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1.
k-Self-correcting circuits of functional elements in the basis {x 1&x 2, $ \bar x $ \bar x } are considered. It is assumed that constant faults on outputs of functional elements are of the same type. Inverters are supposed to be reliable in service. The weight of each inverter is equal to 1. Conjunctors can be reliable in service, or not reliable. Each reliable conjunctor implements a conjunction of two variables and has a weight p > k + 2. Each unreliable conjunctor implements a conjunction in its correct state and implements a Boolean constant δ (δ ∈ {0, 1}) otherwise. Each unreliable conjunctor has the weight 1. It is stated that the complexity of realization of monotone threshold symmetric functions $ f_2^n \left( {x_1 ,...,x_n } \right) = \mathop \vee \limits_{1 \leqslant i < j \leqslant n} x_1 x_j ,n = 3,4 $ f_2^n \left( {x_1 ,...,x_n } \right) = \mathop \vee \limits_{1 \leqslant i < j \leqslant n} x_1 x_j ,n = 3,4 , ... by such circuits asymptotically equals (k + 3)n.  相似文献   

2.
The convergence behavior of best uniform rational approximants r n,m * with numerator degree n and denominator degree m on a compact set E is investigated for functions f continuous on E and ray sequences above the diagonal of the Walsh table, i. e. sequences {n,m(n)} n=1 with
$ \mathop {\lim \inf }\limits_{n \to \infty } \frac{n} {{m(n)}} \geqslant c > 1. $ \mathop {\lim \inf }\limits_{n \to \infty } \frac{n} {{m(n)}} \geqslant c > 1.   相似文献   

3.
Approximation to the function |x| plays an important role in approximation theory. This paper studies the approximation to the function xαsgn x, which equals |x| if α = 1. We construct a Newman Type Operator rn(x) and prove max |x|≤1|xαsgn x-rn(x)|~Cn1/4e-π1/2(1/2)αn.  相似文献   

4.
Let X,X(1),X(2),... be independent identically distributed random variables with mean zero and a finite variance. Put S(n) = X(1) + ... + X(n), n = 1, 2,..., and define the Markov stopping time η y = inf {n ≥ 1: S(n) ≥ y} of the first crossing a level y ≥ 0 by the random walk S(n), n = 1, 2,.... In the case $ \mathbb{E} $ \mathbb{E} |X|3 < ∞, the following relation was obtained in [8]: $ \mathbb{P}\left( {\eta _0 = n} \right) = \frac{1} {{n\sqrt n }}\left( {R + \nu _n + o\left( 1 \right)} \right) $ \mathbb{P}\left( {\eta _0 = n} \right) = \frac{1} {{n\sqrt n }}\left( {R + \nu _n + o\left( 1 \right)} \right) as n → ∞, where the constant R and the bounded sequence ν n were calculated in an explicit form. Moreover, there were obtained necessary and sufficient conditions for the limit existence $ H\left( y \right): = \mathop {\lim }\limits_{n \to \infty } n^{{3 \mathord{\left/ {\vphantom {3 2}} \right. \kern-\nulldelimiterspace} 2}} \mathbb{P}\left( {\eta _y = n} \right) $ H\left( y \right): = \mathop {\lim }\limits_{n \to \infty } n^{{3 \mathord{\left/ {\vphantom {3 2}} \right. \kern-\nulldelimiterspace} 2}} \mathbb{P}\left( {\eta _y = n} \right) for every fixed y ≥ 0, and there was found a representation for H(y). The present paper was motivated by the following reason. In [8], the authors unfortunately did not cite papers [1, 5] where the above-mentioned relations were obtained under weaker restrictions. Namely, it was proved in [5] the existence of the limit $ \mathop {\lim }\limits_{n \to \infty } n^{{3 \mathord{\left/ {\vphantom {3 2}} \right. \kern-\nulldelimiterspace} 2}} \mathbb{P}\left( {\eta _y = n} \right) $ \mathop {\lim }\limits_{n \to \infty } n^{{3 \mathord{\left/ {\vphantom {3 2}} \right. \kern-\nulldelimiterspace} 2}} \mathbb{P}\left( {\eta _y = n} \right) for every fixed y ≥ 0 under the condition $ \mathbb{E} $ \mathbb{E} X 2 < ∞ only; In [1], an explicit form of the limit $ \mathop {\lim }\limits_{n \to \infty } n^{{3 \mathord{\left/ {\vphantom {3 2}} \right. \kern-\nulldelimiterspace} 2}} \mathbb{P}\left( {\eta _0 = n} \right) $ \mathop {\lim }\limits_{n \to \infty } n^{{3 \mathord{\left/ {\vphantom {3 2}} \right. \kern-\nulldelimiterspace} 2}} \mathbb{P}\left( {\eta _0 = n} \right) was found under the same condition $ \mathbb{E} $ \mathbb{E} X 2 < ∞ in the case when the summand X has an arithmetic distribution. In the present paper, we prove that the main assertion in [5] fails and we correct the original proof. It worth noting that this corrected version was formulated in [8] as a conjecture.  相似文献   

5.
Considering the positive d-dimensional lattice point Z + d (d ≥ 2) with partial ordering ≤, let {X k: kZ + d } be i.i.d. random variables taking values in a real separable Hilbert space (H, ‖ · ‖) with mean zero and covariance operator Σ, and set $ S_n = \sum\limits_{k \leqslant n} {X_k } $ S_n = \sum\limits_{k \leqslant n} {X_k } , nZ + d . Let σ i 2, i ≥ 1, be the eigenvalues of Σ arranged in the non-increasing order and taking into account the multiplicities. Let l be the dimension of the corresponding eigenspace, and denote the largest eigenvalue of Σ by σ 2. Let logx = ln(xe), x ≥ 0. This paper studies the convergence rates for $ \sum\limits_n {\frac{{\left( {\log \log \left| n \right|} \right)^b }} {{\left| n \right|\log \left| n \right|}}} P\left( {\left\| {S_n } \right\| \geqslant \sigma \varepsilon \sqrt {2\left| n \right|\log \log \left| n \right|} } \right) $ \sum\limits_n {\frac{{\left( {\log \log \left| n \right|} \right)^b }} {{\left| n \right|\log \left| n \right|}}} P\left( {\left\| {S_n } \right\| \geqslant \sigma \varepsilon \sqrt {2\left| n \right|\log \log \left| n \right|} } \right) . We show that when l ≥ 2 and b > −l/2, E[‖X2(log ‖X‖) d−2(log log ‖X‖) b+4] < ∞ implies $ \begin{gathered} \mathop {\lim }\limits_{\varepsilon \searrow \sqrt {d - 1} } (\varepsilon ^2 - d + 1)^{b + l/2} \sum\limits_n {\frac{{\left( {\log \log \left| n \right|} \right)^b }} {{\left| n \right|\log \left| n \right|}}P\left( {\left\| {S_n } \right\| \geqslant \sigma \varepsilon \sqrt 2 \left| n \right|\log \log \left| n \right|} \right)} \hfill \\ = \frac{{K(\Sigma )(d - 1)^{\frac{{l - 2}} {2}} \Gamma (b + l/2)}} {{\Gamma (l/2)(d - 1)!}} \hfill \\ \end{gathered} $ \begin{gathered} \mathop {\lim }\limits_{\varepsilon \searrow \sqrt {d - 1} } (\varepsilon ^2 - d + 1)^{b + l/2} \sum\limits_n {\frac{{\left( {\log \log \left| n \right|} \right)^b }} {{\left| n \right|\log \left| n \right|}}P\left( {\left\| {S_n } \right\| \geqslant \sigma \varepsilon \sqrt 2 \left| n \right|\log \log \left| n \right|} \right)} \hfill \\ = \frac{{K(\Sigma )(d - 1)^{\frac{{l - 2}} {2}} \Gamma (b + l/2)}} {{\Gamma (l/2)(d - 1)!}} \hfill \\ \end{gathered} , where Γ(·) is the Gamma function and $ \prod\limits_{i = l + 1}^\infty {((\sigma ^2 - \sigma _i^2 )/\sigma ^2 )^{ - {1 \mathord{\left/ {\vphantom {1 2}} \right. \kern-\nulldelimiterspace} 2}} } $ \prod\limits_{i = l + 1}^\infty {((\sigma ^2 - \sigma _i^2 )/\sigma ^2 )^{ - {1 \mathord{\left/ {\vphantom {1 2}} \right. \kern-\nulldelimiterspace} 2}} } .  相似文献   

6.
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   

7.
We provide a characterization of the Banach spaces X with a Schauder basis (e n ) n∈ℕ which have the property that the dual space X* is naturally isomorphic to the space L diag(X) of diagonal operators with respect to (e n ) n∈ℕ. We also construct a Hereditarily Indecomposable Banach space $ \mathfrak{X} $ \mathfrak{X} D with a Schauder basis (e n ) n∈ℕ such that $ \mathfrak{X} $ \mathfrak{X} *D is isometric to L diag($ \mathfrak{X} $ \mathfrak{X} D) with these Banach algebras being Hereditarily Indecomposable. Finally, we show that every TL diag($ \mathfrak{X} $ \mathfrak{X} D) is of the form T = λI + K, where K is a compact operator.  相似文献   

8.
In this note we give a negative answer to Zemánek’s question (1994) of whether it always holds that a Cesàro bounded operator T on a Hilbert space with a single spectrum satisfies $ \mathop {\lim }\limits_{n \to \infty } $ \mathop {\lim }\limits_{n \to \infty } ∥T n+1T n ∥ = 0.  相似文献   

9.
Let ∧ be the Z2-Galois covering of the Grassmann algebra A over a field k of characteristic not equal to 2. In this paper, the dimensional formulae of Hochschild homology and cohomology groups of ∧ are calculated explicitly. And the cyclic homology of∧ can also be calculated when the underlying field is of characteristic zero. As a result, we prove that there is an isomorphism from i≥1 HH^i(∧) to i≥1 HH^i(∧).  相似文献   

10.
Let U n be the unit polydisk in C n and S be the space of functions of regular variation. Let 1 ≤ p < ∞, ω = (ω 1, ..., ω n ), ω j S(1 ≤ jn) and fH(U n ). The function f is said to be in holomorphic Besov space B p (ω) if
$ \left\| f \right\|_{B_p (\omega )}^p = \int_{U^n } {\left| {Df(z)} \right|^p \prod\limits_{j = 1}^n {\frac{{\omega _j (1 - |z_j |)}} {{(1 - |z_j |^{2 - p} )}}} dm_{2n} (z) < + \infty } $ \left\| f \right\|_{B_p (\omega )}^p = \int_{U^n } {\left| {Df(z)} \right|^p \prod\limits_{j = 1}^n {\frac{{\omega _j (1 - |z_j |)}} {{(1 - |z_j |^{2 - p} )}}} dm_{2n} (z) < + \infty }   相似文献   

11.
Explicit formulas are obtained for the maximum possible values of the derivatives f (k)(x), x ∈ (−1, 1), k ∈ {0, 1, ..., r − 1}, for functions f that vanish together with their (absolutely continuous) derivatives of order up to ≤ r − 1 at the points ±1 and are such that $ \left\| {f^{\left( r \right)} } \right\|_{L_2 ( - 1,1)} \leqslant 1 $ \left\| {f^{\left( r \right)} } \right\|_{L_2 ( - 1,1)} \leqslant 1 . As a corollary, it is shown that the first eigenvalue λ 1,r of the operator (−D 2) r with these boundary conditions is $ \sqrt 2 $ \sqrt 2 (2r)! (1 + O(1/r)), r → ∞.  相似文献   

12.
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   

13.
Let $ \mathfrak{S} $ \mathfrak{S} be a locally compact semigroup, ω be a weight function on $ \mathfrak{S} $ \mathfrak{S} , and M a ($ \mathfrak{S} $ \mathfrak{S} , ω) be the weighted semigroup algebra of $ \mathfrak{S} $ \mathfrak{S} . Let L 0 ($ \mathfrak{S} $ \mathfrak{S} ; M a ($ \mathfrak{S} $ \mathfrak{S} , ω)) be the C*-algebra of all M a ($ \mathfrak{S} $ \mathfrak{S} , ω)-measurable functions g on $ \mathfrak{S} $ \mathfrak{S} such that g/ω vanishes at infinity. We introduce and study a strict topology β 1($ \mathfrak{S} $ \mathfrak{S} , ω) on M a ($ \mathfrak{S} $ \mathfrak{S} , ω) and show that the Banach space L 0 ($ \mathfrak{S} $ \mathfrak{S} ; M a ($ \mathfrak{S} $ \mathfrak{S} , ω)) can be identified with the dual of M a ($ \mathfrak{S} $ \mathfrak{S} , ω) endowed with β 1($ \mathfrak{S} $ \mathfrak{S} , ω). We finally investigate some properties of the locally convex topology β 1($ \mathfrak{S} $ \mathfrak{S} , ω) on M a ($ \mathfrak{S} $ \mathfrak{S} , ω).  相似文献   

14.
We study some properties of sets of differences of dense sets in ℤ2 and ℤ3 and their interplay with Bohr neighbourhoods in ℤ. We obtain, inter alia, the following results.
(i)  If E ⊂ ℤ2, $ \bar d $ \bar d (E) > 0 and p i , q i ∈ ℤ[x], i = 1, ..., m satisfy p i (0) = q i (0) = 0, then there exists B ⊂ ℤ such that $ \bar d $ \bar d (B) > 0 and
$ E - E \supset \bigcup\limits_{i = 1}^m {(p_i (B) \times q_i (B))} . $ E - E \supset \bigcup\limits_{i = 1}^m {(p_i (B) \times q_i (B))} .   相似文献   

15.
Let A be a closed linear operator on a Banach space $ \mathfrak{B} $ \mathfrak{B} over the field Ω of complex p-adic numbers having an inverse operator defined on the whole $ \mathfrak{B} $ \mathfrak{B} , and f be a locally holomorphic at 0 $ \mathfrak{B} $ \mathfrak{B} -valued vector function. The problem of existence and uniqueness of a locally holomorphic at 0 solution of the differential equation y (m)Ay = f is considered in this paper. In particular, it is shown that this problem is solvable under the condition $ \mathop {\lim }\limits_{n \to \infty } \sqrt[n]{{\left\| {A^{ - n} } \right\|}} $ \mathop {\lim }\limits_{n \to \infty } \sqrt[n]{{\left\| {A^{ - n} } \right\|}} = 0. It is proved also that if the vector-function f is entire, then there exists a unique entire solution of this equation. Moreover, the necessary and sufficient conditions for the Cauchy problem for such an equation to be correctly posed in the class of locally holomorphic functions are presented.  相似文献   

16.
Let f be a primitive positive integral binary quadratic form of discriminant −D, and r f (n) the number of representations of n by f up to automorphisms of f. We first improve the error term E(x) of $ \sum\limits_{n \leqq x} {r_f (n)^\beta } $ \sum\limits_{n \leqq x} {r_f (n)^\beta } for any positive integer β. Next, we give an estimate of ∫1 T |E(x)|2 x −3/2 dx when β = 1.  相似文献   

17.
Let $ \mathbb{B} $ \mathbb{B} be the unit ball in ℂ n and let H($ \mathbb{B} $ \mathbb{B} ) be the space of all holomorphic functions on $ \mathbb{B} $ \mathbb{B} . We introduce the following integral-type operator on H($ \mathbb{B} $ \mathbb{B} ):
$ I_\phi ^g (f)(z) = \int\limits_0^1 {\operatorname{Re} f(\phi (tz))g(tz)\frac{{dt}} {t}} ,z \in \mathbb{B}, $ I_\phi ^g (f)(z) = \int\limits_0^1 {\operatorname{Re} f(\phi (tz))g(tz)\frac{{dt}} {t}} ,z \in \mathbb{B},   相似文献   

18.
Let t ≥ 1, let A and B be finite, nonempty subsets of an abelian group G, and let $ A\mathop + \limits_i B $ A\mathop + \limits_i B denote all the elements c with at least i representations of the form c = a + b, with aA and bB. For |A|, |B| ≥ t, we show that either
$ \sum\limits_{i = 1}^t {|A\mathop + \limits_i B| \geqslant t|A| + t|B| - 2t^2 + 1,} $ \sum\limits_{i = 1}^t {|A\mathop + \limits_i B| \geqslant t|A| + t|B| - 2t^2 + 1,}   相似文献   

19.
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   

20.
This work is a continuation of paper [1], where was considered analog of the problem of the first return for ultrametric diffusion. The main result of this paper consists in construction and investigation of stochastic quantity $ \tau _{B_r (a)} $ \tau _{B_r (a)} (ω), which has meaning of the first passage time into domain B r (a) by trajectories of the Markov stochastic process ζ(t, ω).Markov stochastic process is given by distribution density f(x, t), x ∈ ℚ p , tR +, which is solution of the Cauchy problem
$ \frac{\partial } {{\partial t}}f(x,t) = - D_x^\alpha f(x,t),f(x,0) = \Omega (\left| x \right|_p ). $ \frac{\partial } {{\partial t}}f(x,t) = - D_x^\alpha f(x,t),f(x,0) = \Omega (\left| x \right|_p ).   相似文献   

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