 1}}} zl_1 zl_2 ...zl_{tk + 1} ,} \hfill \\ p = 1,2,...,n. \hfill \\ \end{gathered} $ \begin{gathered} \frac{{D^{tk + 1} + f_p \left( 0 \right)\left( {z^{tk + 1} } \right)}} {{\left( {tk + 1} \right)!}} = \sum\limits_{l_1 ,l_2 ,...,l_{tk + 1} = 1}^n {\left| {apl_1 l_2 ...l_{tk + 1} } \right|e^{i\tfrac{{\theta pl_1 + \theta pl_2 + ... + \theta pl_{tk + 1} }} {{tk + 1}}} zl_1 zl_2 ...zl_{tk + 1} ,} \hfill \\ p = 1,2,...,n. \hfill \\ \end{gathered}   相似文献   

16.
In this paper, the following results are obtained: 1) It is proved that, in the fourth order differential neighborhood, a regular hypersurface V n−1 embedded into a projective-metric space K n , n ≥ 3, intrinsically induces a dual projective-metric space $ \bar K_n $ \bar K_n . 2) An invariant analytical condition is established under which a normalization of a hypersurface V n−1 ⊂ K n (a tangential hypersurface $ \bar V_{n - 1} $ \bar V_{n - 1} ⊂ $ \bar K_n $ \bar K_n ) by quasitensor fields H n i , H i ($ \bar H_n^i $ \bar H_n^i , $ \bar H_i $ \bar H_i ) induces a Riemannian space of constant curvature. If the two conditions are fulfilled simultaneously, the spaces R n−1 and $ \bar R_{n - 1} $ \bar R_{n - 1} are spaces of the same constant curvature $ K = - \tfrac{1} {c} $ K = - \tfrac{1} {c} . 3) Geometric interpretations of the obtained analytical conditions are given.  相似文献   

17.
We obtain characterizations (and prove the corresponding equivalence of norms) of function spaces B pq sm ($ \mathbb{I} $ \mathbb{I} k ) and L pq sm ($ \mathbb{I} $ \mathbb{I} k ) of Nikol’skii-Besov and Lizorkin-Triebel types, respectively, in terms of representations of functions in these spaces by Fourier series with respect to a multiple system $ \mathcal{W}_m^\mathbb{I} $ \mathcal{W}_m^\mathbb{I} of Meyer wavelets and in terms of sequences of the Fourier coefficients with respect to this system. We establish order-sharp estimates for the approximation of functions in B pq sm ($ \mathbb{I} $ \mathbb{I} ) and L pq sm ($ \mathbb{I} $ \mathbb{I} k ) by special partial sums of these series in the metric of L r ($ \mathbb{I} $ \mathbb{I} k ) for a number of relations between the parameters s, p, q, r, and m (s = (s 1, ..., s n ) ∈ ℝ+ n , 1 ≤ p, q, r ≤ ∞, m = (m 1, ..., m n ) ∈ ℕ n , k = m 1 +... + m n , and $ \mathbb{I} $ \mathbb{I} = ℝ or $ \mathbb{T} $ \mathbb{T} ). In the periodic case, we study the Fourier widths of these function classes.  相似文献   

18.
Let λ be a real number such that 0 < λ < 1. We establish asymptotic formulas for the weighted real moments Σ nx R λ (n)(1 − n/x), where R(n) =$ \prod\nolimits_{\nu = 1}^k {p_\nu ^{\alpha _\nu - 1} } $ \prod\nolimits_{\nu = 1}^k {p_\nu ^{\alpha _\nu - 1} } is the Atanassov strong restrictive factor function and n =$ \prod\nolimits_{\nu = 1}^k {p_\nu ^{\alpha _\nu } } $ \prod\nolimits_{\nu = 1}^k {p_\nu ^{\alpha _\nu } } is the prime factorization of n.  相似文献   

19.
Let X, X1 , X2 , . . . be i.i.d. random variables, and set Sn = X1 +···+Xn , Mn = maxk≤n |Sk|, n ≥1. Let an = o( (n)(1/2)/logn). By using the strong approximation, we prove that, if EX = 0, VarX = σ2 0 and E|X| 2+ε ∞ for some ε 0, then for any r 1, lim ε1/(r-1)(1/2) [ε-2-(r-1)]∞∑n=1 nr-2 P{Mn ≤εσ (π2n/(8log n))(1/2) + an } = 4/π . We also show that the widest a n is o( n(1/2)/logn).  相似文献   

20.
In this article, we study geometric aspects of the space of arcs parameterized by unit speed in the L 2 metric. Physically, this corresponds to the motion of a whip, and it also arises in studying shape recognition. The geodesic equation is the nonlinear, nonlocal wave equation η tt = ∂ s (σ η s ), with \lvert hs\rvert o 1{\lvert \eta_{s}\rvert\equiv 1} and σ given by sss- \lvert hss\rvert2 s = -\lvert hst\rvert2{\sigma_{ss}- \lvert \eta_{ss}\rvert^2 \sigma = -\lvert \eta_{st}\rvert^2}, with boundary conditions σ(t, 1) = σ(t, −1) = 0 and η(t, 0) = 0. We prove that the space of arcs is a submanifold of the space of all curves, that the orthogonal projection exists but is not smooth, and as a consequence we get a Riemannian exponential map that is continuous and even differentiable but not C 1. This is related to the fact that the curvature is positive but unbounded above, so that there are conjugate points at arbitrarily short times along any geodesic.  相似文献   

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