共查询到20条相似文献,搜索用时 15 毫秒
1.
We prove that the Birkhoff sums for ``almost every' relevant observable in the stadium billiard obey a non-standard limit
law. More precisely, the usual central limit theorem holds for an observable if and only if its integral along a one-codimensional
invariant set vanishes, otherwise a normalization is needed. As one of the two key steps in the argument, we obtain a limit theorem that holds in Young towers
with exponential return time statistics in general, an abstract result that seems to be applicable to many other situations. 相似文献
2.
We study deviation of ergodic averages for dynamical systems given by self-similar tilings on the plane and in higher dimensions. The main object of our paper is a special family of finitely-additive measures for our systems. An asymptotic formula is given for ergodic integrals in terms of these finitely-additive measures, and, as a corollary, limit theorems are obtained for dynamical systems given by self-similar tilings. 相似文献
3.
Suppose B i := B( p, r i ) are nested balls of radius r i about a point p in a dynamical system ( T, X, μ). The question of whether T i x∈ B i infinitely often (i.o.) for μ a.e. x is often called the shrinking target problem. In many dynamical settings it has been shown that if $E_{n}:=\sum_{i=1}^{n} \mu(B_{i})$ diverges then there is a quantitative rate of entry and $\lim_{n\to\infty} \frac{1}{E_{n}} \sum_{j=1}^{n} 1_{B_{i}} (T^{i} x) \to1$ for μ a.e. x∈ X. This is a self-norming type of strong law of large numbers. We establish self-norming central limit theorems (CLT) of the form $\lim_{ n\to\infty} \frac{1}{a_{n}} \sum_{i=1}^{n} [1_{B_{i}} (T^{i} x)-\mu(B_{i})] \to N(0,1)$ (in distribution) for a variety of hyperbolic and non-uniformly hyperbolic dynamical systems, the normalization constants are $a^{2}_{n} \sim E [\sum_{i=1}^{n} 1_{B_{i}} (T^{i} x)-\mu(B_{i})]^{2}$ . Dynamical systems to which our results apply include smooth expanding maps of the interval, Rychlik type maps, Gibbs-Markov maps, rational maps and, in higher dimensions, piecewise expanding maps. For such central limit theorems the main difficulty is to prove that the non-stationary variance has a limit in probability. 相似文献
4.
We study occurrences of patterns on clusters of size n in random fields on ℤ
d
. We prove that for a given pattern, there is a constant a>0 such that the probability that this pattern occurs at most na times on a cluster of size n is exponentially small. Moreover, for random fields obeying a certain Markov property, we show that the ratio between the
numbers of occurrences of two distinct patterns on a cluster is concentrated around a constant value. This leads to an elegant
and simple proof of the ratio limit theorem for these random fields, which states that the ratio of the probabilities that
the cluster of the origin has sizes n+1 and n converges as n→∞. Implications for the maximal cluster in a finite box are discussed. 相似文献
5.
Suppose \(\{T^t\}\) is a Borel flow on a complete separable metric space X, \(f:X\rightarrow \mathbb R\) is Borel, and \(x\in X\). A temporal distributional limit theorem is a scaling limit for the distributions of the random variables \(X_T:=\int _0^t f(T^s x)ds\), where t is chosen randomly uniformly from [0, T], x is fixed, and \(T\rightarrow \infty \). We discuss such laws for irrational rotations, Anosov flows, and horocycle flows. 相似文献
6.
We consider the limit distributions of open quantum random walks on one-dimensional lattice space. We introduce a dual process to the original quantum walk process, which is quite similar to the relation of Schrödinger-Heisenberg representation in quantum mechanics. By this, we can compute the distribution of the open quantum random walks concretely for many examples and thereby we can also obtain the limit distributions of them. In particular, it is possible to get rid of the initial state when we consider the evolution of the walk, it appears only in the last step of the computation. 相似文献
7.
Dispersing billiards with cusps are deterministic dynamical systems with a mild degree of chaos, exhibiting “intermittent” behavior that alternates between regular and chaotic patterns. Their statistical properties are therefore weak and delicate. They are characterized by a slow (power-law) decay of correlations, and as a result the classical central limit theorem fails. We prove that a non-classical central limit theorem holds, with a scaling factor of \({\sqrt{n\log n}}\) replacing the standard \({\sqrt{n}}\) . We also derive the respective Weak Invariance Principle, and we identify the class of observables for which the classical CLT still holds. 相似文献
8.
We consider a deposition model in which balls rain down at random towards a 2-dimensional surface, roll downwards over existing adsorbed balls, are adsorbed if they reach the surface, and discarded if not. We prove a spatial law of large numbers and central limit theorem for the ultimate number of balls adsorbed onto a large toroidal surface, and also for the number of balls adsorbed on the restriction to a large region of an infinite surface. 相似文献
12.
Let a random variable x
0 and a function f:[ a, b]
k
[ a, b] be given. A hierarchical sequence { x
n
: n=0, 1, 2,...} of random variables is defined inductively by the relation x
n
= f( x
n–1, 1, x
n–1, 2..., x
n–1, k
), where { x
n–1, i
: i=1, 2,..., k} is a family of independent random variables with the same distribution as x
n–1. We prove a central limit theorem for this hierarchical sequence of random variables when a function f satisfies a certain averaging condition. As a corollary under a natural assumption we prove a central limit theorem for a suitably normalized sequence of conductivities of a random resistor network on a hierarchical lattice. 相似文献
13.
We consider the open quantum random walks on the crystal lattices and investigate the central limit theorems for the walks. On the integer lattices the open quantum random walks satisfy the central limit theorems as was shown by Attal et al (Ann Henri Poincaré 16(1):15–43, 2015). In this paper we prove the central limit theorems for the open quantum random walks on the crystal lattices. We then provide with some examples for the Hexagonal lattices. We also develop the Fourier analysis on the crystal lattices. This leads to construct the so called dual processes for the open quantum random walks. It amounts to get Fourier transform of the probability densities, and it is very useful when we compute the characteristic functions of the walks. In this paper we construct the dual processes for the open quantum random walks on the crystal lattices providing with some examples. 相似文献
14.
We introduce a solvable model of randomly growing systems consisting of many independent subunits. Scaling relations and growth rate distributions in the limit of infinite subunits are analysed theoretically. Various types of scaling properties and distributions reported for growth rates of complex systems in a variety of fields can be derived from this basic physical model. Statistical data of growth rates for about 1 million business firms are analysed as a real-world example of randomly growing systems. Not only are the scaling relations consistent with the theoretical solution, but the entire functional form of the growth rate distribution is fitted with a theoretical distribution that has a power-law tail. 相似文献
15.
The limit log-infinitely divisible multifractals of Muzy and Bacry (Phys. Rev. E 66:056121, 2002) are reviewed and shown to possess novel invariance relations that translate into functional Feynman-Kac equations for the corresponding probability distributions. In the special case of the limit lognormal process of Mandelbrot (in Statistical Models and Turbulence, M. Rosenblatt, C. Van Atta (Eds.), Springer, New York, 1972), the limit distribution is represented exactly in an operator form using the technique of intermittency expansions. A novel representation for the Mellin transform of the limit distribution is derived and related to the Hurwitz zeta function. For application, the cumulants of the logarithm of the limit lognormal distribution are computed explicitly. 相似文献
16.
We show central limit theorems (CLT) for the linear statistics of symmetric matrices with independent heavy tailed entries, including entries in the domain of attraction of α-stable laws and entries with moments exploding with the dimension, as in the adjacency matrices of Erdös-Rényi graphs. For the second model, we also prove a central limit theorem of the moments of its empirical eigenvalues distribution. The limit laws are Gaussian, but unlike the case of standard Wigner matrices, the normalization is the one of the classical CLT for independent random variables. 相似文献
17.
We give a general method for deducing statistical limit laws in situations where rapid decay of correlations has been established.
As an application of this method, we obtain new results for time-one maps of hyperbolic flows.
In particular, using recent results of Dolgopyat, we prove that many classical limit theorems of probability theory, such
as the central limit theorem, the law of the iterated logarithm, and approximation by Brownian motion (almost sure invariance
principle), are typically valid for such time-one maps.
The central limit theorem for hyperbolic flows goes back to Ratner 1973 and is always valid, irrespective of mixing hypotheses.
We give examples which demonstrate that the situation for time-one maps is more delicate than that for hyperbolic flows, illustrating
the need for rapid mixing hypotheses.
Received: 4 January 2002 / Accepted: 16 February 2002?Published online: 24 July 2002 相似文献
18.
We derive probabilistic limit theorems that reveal the intricate structure of the phase transitions in a mean-field version
of the Blume–Emery–Griffiths model [ Phys. Rev. A
4 (1971) 1071–1077]. These probabilistic limit theorems consist of scaling limits for the total spin and moderate deviation
principles (MDPs) for the total spin. The model under study is defined by a probability distribution that depends on the parameters
n, β, and K, which represent, respectively, the number of spins, the inverse temperature, and the interaction strength. The intricate
structure of the phase transitions is revealed by the existence of 18 scaling limits and 18 MDPs for the total spin. These
limit results are obtained as (β, K) converges along appropriate sequences (β n, kn) to points belonging to various subsets of the phase diagram, which include a curve of second-order points and a tricritical
point. The forms of the limiting densities in the scaling limits and of the rate functions in the MDPs reflect the influence
of one or more sets that lie in neighborhoods of the critical points and the tricritical point. Of all the scaling limits,
the structure of those near the tricritical point is by far the most complex, exhibiting new types of critical behavior when
observed in a limit-theorem phase diagram in the space of the two parameters that parametrize the scaling limits.
American Mathematical Society 2000 Subject Classifications. Primary 60F10, 60F05, Secondary 82B20 相似文献
19.
We consider a finite sequence of random points in a finite domain of finite-dimensional Euclidean space. The points are sequentially allocated in the domain according to the model of cooperative sequential adsorption. The main peculiarity of the model is that the probability distribution of any point depends on previously allocated points. We assume that the dependence vanishes as the concentration of points tends to infinity. Under this assumption the law of large numbers, Poisson approximation and the central limit theorem are proved for the generated sequence of random point measures. 相似文献
20.
We provide a general study on quadratic Poisson structures on a vector space. In particular, we obtain a decomposition for any quadratic Poisson structures. As an application, we classify all the three-dimensional quadratic Poisson structures up to a Poisson diffeomorphism.Research partially supported by NSF Grant DMS 90-01956 and Research Foundation of the University of Pennsylvania. 相似文献
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