On Ergodic Hypothesis

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  • Title: On Ergodic Hypothesis
  • ArXiv ID: 1102.5668
  • Date: 2011-03-01
  • Authors: ** I. Sh. Jabbarov (I. Sh. Jabbarov) **

📝 Abstract

In this paper The Ergodic Hypothesis is proven for one class of functions defined in the infinite dimensional unite cube where is given an action of some semigroup of mappings without the condition on metric transitivity. The result has not a finite analog.

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I. Sh. Jabbarov On Ergodic Hypothesis.

  1. Introduction
    In the theory of stochastic processes The Ergodic Hypothesis of Boltzman (see [6, 7, 8, 14]) is well known. This hypothesis asserts that the average time of a finding of physical systems in some domain of phase space is equal to the relative measure of given domain (see [6], p. 701, [7], p. 522). However, the movement trajectory, in this case, depends on an initial position of a point, and the average on time undertaken irrespectively of it. The exact mathematical formulation of this hypothesis is expressed by a limit relation of a type
      ,) ( ) ( ) ( 1 lim 0          d f dt x T f T T t T (1) where tT some semigroup of mappings of phase space (see [6], [7]), x is, generally speaking, any point of the phase space. We will, at the expense of generality, to consider the problem in such statement. In [2, p. 457] this case is considered for continuous functions f in “a narrowed ergodic” case. Let’s notice that the Ergodic hypothesis, generally, is not true for the function (the example in [8] see, p. 536), accepting value 1 on a given trajectory, and 0, on other points of the phase space. Analogically, it is possible to construct a similar example in the infinite dimensional case. This is clear from the definition of product Lebesgue measure. In the works [6, 7, 8, 14] some have been proved ergodic theorems in which the relation (1) is proved for almost all points x of the phase space.
    In the present work we show that, if as a phase space to consider the cube      ]1,0 [ ]1,0 [ , it is possible to enter such a dynamical system for which the hypothesis mentioned above holds for a certain class of functions and any point x.

Let’s consider the dynamical system defined by a semigroup of mappings: ) (x x t  , where

2 }) ({ } { ) ( n n t t x t x x        , ,   x (the symbol {·} means a fractional part),   ( n ),   n 

is a sequence of positive numbers. Let f be a function defined in ,  ) , ( 0 2   L f where 0  designates the measures in the  introduced in the works [9, 11, 12, 13]. Function   ,… , ) ( 2 1    f f f   can be expanded into the Fourier series f ~ ) , ( 2 ) (  m i e m a  , where    , ,…) , ( 2 1 m m m  and
0  k m for all k m , with exception of finite number of them. Let for any natural N r  the multiple series
    r r Z m m m r m m m a ,…, , 2 1 2 1 ,…) 0, ,…, , (

converges (i.e. the corresponding subseries of given Fourier series converges absolutely). We will say that the function f belongs to the class  J if this condition satisfied for any natural r . Below we use the notions and designations defined in the works [9, 11, 12, 13].

Definition 1. Let N N  :  be any one to one mapping of the set of natural numbers. If for any m n > there is a natural number m such that n n = ) (  , then we call  a finite permutation. A subset   A is called to be finite-symmetrical if for any element A n  ) ( =   and any finite permutation  one has A n  ) (

) (    .

Let    and } | { ) (         . It is a countable set. We will designate ) (  the set of all limit points of the sequence ) (  . For every real t we write }) ({ } { n t t    . Let   ) , ( 2 ,… 1 ) , ( 2 1 ,…) 0, ,… ( ) ( ) (      m i Z m m r m i r e m m a e m a f r r      . The following theorem holds:

Theorem 1. There is a sequence of natural numbers  kr and a subset   0 of full measure such that the series     2 ) ( ) ( 1 k r r k k f f   converges everywhere in 0 .

Thus, the sequence   krf converges in 0  to some function ) ( f . The relation ) ( ) (   f f  is fair almoct everywhere in  and we will prove the relation (1) at first for the function ) ( ) (   f f  .

Theorem 2. For any function  J f the following relation holds                 ) ( ) ( ) ( ) ( 1 lim 0 0 0        d f d f dt t u f T T n T , for any point   u .

3

The increasing sequence of linearly independent frequencies n  plays here an essential role. In H. Bohr’s works [3, 4] averages of a kind (1) on the basis of Croneker’s theorem on the uniform distribution (mod1) of some curves in the multidimensional unite cube are studied. The theorem of
Croneker (see [18, p. 301]) states: Let N    ,…, , 2 1 be real numbers linearly independent over the field of rational numbers,  be a subdomain of N – dimensional unite cube with the volume  in Jordan meaning. Let further, ) (T I is a measure of a set of such ) ,0 ( T t  for which )1 (mod ) ,…, , ( 2 1      t t t N . Then . ) ( lim     T T I T 

Later the theory of uniform distribution of curves has been generalized and deeply studied by many other authors (see [15]). Generalization of this theory to the curves given by functions

Reference

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