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1.
Generating functions are obtained for certain types of permutations analogous to up-down and down-up permutations. In each case the generating function is a quotient of entire functions; the denominator in each case is φ02(x) ? φ1(x)φ3(x), where
φj(x)=n=ox4n+j(4n+j)!.
  相似文献   

2.
A variety of continuous parameter Markov chains arising in applied probability (e.g. epidemic and chemical reaction models) can be obtained as solutions of equations of the form
XN(t)=x0+∑1NlY1N ∫t0 f1(XN(s))ds
where l∈Zt, the Y1 are independent Poisson processes, and N is a parameter with a natural interpretation (e.g. total population size or volume of a reacting solution).The corresponding deterministic model, satisfies
X(t)=x0+ ∫t0 ∑ lf1(X(s))ds
Under very general conditions limN→∞XN(t)=X(t) a.s. The process XN(t) is compared to the diffusion processes given by
ZN(t)=x0+∑1NlB1N∫t0 ft(ZN(s))ds
and
V(t)=∑ l∫t0f1(X(s))dW?1+∫t0 ?F(X(s))·V(s)ds.
Under conditions satisfied by most of the applied probability models, it is shown that XN,ZN and V can be constructed on the same sample space in such a way that
XN(t)=ZN(t)+OlogNN
and
N(XN(t)?X(t))=V(t)+O log NN
  相似文献   

3.
A general branching process begins with a single individual born at time t=0. At random ages during its random lifespan L it gives birth to offspring, N(t) being the number born in the age interval [0,t]. Each offspring behaves as a probabilistically independent copy of the initial individual. Let Z(t) be the population at time t, and let N=N(∞). Theorem: If a general branching process is critical, i. e E{N}=1, and if σ2=E {N(N?1)}<∞, 0<a≡0 tdE{N(t)},and as t → ∞ both t2(1?E {N(t)})→0 and t2P[L>t]→0, then tP[Z(t)>0]→2aσ2 as t→∞.  相似文献   

4.
The message m = {m(t)} is a Gaussian process that is to be transmitted through the white Gaussian channel with feedback: Y(t) = ∫0tF(s, Y0s, m)ds + W(t). Under the average power constraint, E[F2(s, Y0s, m)] ≤ P0, we construct causally the optimal coding, in the sense that the mutual information It(m, Y) between the message m and the channel output Y (up to t) is maximized. The optimal coding is presented by Y(t) = ∫0t A(s)[m(s) ? m?(s)] ds + W(t), where m?(s) = E[m(s) ¦ Y(u), 0 ≤ u ≤ s] and A(s) is a positive function such that A2(s) E |m(s) ? m?(s)|2 = P0.  相似文献   

5.
Two related almost sure limit theorems are obtained in connection with a stochastic process {ξ(t), ?∞ < t < ∞} with independent increments. The first result deals with the existence of a simultaneous stabilizing function H(t) such that (ξ(t) ? ξ(0))H(t) → 0 for almost all sample functions of the process. The second result deals with a wide-sense stationary process whose random spectral distributions is ξ. It addresses the question: Under what conditions does (2T)?1?TTX(t)X(t + τ)dt converge as T → ∞ for all τ for almost all sample functions?  相似文献   

6.
On a modified space Φ′ from the space J′ of tempered distributions, it is proven that a stochastic equation, X(t) = γ + W(t) + ∝0t L1(s) X(s) ds, has a unique solution, where W(t) is a Φ′-valued Brownian motion independent of a Φ′-valued Gaussian random variable γ and L1(s) is an integro-differential operator. As an application, a fluctuaton result (or central limit theorem) is shown for interacting diffusions.  相似文献   

7.
The system ?x?t = Δx + F(x,y), ?y?t = G(x,y) is investigated, where x and y are scalar functions of time (t ? 0), and n space variables 1,…, ξn), Δx ≡ ∑i = 1n?2xi2, and F and G are nonlinear functions. Under certain hypotheses on F and G it is proved that there exists a unique spherically symmetric solution (x(r),y(r)), where r = (ξ12 + … + ξn2)12, which is bounded for r ? 0 and satisfies x(0) >x0, y(0) > y0, x′(0) = 0, y′(0) = 0, and x′ < 0, y′ > 0, ?r > 0. Thus, (x(r), y(r)) represents a time independent equilibrium solution of the system. Further, the linearization of the system restricted to spherically symmetric solutions, around (x(r), y(r)), has a unique positive eigenvalue. This is in contrast to the case n = 1 (i.e., one space dimension) in which zero is an eigenvalue. The uniqueness of the positive eigenvalue is used in the proof that the spherically symmetric solution described is unique.  相似文献   

8.
The iterative method of the first author makes possible a self-correcting scheme for the approximate solution obtained. This scheme accelerates the convergence and substantially decreases the number of terms necessary in computation for applications involving either linear or nonlinear stochastic systems. A “feedback” term compensates for the approximation of the system inverse operator by a partial sum. Further, errors are determined in calculating the mean solution 〈y〉 and the correlation Ry(t1,t2) = 〈y(t1)y1(t2)〉 by using the approximations 〈φn〉 and 〈φn(t1)φn(t2)〉 , where φn represents n terms of the solution by the iterative method for stochastic differential equations.  相似文献   

9.
A multivariate correlation ratio of a random vector Y upon a random vector X is defined by
ηδ (Y;X)={tr?1 CovE(Y|X))}12 {tr?1Y)}?12
where Λ, a fixed positive definite matrix, is related to the relative importance of predictability for the entries of Y. The properties of ηΛ are discussed, with particular attention paid to a ‘correlation-maximizing’ property. Given are applications of ηΛ to the elliptically symmetric family of distributions and the multinomial distribution. Also discussed is the problem of finding those r linear functions of Y that are most predictable (in a correlation ratio sense) from X.  相似文献   

10.
Sufficient conditions are given for the L2-stability of a class of feedback systems consisting of a linear operator G and a nonlinear gain function, either odd monotone or restricted by a power-law, in cascade, in a negative feedback loop. The criterion takes the form of a frequency-domain inequality, Re[1 + Z()] G() ? δ > 0 ?ω? (?∞, +∞), where Z() is given by, Z() = β[Y1() + Y2()] + (1 ? β)[Y3() ? Y3(?)], with 0 ? β ? 1 and the functions y1(·), y2(·) and y3(·) satisfying the time-domain inequalities, ?∞+∞¦y1(t) + y2(t)¦ dt ? 1 ? ?, y1(·) = 0, t < 0, y2(·) = 0, t > 0 and ? > 0, and 0¦y3(t)¦ dt < 12c2, c2 being a constant depending on the order of the power-law restricting the nonlinear function. The criterion is derived using Zames' passive operator theory and is shown to be more general than the existing criteria.  相似文献   

11.
12.
We prove the existence and uniqueness of a continuous solution F = φ + w of the initial-value problem for vehicular traffic according to the nonlinear Prigogine-Herman model, where φ is a suitable t- and x-independent car distribution.We then show that the perturbation w is strongly continuous and strongly differentiable any number of times with respect to the probability of not passing q. Moreover, the derivatives ?mw?qm (in the strong sense) satisfy linear systems.We finally investigate the behavior of w(t) as t → + ∞ and, under the assumption that the probability of not passing remains unchanged after the instant t = 0, we prove that lim ∥w(t)∥ = 0 as t → + ∞.  相似文献   

13.
{Xn,n?1} are i.i.d. random variables with continuous d.f. F(x). Xj is a record value of this sequence if Xj>max{X1,…,Xj?1}. Consider the sequence of such record values {XLn,n?1}. Set R(x)=-log(1?F(x)). There exist Bn > 0 such that XLnBn→1. in probability (i.p.) iff XLnR-1(n)→1 i.p. iff {R(kx)?R(x)}R12(kx) → ∞ as x→∞ for all k>1. Similar criteria hold for the existence of constants An such that XLn?An → 0 i.p. Limiting record value distributions are of the form N(-log(-logG(x))) where G(·) is an extreme value distribution and N(·) is the standard normal distribution. Domain of attraction criteria for each of the three types of limit laws can be derived by appealing to a duality theorem relating the limiting record value distributions to the extreme value distributions. Repeated use is made of the following lemma: If P{Xn?x}=1?e-x,x?0, then XLn=Y0+…+Yn where the Yj's are i.i.d. and P{Yj?x}=1?e-x.  相似文献   

14.
According to a result of A. Ghizzetti, for any solution y(t) of the differential equation where y(n)(t)+ i=0n?1 gi(t) yi(t)=0 (t ? 1), 1 ¦gi(x)¦xn?I?1 dx < ∞ (0 ?i ? n ?1, either y(t) = 0 for t ? 1 or there is an integer r with 0 ? r ? n ? 1 such that limt → ∞ y(t)tr exists and ≠0. Related results are obtained for difference and differential inequalities. A special case of the former has interesting applications in the study of orthogonal polynomials.  相似文献   

15.
Given a cocycle a(t) of a unitary group {U1}, ?∞ < t < ∞, on a Hilbert space H, such that a(t) is of bounded variation on [O, T] for every T > O, a(t) is decomposed as a(t) = f;t0Usxds + β(t) for a unique x ? H, β(t) yielding a vector measure singular with respect to Lebesgue measure. The variance is defined as σ2({rmUt}, a(t)) = limT→∞(1T)∥∝t0 Us x ds∥2 if existing. For a stationary diffusion process on R1, with Ω1, the space of paths which are natural extensions backwards in time, of paths confined to one nonsingular interval J of positive recurrent type, an information function I(ω) is defined on Ω1, based on the paths restricted to the time interval [0, 1]. It is shown that I(Ω) is continuous and bounded on Ω1. The shift τt, defines a unitary representation {Ut}. Assuming Ω1 I dm = 0, dm being the stationary measure defined by the transition probabilities and the invariant measure on J, I(Ω) has a C spectral density function f;. It is then shown that σ2({Ut}, I) = f;(O).  相似文献   

16.
For Gaussian vector fields {X(t) ∈ Rn:tRd} we describe the covariance functions of all scaling limits Y(t) = Llimα↓0 B?1(α) Xt) which can occur when B(α) is a d × d matrix function with B(α) → 0. These matrix covariance functions r(t, s) = EY(t) Y1(s) are found to be homogeneous in the sense that for some matrix L and each α > 0, (1) r(αt, αs) = αL1r(t, s) αL. Processes with stationary increments satisfying (1) are further analysed and are found to be natural generalizations of Lévy's multiparameter Brownian motion.  相似文献   

17.
We consider a branching diffusion {Zt}t?0 in which particles move during their life time according to a Brownian motion with drift -μ and variance coefficient σ2, and in which each particle which enters the negative half line is instantaneously removed from the population. If particles die with probability c dt+o(dt) in [t,t+dt] and if the mean number of offspring per particle is m>1, then Zt dies out w.p.l. if μ?μ0≡{2σ2c(m?1)}12. If μ<μ0, then itZt grows exponentially with positive probability. Our main concern here is with the critical case where μ=μ0. Even though E{ZT}∽const.T?32 in this case, we find that P{ZT>0} is only exp{–const.T13+0(logT)2}, and conditionally on {ZT>0} there are with high probability much fewer particles alive at time T than E{ZT|ZT0}.  相似文献   

18.
Let X be a Banach space, let B be the generator of a continuous group in X, and let A = B2. Assume that D(Ar) is dense in X for r an arbitrarily large positive integer and that a and b are non-negative reals. Solution representations are developed for the abstract differential equation
(D2t + bt Dt ? A) · (D2t + at Dt ? A) u(t) = 0, t > 0
corresponding to initial conditions of the form: (i) u(0+) = φ, u(j)(0+) = 0, j = 1, 2, 3 and (ii) u2(0+) = φ, uj(0+) = 0, j = 0, 1, 3 (with φD(Ar)) for all choices of a and b.  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.
Let O = limnZ/pnZ, let A = O[g2, g3]Δ, where g2 and g3 are coefficients of the elliptic curve: Y2 = 4X3 ? g2X ? g3 over a finite field and Δ = g23 ? 27g32 and let B = A[X, Y](Y2 ? 4X3 + g2X + g3). Then the p-adic cohomology theory will be applied to compute explicitly the zeta matrices of the elliptic curves, induced by the pth power map on the free A2?ZQ-module H1(X, A2?ZQ). Main results are; Theorem 1.1: X2dY and YdX are basis elements for H1(X, ΓA1(X)2?ZQ); Theorem 1.2: YdX, X2dY, Y?1dX, Y?2dX and XY?2dX are basis elements for H1(X ? (Y = 0), ΓA1(X)2?ZQ), where X is a lifting of X, and all the necessary recursive formulas for this explicit computation are given.  相似文献   

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