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    <link>http://bactra.org/notebooks/2007/10/29#ergodic-theory</link>
    <description>Ergodic Theory 



&lt;P&gt;A measure on a mathematical space is a way of assigning weights to different 
parts of the space; volume is a measure on ordinary three-dimensional Euclidean 
space.  Probability distributions are measures, such that the largest measure 
of any set is 1 (and some other restrictions).  Suppose we're interested in a 
dynamical system --- a transformation that maps a space into itself.  The set 
of points we get from applying the transformation repeatedly to a point is 
called its trajectory or orbit.  Some dynamical systems are &lt;em&gt;measure 
preserving,&lt;/em&gt; meaning that the measure of a set is always the same as the 
measure of the set of points which map to it.  (In symbols, using &lt;em&gt;T&lt;/em&gt; 
for the map and &lt;em&gt;P&lt;/em&gt; for the probability measure,  
&lt;img align=absmiddle src=&quot;ergodic-theory_1.gif&quot; alt=&quot;$ P(T^{-1}(A)) = 
P(A) $ &quot;&gt;
 for any measureable set &lt;em&gt;A&lt;/em&gt;.)  Some sets may be invariant: 
they are the same as their images.  An ergodic dynamical system is one in 
which, with respect to some probability distribution, all invariant sets either 
have measure 0 or measure 1.  (Sometimes non-ergodic systems can be decomposed 
into a number of components, each of which is separately ergodic.)  The 
dynamics need not be deterministic; in particular, irreducible Markov chains 
with finite state spaces are ergodic processes, since they have a unique 
invariant distribution over the states.  (In the Markov chain case, each of the 
ergodic components corresponds to an irreducible sub-space.) 

&lt;P&gt;Ergodicity is important because of the following theorem (due to von 
Neumann, and then improved substantially by Birkhoff, in the 1930s).  If we 
take any well-behaved (integrable) function of our space, pick a point in the 
space at random (according to the ergodic distribution) and calculate the 
average of the function along the point's orbit, the time-average.  Then, with 
probability 1, in the limit as the time goes to infinity, (1) the time-average 
converges to a limit and (2) that limit is equal to the weighted average of the 
value of the function at all points in the space (with the weights given by the 
same distribution), the space-average.  The orbit of almost any point you 
please will in some sense look like the whole of the state space. 

&lt;P&gt;(Symbolically, write &lt;em&gt;x&lt;/em&gt; for a point in the state 
space, &lt;em&gt;f&lt;/em&gt; for the function we're averaging, and &lt;em&gt;T&lt;/em&gt; and 
&lt;em&gt;P&lt;/em&gt; for the map and the probability measure as before.  The 
space-average,  
&lt;img align=absmiddle src=&quot;ergodic-theory_2.gif&quot; alt=&quot;$ \overline{f} = \int{f(x)P(dx)} $ &quot;&gt;
.  The time-average 
starting from &lt;em&gt;x&lt;/em&gt;,  
&lt;img align=absmiddle src=&quot;ergodic-theory_3.gif&quot; alt=&quot;$ {\langle f\rangle}_x = 
\lim_{n\rightarrow\infty}{(1/n) \sum_{i=0}^{n}{f(T^i(x))}} $ &quot;&gt;
.  The ergodic 
theorem asserts that if &lt;em&gt;f&lt;/em&gt; is integrable and &lt;em&gt;T&lt;/em&gt; is ergodic 
with respect to &lt;em&gt;P&lt;/em&gt;, then  
&lt;img align=absmiddle src=&quot;ergodic-theory_4.gif&quot; alt=&quot;$ {\langle f \rangle}_x $ &quot;&gt;
 exists, 
and  
&lt;img align=absmiddle src=&quot;ergodic-theory_5.gif&quot; alt=&quot;$ P\left\{x : {\langle f \rangle}_x = \overline{f} \right\} = 
1 $ &quot;&gt;
.  --- A similar result holds for continuous-time dynamical systems, 
where we replace the summation in the time average with an integral.) 

&lt;P&gt;This is an extremely important property for statistical mechanics.  In fact, 
the founder of statistical mechanics, Ludwig Boltzmann, coined &quot;ergodic&quot; as the 
name for a stronger but related property: starting from a random point in state 
space, orbits will typically pass through every point in state space.  It is 
easy to show (with set theory) that this isn't doable, so people appealled to a 
weaker property which was for a time known as &quot;quasi-ergodicity&quot;: a typical 
trajectory will pass &lt;em&gt;arbitrarily close&lt;/em&gt; to every point in phase space. 
Finally it became clear that only the modern ergodic property is needed.  To 
see the relation, consider the function, call it &lt;em&gt;I&lt;/em&gt;, which is 1 on a 
certain set, call it &lt;em&gt;A&lt;/em&gt;, and 0 elsewhere.  The time-average 
of &lt;em&gt;I&lt;/em&gt; is the fraction of time that the orbit spends in &lt;em&gt;A&lt;/em&gt;.  The 
space-average of &lt;em&gt;I&lt;/em&gt; is the probability that a randomly picked point is 
in &lt;em&gt;A&lt;/em&gt;.  Since the two averages are almost always equal, almost all 
trajectories end up covering the state space in the same way. 

&lt;P&gt;One way of thinking about the classical ergodic theorem is that it's a 
version of the law of large numbers --- it tells us that a sufficiently large 
sample (i.e., an average over a long time) is representative of the whole 
population (i.e., the space average).  One thing I'd like to know more about 
than I do is ergodic equivalents of the central limit theorem, which say how 
big the sampling fluctuations are, and how they're distributed.  The other 
thing I want to know about is the rate of convergence in the ergodic theorem 
--- how long must I wait before my time average is within a certain margin of 
probable error of the state average.  Here I do know a bit more of the relevant 
literature, from &lt;a href=&quot;large-deviations.html&quot;&gt;large deviations theory&lt;/a&gt;. 

&lt;P&gt;Again in symbols: Let's write  
&lt;img align=absmiddle src=&quot;ergodic-theory_6.gif&quot; alt=&quot;$ {\langle f\rangle}_{x,n} $ &quot;&gt;
 for the 
time-average of &lt;em&gt;f&lt;/em&gt;, starting from &lt;em&gt;x&lt;/em&gt;, taken over &lt;em&gt;n&lt;/em&gt; 
steps.  Then a central-limit theorem result would say that (for example) 
 
&lt;img align=absmiddle src=&quot;ergodic-theory_7.gif&quot; alt=&quot;$ \frac{{\langle f\rangle}_{X,n} - \overline{f}}{\sigma^{2}r(n)} $ &quot;&gt;

converges in distribution to a Gaussian with mean zero and variance one, where 
 
&lt;img align=absmiddle src=&quot;ergodic-theory_8.gif&quot; alt=&quot;$ \sigma^2 $ &quot;&gt;
 is the (space-averaged) variance of &lt;em&gt;f&lt;/em&gt; and 
 
&lt;img align=absmiddle src=&quot;ergodic-theory_9.gif&quot; alt=&quot;$ r(n) $ &quot;&gt;
 is some positive, increasing function of &lt;em&gt;n&lt;/em&gt;.  This 
would be weak convergence of the time averages to the space averages, and 
 
&lt;img align=absmiddle src=&quot;ergodic-theory_10.gif&quot; alt=&quot;$ r(n) $ &quot;&gt;
 would give the rate.  (In the usual IID case,  
&lt;img align=absmiddle src=&quot;ergodic-theory_11.gif&quot; alt=&quot;$ r(n) = 
\sqrt{n} $ &quot;&gt;
.)  Somewhat stronger would be a convegence in probability 
result, giving us a function  
&lt;img align=absmiddle src=&quot;ergodic-theory_12.gif&quot; alt=&quot;$ N(\varepsilon,\delta) $ &quot;&gt;
 such that 
 
&lt;img align=absmiddle src=&quot;ergodic-theory_13.gif&quot; alt=&quot;$ P\left\{x : \left|{\langle f\rangle}_{x,n} - \overline{f}\right| \geq 
\varepsilon \right\} \leq \delta $ &quot;&gt;
 if  
&lt;img align=absmiddle src=&quot;ergodic-theory_14.gif&quot; alt=&quot;$ n \geq 
N(\varepsilon,\delta) $ &quot;&gt;
.  Proving many of these results requires stronger 
assumptions than proving ergodicity does --- for instance, Markov properties, 
or mixing properties (which I should explain here, but won't). 

&lt;P&gt;These issues are part of a more general question about how to do statistical 
inference for stochastic processes, a.k.a. time-series analysis.  I am 
especially interested in &lt;a href=&quot;dependent-learning.html&quot;&gt;statistical learning 
theory&lt;/a&gt; in this setting. 

&lt;P&gt;Another thing I need to understand, but don't have time to explain here, 
are Pinsker sigma-algebras. 

&lt;P&gt;&lt;em&gt;See also&lt;/em&gt;: 
	&lt;a href=&quot;chaos.html&quot;&gt;Dynamical Systems and Chaos&lt;/a&gt;; 
	&lt;a href=&quot;empirical-process-theory.html&quot;&gt;Empirical Process Theory&lt;/a&gt;; 
	&lt;a href=&quot;information-theory.html&quot;&gt;Information Theory&lt;/a&gt;; 
	&lt;a href=&quot;noneq-sm.html&quot;&gt;Nonequilibrium Statistical Mechanics&lt;/a&gt;; 
	&lt;a href=&quot;probability.html&quot;&gt;Probability Theory&lt;/a&gt;; 
	&lt;a href=&quot;recurrence-times.html&quot;&gt;Recurrence Times of Stochastic 
Processes&lt;/a&gt;; 
	&lt;a href=&quot;stochastic-processes.html&quot;&gt;Stochastic Processes&lt;/a&gt;; 
	&lt;a href=&quot;symbolic-dynamics.html&quot;&gt;Symbolic Dynamics&lt;/a&gt;; 
	&lt;a href=&quot;time-series.html&quot;&gt;Time Series&lt;/a&gt;; 
	&lt;a href=&quot;universal-prediction.html&quot;&gt;Universal Prediction Algorithms&lt;/a&gt; 

&lt;ul&gt;Recommended, synoptic: 
	&lt;li&gt;Peter Billingsley, &lt;cite&gt;Ergodic Theory and Information&lt;/cite&gt; 
	&lt;li&gt;Robert M. Gray, &lt;cite&gt;Probability, Random Processes, and Ergodic 
Properties&lt;/cite&gt; 
[&lt;a href=&quot;http://ee-www.stanford.edu/~gray/arp.html&quot;&gt;Full-text online&lt;/a&gt;] 
	&lt;li&gt;A. I. Khinchin, &lt;cite&gt;Mathematical Foundations of Statistical 
Mechanics&lt;/cite&gt; [Proves the von Neumann-Birkhoff ergodic theorem in detail] 
	&lt;li&gt;Mark Kac, &lt;cite&gt;Probability and Related Topics in Physical 
Science&lt;/cite&gt; 
	&lt;li&gt;Andrzej Lasota and Michael C. Mackey, &lt;cite&gt;Chaos, Fractals and 
Noise: Stochastic Aspects of Dynamics&lt;/cite&gt; 
	&lt;li&gt;&lt;a href=&quot;wiener.html&quot;&gt;Norbert Wiener&lt;/a&gt;, &lt;cite&gt;Cybernetics: Or 
Control and Communication in the Animal and the Machine&lt;/cite&gt; 
	&lt;/ul&gt; 

&lt;ul&gt;Recommended, close-up: 
	&lt;li&gt;J.-R. Chazottes and R. Leplaideur, &quot;Birkhoff averages of Poincare 
cycles for Axiom-A diffeomorphisms,&quot; &lt;a 
href=&quot;http://arxiv.org/abs/math.DS/0312291&quot;&gt;math.DS/0312291&lt;/a&gt; 
	&lt;li&gt;J&amp;eacute;r&amp;ocirc;me Dedecker, Paul Doukhan, Gabriel Lang, 
Jos&amp;eacute; Rafael Le&amp;oacute;n R., Sana Louhichi and Cl&amp;eacute;mentine 
Prieur, &lt;cite&gt;Weak Dependence: With Examples and Applications&lt;/cite&gt; [&lt;a href=&quot;../weblog/algae-2009-04.html#weak&quot;&gt;Mini-review&lt;/a&gt;] 
	&lt;li&gt;Paul Doukhan, &lt;cite&gt;Mixing: Properties and Examples&lt;/cite&gt; 
	&lt;li&gt;E. B. Dynkin, &quot;Sufficient statistics and extreme 
points&quot;, &lt;cite&gt;Annals of Probability&lt;/cite&gt; &lt;strong&gt;6&lt;/strong&gt; (1978): 705--730 
[&quot;The connection between ergodic decompositions 
and &lt;a href=&quot;sufficient-statistics.html&quot;&gt;sufficient statistics&lt;/a&gt; is explored 
in an elegant paper by DYNKIN&quot; --- Kallenberg, &lt;cite&gt;Foundations of Modern 
Probability&lt;/cite&gt;, p. 577] 
	&lt;li&gt;Jean-Pierre Eckmann and David Ruelle, &quot;Ergodic Theory of 
Chaos and Strange Attractors,&quot; &lt;cite&gt;Reviews of Modern Physics&lt;/cite&gt; 
&lt;strong&gt;57&lt;/strong&gt; (1985): 617--656 
	&lt;li&gt;Roberto Fern&amp;aacute;ndez and Gr&amp;eacute;gory Maillard, &quot;Chains with 
Complete Connections: General Theory, Uniqueness, Loss of Memory and Mixing 
Properties&quot;, &lt;a 
href=&quot;http://dx.doi.org/10.1007/s10955-004-8821-5&quot;&gt;&lt;cite&gt;Journal of Statistical 
Physics&lt;/cite&gt; &lt;strong&gt;118&lt;/strong&gt; (2005): 555--588&lt;/a&gt; 
	&lt;li&gt;Stefano Galatolo, Mathieu Hoyrup, and Crist&amp;oacute;bal Rojas, 
&quot;Effective symbolic dynamics, random points, statistical behavior, complexity 
and entropy&quot;, &lt;a href=&quot;http://arxiv.org/abs/0801.0209&quot;&gt;arxiv:0801.0209&lt;/a&gt; 
[&lt;em&gt;All&lt;/em&gt;, not almost all, Martin-L&amp;ouml;f points are statistically 
typical.] 
	&lt;li&gt;Weihong Huang, &quot;On the long-run average growth rate of chaotic 
systems&quot;, &lt;cite&gt;Chaos&lt;/cite&gt; &lt;strong&gt;14&lt;/strong&gt; (2004): 38--47 [An amusing 
demonstration that positive-valued ergodic processes will seem to always have a 
positive long-run growth rate, even though they're stationary!] 
	&lt;li&gt;Michael Keane and Karl Petersen, &quot;Easy and nearly simultaneous 
proofs of the Ergodic Theorem and Maximal Ergodic 
Theorem&quot;, &lt;a href=&quot;http://arxiv.org/abs/math.DS/0608251&quot;&gt;math.DS/0608251&lt;/a&gt; 
[This is a &lt;em&gt;lovely&lt;/em&gt; little four-page paper, and the simplest proof by 
far that I've seen, but they do rely rather heavily on the reader being 
familiar with facts about time averages, invariant functions, etc.  Still, I 
should definitely teach this 
in &lt;a href=&quot;http://www.stat.cmu.edu/~cshalizi/almost-none/&quot;&gt;my class&lt;/a&gt;.] 
	&lt;li&gt;Aryeh (Leo) Kontorovich, &quot;Metric and Mixing Sufficient Conditions 
for Concentration of 
Measure&quot;, &lt;a href=&quot;http://arxiv.org/abs/math.PR/0610427&quot;&gt;math.PR/0610427&lt;/a&gt; 
[See &lt;a href=&quot;http://bactra.org/weblog/464.html&quot;&gt;weblog comments&lt;/a&gt;] 
	&lt;li&gt;Aryeh Kontorovich and Anthony Brockwell, &quot;A Strong Law of Large Numbers for Strongly Mixing Processes&quot;, &lt;a href=&quot;http://arxiv.org/abs/0807.4665&quot;&gt;arxiv:0807.4665&lt;/a&gt; 
	&lt;li&gt;Michael C. Mackey, &lt;cite&gt;Time's Arrow: The Origins of Thermodynamic 
Behavior&lt;/cite&gt; 
	&lt;li&gt;Florence Merlev&amp;egrave;de, Magda Peligrad, Sergey Utev, &quot;Recent 
advances in invariance principles for stationary 
sequences&quot;, &lt;a href=&quot;http://arxiv.org/abs/math.PR/0601315&quot;&gt;math.PR/0601315&lt;/a&gt; 
= &lt;a href=&quot;http://dx.doi.org/10%2E1214/154957806100000202&quot;&gt;&lt;cite&gt;Probability 
Surveys&lt;/cite&gt; &lt;strong&gt;3&lt;/strong&gt; (2006): 1--36&lt;/a&gt; [Can I just say how much I 
hate calling the functional central limit theorem &quot;&lt;em&gt;the&lt;/em&gt; invariance 
principle&quot;?] 
	&lt;li&gt;Mehryar Mohri and Afshin Rostamizadeh, &quot;Stability Bound for 
Stationary Phi-mixing and Beta-mixing 
Processes&quot;, &lt;a href=&quot;http://arxiv.org/abs/0811.1629&quot;&gt;arxiv:0811.1629&lt;/a&gt; 
[&quot;Stability&quot; is the property of a learning algorithm that changing a single 
observation in the training set leads to only small changes in predictions on 
the test set.  This paper shows that stable learning algorithms continue to 
perform well with dependent data, provided the data are either phi mixing 
or beta mixing.  The results for phi-mixing depend on Leo's work.] 
	&lt;li&gt;Andrew Nobel and Amir Dembo, &quot;A Note on Uniform Laws of Averages for Dependent Processes&quot;, &lt;citE&gt;Statistics and Probability Letters&lt;/cite&gt; 
&lt;strong&gt;17&lt;/strong&gt; (1993): 169--172 [An extremely easy way to extend uniform 
laws of large numbers to uniform ergodic theorems for mixing processes. 
Actually I suspect that mixing is only necessary to get an explicit rate; I 
should re-read 
it.  &lt;a 
href=&quot;http://stat-or.unc.edu/webspace/public_html.stat/faculty/nobel/links/Papers/ULA-wkbern.pdf&quot;&gt;PDF 
preprint&lt;/a&gt; via Dr. Nobel.] 
	&lt;li&gt;Donald Ornstein and Benjamin Weiss, &quot;How Sampling Reveals a 
Process&quot;, &lt;a href=&quot;http://dx.doi.org/10.1214/aop/1176990729&quot;&gt;&lt;cite&gt;Annals of 
Probability&lt;/cite&gt; &lt;strong&gt;18&lt;/strong&gt; (1990): 905--930&lt;/a&gt; [Open access.  Some 
comments under &lt;a href=&quot;universal-prediction.html&quot;&gt;Universal Prediction&lt;/a&gt;.] 
	&lt;li&gt;Murray Rosenblatt, &quot;A Central Limit Theorem and a Strong Mixing 
Condition&quot;, &lt;cite&gt;Proceedings of the National Academy of Sciences&lt;/cite&gt; 
(USA) &lt;strong&gt;42&lt;/strong&gt; (1956): 43--47 [The root from which much subsequent 
ergodic theory has 
sprung.  &lt;a href=&quot;http://www.pnas.org/cgi/reprint/42/1/43&quot;&gt;PDF reprint&lt;/a&gt;] 
	&lt;li&gt;Daniil Ryabko and Boris Ryabko, &quot;Testing Statistical Hypotheses 
About Ergodic 
Processes&quot;, &lt;a href=&quot;http://arxiv.org/abs/0804.0510&quot;&gt;arxiv:0804.0510&lt;/a&gt; 
	&lt;li&gt;Nobusumi Sagara, &quot;Nonparametric maximum-likelihood estimation of 
probability measures: existence and consistency&quot;, &lt;a 
href=&quot;http://dx.doi.org/10.1016/j.jspi.2004.03.017&quot;&gt;&lt;cite&gt;Journal of 
Statistical Planning and Inference&lt;/cite&gt; &lt;strong&gt;133&lt;/strong&gt; (2005): 
249--271&lt;/a&gt; [&quot;This paper formulates the nonparametric maximum-likelihood 
estimation of probability measures and generalizes the consistency result on 
the maximum-likelihood estimator (MLE). We drop the independent assumption on 
the underlying stochastic process and replace it with the assumption that the 
stochastic process is stationary and ergodic. The present proof employs 
Birkhoff's ergodic theorem and the martingale convergence theorem. The main 
result is applied to the parametric and nonparametric maximum-likelihood 
estimation of density functions.&quot;  &lt;em&gt;Very&lt;/em&gt; cool.] 
	&lt;li&gt;Paul C. Shields, &lt;cite&gt;The Ergodic Theory of Discrete Sample 
Paths&lt;/cite&gt; [Well-written modern text, extremely strong on connections 
to &lt;a href=&quot;information-theory.html&quot;&gt;information theory and coding&lt;/a&gt;.  I 
haven't gotten through the last chapter, however. 
Shield's &lt;a href=&quot;http://www.math.utoledo.edu/~pshields/ergodic.html&quot;&gt;page on 
the book&lt;/a&gt;.] 
	&lt;li&gt;Leslie Sklar, &lt;cite&gt;Physics and Chance: Philosophical Issues in the 
Foundations of Statistical Mechanics&lt;/cite&gt; [Good discussion of ergodic results 
in several places] 
	&lt;li&gt;Marta Tyran-Kaminska, &quot;An Invariance Principle for Maps with 
Polynomial Decay of Correlations&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/math.DS/0408185&quot;&gt;math.DS/0408185&lt;/a&gt; = 
&lt;a href=&quot;http://dx.doi.org/10.1007/s00220-005-1400-z&quot;&gt;&lt;cite&gt;Communications in 
Mathematical Physics&lt;/cite&gt; &lt;strong&gt;260&lt;/strong&gt; (2005): 1--15&lt;/a&gt; [&quot;We give a 
general method of deriving statistical limit theorems, such as the central 
limit theorem and its functional version, in the setting of ergodic measure 
preserving transformations. This method is applicable in situations where the 
iterates of discrete time maps display a polynomial decay of correlations.&quot;] 
	&lt;li&gt;Mathukumalli Vidyasagar, &lt;cite&gt;A Theory of Learning and 
Generalization: With Applications to Neural Networks and Control Systems&lt;/cite&gt; 
[Has a very nice discussion of when the uniform laws of large numbers 
of &lt;a href=&quot;learning-theory.html&quot;&gt;statistical learning theory&lt;/a&gt; transfer from 
the usual IID setting to dependent processes, becoming uniform ergodic 
theorems. (Sufficient conditions include things like beta-mixing, but necessary 
and sufficient conditions seem to still be 
unknown.)  &lt;a href=&quot;../weblog/algae-209-01.html#vidyasagar&quot;&gt;Mini-review&lt;/a&gt;] 
	&lt;li&gt;Benjamin Weiss, &lt;cite&gt;Single Orbit Dynamics&lt;/cite&gt; 
	&lt;li&gt;Wei Biao Wu, &quot;Nonlinear system theory: Another look at 
dependence&quot;, &lt;a 
href=&quot;http://dx.doi.org/10.1073/pnas.0506715102&quot;&gt;&lt;cite&gt;Proceedings of the 
National Academy of Sciences&lt;/cite&gt; &lt;strong&gt;102&lt;/strong&gt; (2005): 
14150--14154&lt;/a&gt; [&quot;we introduce [new] dependence measures for stationary causal 
processes. Our physical and predictive dependence measures quantify the degree 
of dependence of outputs on inputs in physical systems. The proposed dependence 
measures provide a natural framework for a limit theory for stationary 
processes. In particular, under conditions with quite simple forms, we present 
limit theorems for partial sums, empirical processes, and kernel density 
estimates. The conditions are mild and easily verifiable because they are 
directly related to the data-generating mechanisms.&quot;  Proofs rely heavily on 
results from Wu's other papers, which I have yet to read.] 
	&lt;/ul&gt; 

&lt;ul&gt;Modesty forbids me to recommend: 
	&lt;li&gt;chs. 5 and 22--27 of &lt;cite&gt;&lt;a href=&quot;http://www.stat.cmu.edu/~cshalizi/almost-none&quot;&gt;Almost None of the Theory of Stochastic Processes&lt;/a&gt;&lt;/cite&gt; 
	&lt;/ul&gt; 

&lt;ul&gt;To read: 
	&lt;li&gt;Jon Aaronson, &lt;cite&gt;An Introduction to Infinite Ergodic 
Theory&lt;/cite&gt; [&lt;a href=&quot;http://www.oup.co.uk/isbn/0-8218-0494-4&quot;&gt;Blurb&lt;/a&gt;] 
	&lt;li&gt;Jon Aaronson and Tom Meyerovitch, &quot;Absolutely continuous, invariant 
measures for dissipative, ergodic transformations&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/math.DS/0509093&quot;&gt;math.DS/0509093&lt;/a&gt; [&quot;We show that 
a dissipative, ergodic measure preserving transformation of a sigma-finite, 
non-atomic measure space always has many non-proportional, absolutely 
continuous, invariant measures and is ergodic with respect to each one of 
these.&quot;] 
	&lt;li&gt;Jose M. Amigo, Matthew B. Kennel and Ljupco Kocarev, &quot;The 
permutation entropy rate equals the metric entropy rate for ergodic information 
sources and ergodic dynamical systems&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/nlin.CD/0503044&quot;&gt;nlin.CD/0503044&lt;/a&gt; 
	&lt;li&gt;Vitor Araujo, &quot;Semicontinuity of entropy, existence of equilibrium 
states and of physical measures&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/math.DS/0410099&quot;&gt;math.DS/0410099&lt;/a&gt; 
	&lt;li&gt;L. Arnold, &lt;citE&gt;Random Dynamical Systems&lt;/cite&gt; 
	&lt;li&gt;V. I. Arnol'd and A. Avez, &lt;cite&gt;Ergodic Problems of Classical 
Mechanics&lt;/cite&gt; 
	&lt;li&gt;Jeremy Avigad, Philipp Gerhardy and Henry Towsner, &quot;Local stability 
of ergodic 
averages&quot;, &lt;a href=&quot;http://arxiv.org/abs/0706.1512&quot;&gt;arxiv:0706.1512&lt;/a&gt; 
[Computing bounds on the rate of convergence in the ergodic theorems; sound 
scool.  Thanks to &lt;a href=&quot;http://www.optimizelife.com&quot;&gt;Gustavo Lacerda&lt;/a&gt; for 
the pointer.] 
	&lt;li&gt;Massimiliano Badino, &quot;The Foundational Role of Ergodic Theory&quot;, 
&lt;a href=&quot;http://philsci-archive.pitt.edu/archive/00002277/&quot;&gt;phil-sci/2277&lt;/a&gt; 
	&lt;li&gt;Dominique Bakry, Patrick Cattiaux, Arnaud Guillin, &quot;Rate of 
Convergence for ergodic continuous Markov processes : Lyapunov versus 
Poincare&quot;, 
&lt;a href=&quot;http://arxiv.org/abs/math.PR/0703355&quot;&gt;math.PR/0703355&lt;/a&gt; 
	&lt;li&gt;Viviane Baladi, &lt;cite&gt;Positive Transfer Operators and Decay of 
Correlations&lt;/cite&gt; 
	&lt;li&gt;Joseph Berkovitz, Roman Frigg and Fred Kronz, &quot;The Ergodic 
Hierarchy, Randomness and Hamiltonian Chaos&quot;, &lt;a 
href=&quot;http://philsci-archive.pitt.edu/archive/00002927/&quot;&gt;phil-sci/2927&lt;/a&gt; 
	&lt;li&gt;A. A. Borovkov, &lt;cite&gt;Ergodicity and Stability of Stochastic 
Processes&lt;/cite&gt; 
	&lt;li&gt;J.-R. Chazottes and P. Collet, &quot;Almost-sure central limit theorems 
and the Erd&amp;ouml;s-R&amp;eacute;nyi law for expanding maps of the interval&quot;, &lt;a 
href=&quot;http://dx.doi.org/10.1017/S0143385704000550&quot;&gt;&lt;cite&gt;Ergodic Theory and 
Dynamical Systems&lt;/cite&gt; &lt;strong&gt;25&lt;/strong&gt; (2005): 419--41&lt;/a&gt; 
	&lt;li&gt;J.-R. Chazottes, P. Collet and B. Schmitt, &quot;Devroye Inequality for 
a Class of Non-Uniformly Hyperbolic Dynamical Systems&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/math.DS/0412166&quot;&gt;math.DS/0412166&lt;/a&gt; = 
&lt;a 
href=&quot;http://dx.doi.org/10.1088/0951-7715/18/5/023&quot;&gt;&lt;cite&gt;Nonlinearity&lt;/cite&gt; &lt;strong&gt;18&lt;/strong&gt; 
(2005): 2323--2340&lt;/a&gt; 
	&lt;li&gt;J.-R. Chazottes, P. Collet and B. Schmitt, &quot;Statistical 
Consequences of Devroye Inequality for Processes.  Applications to a Class of 
Non-Uniformly Hyperbolic Dynamical Systems&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/math.DS/0412167&quot;&gt;math.DS/0412167&lt;/a&gt; = &lt;a 
href=&quot;http://dx.doi.org/10.1088/0951-7715/18/5/024&quot;&gt;&lt;cite&gt;Nonlinearity&lt;/cite&gt; &lt;strong&gt;18&lt;/strong&gt; 
(2005): 2341--2364&lt;/a&gt; 
	&lt;li&gt;J.-R. Chazottes and G. Gouezel, &quot;On almost-sure versions of 
classical limit theorems for dynamical 
systems&quot;, &lt;a href=&quot;http://arxiv.org/abs/math.DS/0601388&quot;&gt;math.DS/0601388&lt;/a&gt; 
[arguing in support of the idea that &quot;whenever we can prove a limit theorem in 
the classical sense for a dynamical system, we can prove a suitable almost-sure 
version based on an empirical measure with log-average&quot;.] 
	&lt;li&gt;J.-R. Chazottes and F. Redig, &quot;Testing the irreversibility of a 
Gibbsian process via hitting and return 
times&quot;, &lt;a href=&quot;http://arxiv.org/abs/math-ph/0503071&quot;&gt;math-ph/0503071&lt;/a&gt; 
= &lt;a 
href=&quot;http://dx.doi.org/10.1088/0951-7715/18/6/004&quot;&gt;&lt;cite&gt;Nonlinearity&lt;/cite&gt; &lt;strong&gt;18&lt;/strong&gt; 
(2005): 2477--2489&lt;/a&gt; 
	&lt;li&gt;Mu-Fa Chen 
		&lt;ul&gt; 
		&lt;li&gt;&lt;cite&gt;Eigenvalues, Inequalities, and Ergodic 
Theory&lt;/cite&gt; [&lt;a 
href=&quot;http://www.springeronline.com/sgw/cda/frontpage/0,11855,5-0-22-30265375-0,00.html&quot;&gt;Blurb&lt;/a&gt;] 
		&lt;li&gt;&quot;Ergodic convergence rates of Markov 
processes--eigenvalues, inequalities and ergodic 
theory&quot;, &lt;a href=&quot;http://arxiv.org/abs/math.PR/0304367&quot;&gt;math.PR/0304367&lt;/a&gt; 
		&lt;/ul&gt; 
	&lt;li&gt;Xia Chen, &lt;citE&gt;Limit Theorems for Functionals of Ergodic Markov 
Chains with General State Space&lt;/cite&gt; 
	&lt;li&gt;Geon Ho Choe, &lt;cite&gt;Computational Ergodic Theory&lt;/citE&gt; 
	&lt;li&gt;Yves Coudene, &quot;On invariant distributions and 
mixing&quot;, &lt;a href=&quot;http://dx.doi.org/10.1017/S0143385706000733&quot;&gt;&lt;cite&gt;Ergodic 
Theory and Dynamical Systems&lt;/cite&gt; &lt;strong&gt;27&lt;/strong&gt; (2007): 109--112&lt;/a&gt; 
[&quot;any probability preserving transformation of a metric space is mixing as soon 
as there are no non-constant $L^2$-functions which are invariant under both the 
stable and unstable distributions&quot;] 
	&lt;li&gt;Thierry De La Rue, &quot;An introduction to joinings in ergodic theory&quot;, 
&lt;a href=&quot;http://arxiv.org/abs/math.DS/0507429&quot;&gt;math.DS/0507429&lt;/a&gt; 
= &lt;cite&gt;Discrete and Continuous Dynamical Systems&lt;/cite&gt; &lt;strong&gt;15&lt;/strong&gt; 
(2006): 121--142 
	&lt;li&gt;G. B. DiMasi and L. Stettner, &quot;Ergodicity of hidden Markov models&quot;, 
&lt;a href=&quot;http://dx.doi.org/10.1007/s00498-005-0153-8&quot;&gt;&lt;cite&gt;Mathematics of 
Control, Signals, and Systems&lt;/cite&gt; &lt;strong&gt;17&lt;/strong&gt; (2005): 269--296&lt;/a&gt; 
	&lt;li&gt;Ian Domowitz and Mahmoud El-Gamal, &quot;A Consistent Nonparametric Test 
of Ergodicity for Time Series with 
Applications&quot;, &lt;a href=&quot;http://dx.doi.org/10.1016/S0304-4076(01)00058-6&quot;&gt;&lt;cite&gt;Journal 
of Econometrics&lt;/cite&gt; &lt;strong&gt;102&lt;/strong&gt; (2001): 365--398&lt;/a&gt; 
[&lt;a href=&quot;http://papers.ssrn.com/sol3/papers.cfm?abstract_id=179912&quot;&gt;SSRN&lt;/a&gt;. 
Having read about 2/3 of this, I completely fail to see how they actually 
overcome the problem that any one sample path is always confined to a single 
ergodic component.] 
	&lt;li&gt;Martin Dyer, Leslie Ann Goldberg, Mark Jerrum, Russell Martin, 
&quot;Markov chain comparison&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/math.PR/0410331&quot;&gt;math.PR/0410331&lt;/a&gt; [i.e., 
comparison theorems for mixing times] 
	&lt;li&gt;Jean-Pierre Eckmann and Itamar Procaccia, &quot;Invariant Measures in 
Generic Dynamical Systems&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/chao-dyn/9708021&quot;&gt;chao-dyn/9708021&lt;/a&gt; [Abstract: 
&quot;Irreversible thermodynamics of simple fluids have been connected recently to 
the theory of dynamical systems and some interesting assumptions have been made 
about the nature of the associated invariant measures.  We show that the tests 
of the validity of these assumptions are insufficient by exhibiting observables 
that are incorrectly sampled with the proposed invariant measures.  Only 
observables belonging to the 'high temperature phase' of the thermodynamic 
formalism are insensitive to the sampling methods.  We outline methods that are 
free of these deficiencies.&quot;  I read this when it came out, but I don't think 
I understood it then.] 
	&lt;li&gt;Bernhold Fiedler (ed.), &lt;cite&gt;Ergodic Theory, Analysis, and 
Efficient Simulation of Dynamical Systems&lt;/cite&gt; 
	&lt;li&gt;Nikos Frantzikinakis, Randall McCutcheon, &quot;Ergodic Theoy: 
Recurrence&quot;, &lt;a href=&quot;http://arxiv.org/abs/0705.0033&quot;&gt;arxiv:0705.0033&lt;/a&gt; 
	&lt;li&gt;Gary Froyland, &quot;Statistical optimal almost-invariant sets&quot;, 
&lt;a href=&quot;http://dx.doi.org/10.1016/j.physd.2004.11.008&quot;&gt;&lt;cite&gt;Physica 
D&lt;/cite&gt; &lt;strong&gt;200&lt;/strong&gt; (2005): 205--219&lt;/a&gt; [Partitioning state space 
into &lt;em&gt;nearly&lt;/em&gt; separated components.] 
	&lt;li&gt;Stefano Galatolo, Mathieu Hoyrup, Cristobal Rojas, &quot;Dynamics and abstract computability: computing invariant measures&quot;, &lt;a href=&quot;http://arxiv.org/abs/0903.2385&quot;&gt;arxiv:0903.2385&lt;/a&gt; 
	&lt;li&gt;Gan Shixin, &quot;Almost sure convergence 
for  
&lt;img align=absmiddle src=&quot;ergodic-theory_15.gif&quot; alt=&quot;$ \tilde{\rho} $ &quot;&gt;
-mixing random variable sequences&quot;, &lt;citE&gt;Statistics 
and Probability Letters&lt;/cite&gt; 
&lt;strong&gt;67&lt;/strong&gt; (2004): 289--298 
	&lt;li&gt;E. Glasner and B. Weiss, &quot;On the interplay between measurable and 
topological dynamics&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/math.DS/0408328&quot;&gt;math.DS/0408328&lt;/a&gt; 
	&lt;li&gt;Beniamin Goldys and Bohdan Maslowski, &quot;Uniform exponential 
ergodicity of stochastic dissipative systems,&quot; &lt;a 
href=&quot;http://arxiv.org/abs/math.PR/0111143&quot;&gt;math.PR/0111143&lt;/a&gt; 
	&lt;li&gt;M. Hairer, &quot;Ergodic properties of a class of non-Markovian 
processes&quot;, &lt;a href=&quot;http://arxiv.org/abs/0708.3338&quot;&gt;arxiv:0708.3338&lt;/a&gt; 
	&lt;li&gt;P. Halmos, &lt;cite&gt;Ergodic Theory&lt;/cite&gt; 
	&lt;li&gt;Nicolai T. A. Haydn, &quot;The Central Limit Theorem for uniformly strong mixing measures&quot;, &lt;a href=&quot;http://arxiv.org/abs/0903.1325&quot;&gt;arxiv:0903.1325&lt;/a&gt; 
	&lt;li&gt;Nicolai Haydn, Y. Lacroix and Sandro Vaienti, &quot;Hitting and return 
times in ergodic dynamical 
systems&quot;, &lt;a href=&quot;http://arxiv.org/abs/math.DS/0410384&quot;&gt;math.DS/0410384&lt;/a&gt; 
= &lt;a href=&quot;http://dx.doi.org/10.1214/009117905000000242&quot;&gt;&lt;cite&gt;Annals of 
Probability&lt;/cite&gt; &lt;strong&gt;33&lt;/strong&gt; (2005): 2043--2050&lt;/a&gt; 
	&lt;li&gt;Nicolai Haydn and Sandro Vaienti, &quot;Fluctuations of the Metric 
Entropy for Mixing Measures&quot;, &lt;a 
href=&quot;http://dx.doi.org/10.1142/S021949370400119X&quot;&gt;&lt;cite&gt;Stochastics and 
Dynamics&lt;/cite&gt; &lt;strong&gt;4&lt;/strong&gt; (2004): 595--627&lt;/a&gt; 
	&lt;li&gt;Bernard Host, &quot;Convergence of multiple ergodic averages&quot;, 
&lt;a href=&quot;http://arxiv.org/abs/math.DS/0606362&quot;&gt;math.DS/0606362&lt;/a&gt; [&quot;We study 
the mean convergence of multiple ergodic averages, that is, averages of a 
product of functions taken at different times.&quot;] 
	&lt;li&gt;Gerhard Keller, &lt;cite&gt;Equilibrium States in Ergodic Theory&lt;/cite&gt; 
	&lt;li&gt;Gerhard Keller and Carlangelo Liverani, &quot;Uniqueness of the SRB 
Measure for Piecewise Expanding Weakly Coupled Map Lattices in Any Dimension&quot;, 
&lt;a href=&quot;http://dx.doi.org/10.1007/s00220-005-1474-7&quot;&gt;&lt;cite&gt;Communications in 
Mathematical Physics&lt;/cite&gt; &lt;strong&gt;262&lt;/strong&gt; (2006): 33--50&lt;/a&gt; 
	&lt;li&gt;U. Kregnel, &lt;cite&gt;Ergodic Theorems&lt;/cite&gt; 
	&lt;li&gt;Anna Kuczmaszewska, &quot;The strong law of large numbers for dependent 
random variables&quot;, &lt;a 
href=&quot;http://dx.doi.org/10.1016/j.spl.2005.04.005&quot;&gt;&lt;cite&gt;Statistics and 
Probability Letters&lt;/citE&gt; &lt;strong&gt;73&lt;/strong&gt; (2005): 305--314&lt;/a&gt; 
	&lt;li&gt;B. K&amp;uuml;mmerer and H. Maassen, &quot;A pathwise ergodic theorem for 
quantum trajectories&quot;, &lt;cite&gt;Journal of Physics A&lt;/cite&gt; &lt;strong&gt;37&lt;/strong&gt; 
(2004): 11889--11896 [&lt;a 
href=&quot;http://www.iop.org/EJ/abstract/-alert=14764/0305-4470/37/49/008&quot;&gt;journal 
link&lt;/a&gt;] 
	&lt;li&gt;Lin Zhengyan and Lu Chuanrong, &lt;cite&gt;Limit Theory for Mixing 
Dependent Random Variables&lt;/cite&gt; 
	&lt;li&gt;Pei-Dong Liu and Min Qian, &lt;cite&gt;Smooth Ergodic Theory of Random 
Dynamical Systems&lt;/cite&gt; 
	&lt;li&gt;Dasha Loukianova, Oleg Loukianov, Eva Loecherbach, &quot;Polynomial 
bounds in the Ergodic Theorem for positive recurrent one-dimensional diffusions 
and integrability of hitting 
times&quot;, &lt;a href=&quot;http://arxiv.org/abs/0903.2405&quot;&gt;arxiv:0903.2405&lt;/a&gt; 
[&lt;em&gt;non-asymptotic&lt;/em&gt; deviation bounds from bounds on moments of 
recurrence times] 
	&lt;li&gt;Stefano Luzzatto 
		&lt;ul&gt; 
		&lt;li&gt;&quot;Mixing and decay of correlations in 
non-uniformly expanding maps: a survey of recent results,&quot; 
&lt;a href=&quot;http://arxiv.org/abs/math.DS/0301319&quot;&gt;math.DS/0301319&lt;/a&gt; 
		&lt;li&gt;&quot;Stochastic-like behaviour in nonuniformly expanding maps&quot;, 
&lt;a href=&quot;http://arxiv.org/abs/math.DS/0409085&quot;&gt;math.DS/0409085&lt;/a&gt; 
		&lt;/ul&gt; 
	&lt;li&gt;Stefano Luzzatto, Ian Melbourne and Frederic Paccaut, &quot;The Lorenz 
Attractor is Mixing&quot;, &lt;a 
href=&quot;http://dx.doi.org/10.1007/s00220-005-1411-9&quot;&gt;&lt;cite&gt;Communications in 
Mathematical Physics&lt;/cite&gt; &lt;strong&gt;260&lt;/strong&gt; (2005): 393--401&lt;/a&gt; 
	&lt;li&gt;Vincent Lynch, &quot;Decay of correlations for non-Holder 
observables&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/math.DS/0401432&quot;&gt;math.DS/0401432&lt;/a&gt; 
	&lt;li&gt;Michael C. Mackey and Marta Tyran-Kaminska 
		&lt;ul&gt; 
		&lt;li&gt;&quot;Deterministic Brownian Motion: The Effects of Perturbing a 
Dynamical System by a Chaotic Semi-Dynamical 
System&quot;, &lt;a href=&quot;http://arxiv.org/abs/cond-mat/0408330&quot;&gt;cond-mat/0408330&lt;/a&gt; 
		&lt;li&gt;&quot;Effects of Noise on Entropy Evolution&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/cond-mat/0501092&quot;&gt;cond-mat/0501092&lt;/a&gt; 
		&lt;li&gt;&quot;Central Limit Theorems 
for Non-Invertible Measure Preserving 
Maps&quot;, &lt;a href=&quot;http://arxiv.org/abs/math.PR/0608637&quot;&gt;math.PR/0608637&lt;/a&gt; [&quot;a 
new functional central limit theorem result for non-invertible measure 
preserving maps that are not necessarily ergodic, using the Perron-Frobenius 
operator&quot;] 
		&lt;/ul&gt; 
	&lt;li&gt;C. Maes, F. Redig and E. Saada, &quot;The Infinite Volume Limit of 
Dissipative Abelian Sandpiles&quot;, &lt;citE&gt;Communications in Mathematical 
Physics&lt;/cite&gt; &lt;strong&gt;244&lt;/strong&gt; (2004): 395--417 
	&lt;li&gt;Katalin Marton and Paul C. Shields, &quot;How many future measures can 
there be?&quot;, &lt;a href=&quot;http://dx.doi.org/10.1017/S0143385702000123&quot;&gt;&lt;citE&gt;Ergodic 
Theory and Dynamical Systems&lt;/cite&gt; &lt;strong&gt;22&lt;/strong&gt; (2002): 257--280&lt;/a&gt; 
	&lt;li&gt;Jonathan C. Mattingly, &quot;On Recent Progress for the Stochastic 
Navier Stokes Equations&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/math.PR/0409194&quot;&gt;math.PR/0409194&lt;/a&gt; [&quot;We give an 
overview of the ideas central to some recent developments in the ergodic theory 
of the stochastically forced Navier Stokes equations and other dissipative 
stochastic partial differential equations.&quot;] 
	&lt;li&gt;Ian Melbourne and Matthew Nicol 
		&lt;ul&gt; 
		&lt;li&gt;&quot;Almost Sure Invariance Principle for Nonuniformly 
Hyperbolic Systems&quot;, &lt;a 
href=&quot;http://dx.doi.org/0.1007/s00220-005-1407-5&quot;&gt;&lt;cite&gt;Communications in 
Mathematical Physics&lt;/cite&gt; &lt;strong&gt;260&lt;/strong&gt; (2005): 131--146&lt;/a&gt; 
= &lt;a href=&quot;http://arxiv.org/abs/math.DS/0503693&quot;&gt;math.DS/0503693&lt;/a&gt; [&quot;We prove 
an almost sure invariance principle that is valid for general classes of 
nonuniformly expanding and nonuniformly hyperbolic dynamical systems. Discrete 
time systems and flows are covered by this result. ... Statistical limit laws 
such as the central limit theorem, the law of the iterated logarithm, and their 
functional versions, are immediate consequences.&quot;] 
		&lt;li&gt;&quot;A Vector-Valued Almost Sure Invariance Principle for 
Hyperbolic Dynamical 
Systems&quot;, &lt;a href=&quot;http://arxiv.org/abs/math.DS/0606535&quot;&gt;math.DS/0606535&lt;/a&gt; 
		&lt;/ul&gt; 
	&lt;li&gt;Mehryar Mohri, Afshin Rostamizadeh, &quot;Stability Bound for Stationary 
Phi-mixing and Beta-mixing 
Processes&quot;, &lt;a href=&quot;http://arxiv.org/abs/0811.1629&quot;&gt;arxiv:0811.1629&lt;/a&gt; 
	&lt;li&gt;D. S. Ornstein and B. Weiss, &quot;Statistical Properties of Chaotic Systems,&quot; &lt;cite&gt;Bulletin 
of the American Mathematical Society&lt;/cite&gt; &lt;strong&gt;24&lt;/strong&gt; (1991): 11--116 
	&lt;li&gt;Goran Peskir, &lt;cite&gt;From Uniform Laws of Large Numbers to 
Uniform Ergodic Theorems&lt;/cite&gt; 
	&lt;li&gt;Karl E. Petersen, &lt;cite&gt;Ergodic Theory&lt;/cite&gt; 
	&lt;li&gt;Mark Pollicott, &lt;cite&gt;Lectures on Ergodic Theory and Pesin Theory 
on Compact Manifolds&lt;/cite&gt; 
	&lt;li&gt;Mark Pollicott and Michiko Yuri, &lt;cite&gt;Dynamical Systems and 
Ergodic Theory&lt;/cite&gt; [PDF files for the individual chapters are available &lt;a 
href=&quot;http://www.ma.man.ac.uk/~mp/book.html&quot;&gt;here&lt;/a&gt;, but many of them don't 
display properly, at least on my laptop...] 
	&lt;li&gt;Charles Pugh and Michael Shub, with an appendix by Alexander 
Starkov, &quot;Stable Ergodicity&quot;, &lt;cite&gt;Bulletin of the American Mathematical 
Society&lt;/cite&gt; (new series) &lt;strong&gt;41&lt;/strong&gt; (2003): 1--41&lt;/a&gt; 
[&lt;a 
href=&quot;http://www.ams.org/bull/2004-41-01/S0273-0979-03-00998-4/S0273-0979-03-00998-4.pdf&quot;&gt;Link&lt;/a&gt;] 
	&lt;li&gt;Maxim Raginsky, &quot;Joint universal lossy coding and identification of stationary mixing sources with general alphabets&quot;, &lt;a href=&quot;http://arxiv.org/abs/0901.1904&quot;&gt;arxiv:0901.1904&lt;/a&gt; 
	&lt;li&gt;Gennady Samorodnitsky, &quot;Extreme value theory, ergodic theory and 
the boundary between short memory and long memory for stationary stable 
processes&quot;, &lt;cite&gt;Annals of Probability&lt;/cite&gt; &lt;strong&gt;32&lt;/strong&gt; (2004): 
1438--1468 = &lt;a href=&quot;http://arxiv.org/abs/math.PR/0410149&quot;&gt;math.PR/0410149&lt;/a&gt; 
	&lt;li&gt;C. E. Silva, &lt;cite&gt;Invitation to Ergodic Theory&lt;/cite&gt; 
[&lt;a href=&quot;http://www.oup.com/uk/catalogue/?ci=9780821844205&quot;&gt;blurb&lt;/a&gt;] 
	&lt;li&gt;Ya. Sinai, &lt;cite&gt;Topics in Ergodic Theory&lt;/cite&gt; 
	&lt;li&gt;Rob Sturman, Julio M. Ottino, and Stephen Wiggins, &lt;cite&gt;The 
Mathematical Foundations of Mixing: The Linked Twist Map as a Paradigm in 
Applications: Micro to Macro, Fluids to Solids&lt;/cite&gt; 
[&lt;a href=&quot;http://cambridge.org/0521868130&quot;&gt;Blurb&lt;/a&gt;] 
	&lt;li&gt;Andre Toom 
		&lt;ul&gt; 
		&lt;li&gt;&quot;Law of Large Numbers for Non-Local 
Functions of Probabilistic Cellular Automata&quot;, &lt;a href=&quot;http://dx.doi.org/10.1007/s10955-008-9643-7&quot;&gt;&lt;cite&gt;Journal of Statistical Physics&lt;/cite&gt; &lt;strong&gt;133&lt;/strong&gt; (2008): 883--897&lt;/a&gt; 
		&lt;li&gt;&quot;Every Continuous Operator Has an Invariant 
Measure&quot;, &lt;a href=&quot;http://dx.doi.org/10.1007/s10955-007-9407-9&quot;&gt;&lt;cite&gt;Journal of Statistical 
Physics&lt;/cite&gt; &lt;strong&gt;129&lt;/strong&gt; (2007): 555--566&lt;/a&gt; 
		&lt;/ul&gt; 
	&lt;li&gt;A. Vershik, &quot;Towards the definition of metric hyperbolicity&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/math.DS/0508514&quot;&gt;math.DS/0508514&lt;/a&gt; 
	&lt;li&gt;Peter Walters, &lt;cite&gt;An Introduction to Ergodic Theory&lt;/cite&gt; 
	&lt;li&gt;Wei Wang, Jianhua Sun and Jinqiao Duan, &quot;Ergodic Dynamics of 
the Stochastic Swift-Hohenberg System&quot;, 
&lt;a href=&quot;http://arxiv.org/abs/math.DS/0408322&quot;&gt;math.DS/0408322&lt;/a&gt; 
	&lt;li&gt;&lt;a href=&quot;http://galton.uchicago.edu/faculty/wu.html&quot;&gt;Wei Biao 
Wu&lt;/a&gt;, Xiaofeng Shao, &quot;Invariance principles for fractionally integrated 
nonlinear 
processes&quot;, &lt;a href=&quot;http://arxiv.org/abs/math.PR/0608223&quot;&gt;math.PR/0608223&lt;/a&gt; 
	&lt;li&gt;&lt;a href=&quot;http://galton.uchicago.edu/faculty/wu.html&quot;&gt;Wei Biao 
Wu&lt;/a&gt; and Michael Woodroofe, &quot;Martingale Approximations for Sums of Stationary 
Processes&quot;, &lt;cite&gt;Annals of Probability&lt;/cite&gt; &lt;strong&gt;32&lt;/strong&gt; (2004): 
1674--1690 = &lt;a href=&quot;http://arxiv.org/abs/math.PR/0410160&quot;&gt;math.PR/0410160&lt;/a&gt; 
	&lt;li&gt;Ivan Werner, &quot;Ergodic theorem for contractive Markov systems&quot;, 
&lt;a 
href=&quot;http://dx.doi.org/10.1088/0951-7715/17/6/016&quot;&gt;&lt;cite&gt;Nonlinearity&lt;/cite&gt; 
&lt;strong&gt;17&lt;/strong&gt; (2303--2313)&lt;/a&gt; [&lt;a 
href=&quot;http://www.mcs.st-and.ac.uk/~iw11/cmsERGODn2.ps&quot;&gt;PS&lt;/a&gt; preprint] 
	&lt;li&gt;Guangyu Yang, Yu Miao, &quot;An invariance principle for the law of the 
iterated logarithm for additive functionals of Markov 
chains&quot;, &lt;a href=&quot;http://arxiv.org/abs/math.PR/0609593&quot;&gt;math.PR/0609593&lt;/a&gt; 
	&lt;li&gt;Radu Zaharopol, &lt;cite&gt;Invariant Probabilities of Markov-Feller 
Operators and Their Supports&lt;/cite&gt; 
	&lt;li&gt;Steve Zelditch, &quot;Quantum ergodicity and mixing&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/quant-ph/0503026&quot;&gt;quant-ph/0503026&lt;/a&gt; [&quot;an 
expository article for the Encyclopedia of Mathematical Physics&quot;] 
	&lt;li&gt;L. Zsido, &quot;Weaking mixing properties of vector sequences&quot;, &lt;a 
href=&quot;http://arxiv.org/abs/math.FA/0506554&quot;&gt;math.FA/0506554&lt;/a&gt; 
	&lt;/ul&gt; 

&lt;P&gt;Updated 29 October 2007; thanks to &quot;tushar&quot; for pointing out an embarrassing 
think-o in the first paragraph. 

&lt;P&gt;Previous versions: &lt;em&gt;15 Nov 2005 16:18&lt;/em&gt;; first version written c. 1997 (?) 
</description>
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