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Daniel W. Stroock - An Introduction to Markov Processes

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Daniel W. Stroock An Introduction to Markov Processes
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Finite state space, a trial run -- Moving to Euclidean space, the real thing -- Itos approach in the Euclidean setting -- Further considerations -- Itos theory of stochastic integration -- Applications of stochastic integration to Brownian motion -- The Kunita-Watanabe extension -- Stratonovishs theory.;Kiyosi Its greatest contribution to probability theory may be his introduction of stochastic differential equations to explain the Kolmogorov-Feller theory of Markov processes. Starting with the geometric ideas that guided him, this book gives an account of Its program. The modern theory of Markov processes was initiated by A.N. Kolmogorov. However, Kolmogorovs approach was too analytic to reveal the probabilistic foundations on which it rests. In particular, it hides the central role played by the simplest Markov processes: those with independent, identically distributed increments. To remedy this defect, It interpreted Kolmogorovs famous forward equation as an equation that describes the integral curve of a vector field on the space of probability measures. Thus, in order to show how Its thinking leads to his theory of stochastic integral equations, Stroock begins with an account of integral curves on the space of probability measures and then arrives at stochastic integral equations when he moves to a pathspace setting. In the first half of the book, everything is done in the context of general independent increment processes and without explicit use of Its stochastic integral calculus. In the second half, the author provides a systematic development of Its theory of stochastic integration: first for Brownian motion and then for continuous martingales. The final chapter presents Stratonovichs variation on Its theme and ends with an application to the characterization of the paths on which a diffusion is supported. The book should be accessible to readers who have mastered the essentials of modern probability theory and should provide such readers with a reasonably thorough introduction to continuous-time, stochastic processes.

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Daniel W. Stroock Graduate Texts in Mathematics An Introduction to Markov Processes 2nd ed. 2014 10.1007/978-3-642-40523-5_1
Springer-Verlag Berlin Heidelberg 2014
1. Random Walks, a Good Place to Begin
Daniel W. Stroock 1
(1)
Department of Mathematics, Massachusetts Institute of Technology, Cambridge, MA, USA
Abstract
In order to introduce as soon as possible some of the ideas that underlie the whole book, Chap. 1 provides an introduction of Bernoulli random walks in one and higher dimensions. Emphasis is placed on the calculation of passage times and the dependence of recurrence properties on dimension.
The purpose of this chapter is to discuss some examples of Markov processes that can be understood even before the term Markov process is. Indeed, anyone who has been introduced to probability theory will recognize that these processes all derive from consideration of elementary coin tossing.
1.1 Nearest Neighbor Random Walks on Picture 1
Let p be a fixed number from the open interval (0,1), and suppose that which are 1 with probability p . That is, for any and any E 1 n 11 n 111 Next set 112 The abov - photo 2 and any E ( 1,, n ){1,1} n ,
An Introduction to Markov Processes - image 3
(1.1.1)
Next, set
An Introduction to Markov Processes - image 4
(1.1.2)
The above family of random variables An Introduction to Markov Processes - image 5 is often called a nearest neighbor random walk on Picture 6 . Nearest neighbor random walks are examples of Markov processes, but the description that I have just given is the one which would be given in elementary probability theory, as opposed to a course, like this one, devoted to stochastic processes. When studying stochastic processes the description should emphasize the dynamic nature of the family. Thus, a stochastic process oriented description might replace () by
113 where denotes the conditional probability cf Sect Specifically - photo 7
(1.1.3)
where denotes the conditional probability cf Sect Specifically it says that - photo 8 denotes the conditional probability (cf. Sect. ). Specifically, it says that the process starts from 0 at time n =0 and proceeds so that, at each time Picture 9 , it moves one step forward with probability p or one step backward with probability q , independent of where it has been before time n .
1.1.1 Distribution at Time n
In this subsection I will present two approaches to computing An Introduction to Markov Processes - image 10 . The first computation is based on the description given in () it is clear that An Introduction to Markov Processes - image 11 . In addition, it is obvious that
An Introduction to Markov Processes - image 12
Finally, given m { n ,, n } with the same parity as n and a string E =( 1,, n ){1,1} n with (cf. ()) S n ( E )= m , An Introduction to Markov Processes - image 13 and so
An Introduction to Markov Processes - image 14
Hence, because, when An Introduction to Markov Processes - image 15 is the binomial coefficient choose k , there are such strings E we see that 114 Our second computation of the same - photo 16 such strings E , we see that
An Introduction to Markov Processes - image 17
(1.1.4)
Our second computation of the same probability will be based on the more dynamic description given in (), we see that An Introduction to Markov Processes - image 18 equals
That is 115 Obviously plus induction on n to see that P n m 0 - photo 19
That is,
115 Obviously plus induction on n to see that P n m 0 unless m 2 - photo 20
(1.1.5)
Obviously, () plus induction on n to see that ( P n ) m =0 unless m =2 n for some 0 n and that ( C n )0=( C n ) n =1 and ( C n ) =( C n 1) 1+( C n 1) for 1< n where ( C n ) p q n ( P n )2 n . In other words, the family are given by Pascals triangle and are therefore the binomial coefficients - photo 21 are given by Pascals triangle and are therefore the binomial coefficients.
1.1.2 Passage Times via the Reflection Principle
More challenging than the computation in Sect.
An Introduction to Markov Processes - image 22
(1.1.6)
Then { a } is the first passage time to a , and our goal here is to find its distribution. Equivalently, we want an expression for An Introduction to Markov Processes - image 23 , and clearly, by the considerations in Sect. , we need only worry about n s which satisfy n | a | and have the same parity as a .
Again I will present two approaches to this problem, here based on (), assume that suppose that has the same parity as a and observe first that Hence it - photo 24 , suppose that has the same parity as a and observe first that Hence it suffices for us to - photo 25 has the same parity as a , and observe first that
Hence it suffices for us to compute For this purpose note that for any E - photo 26
Hence, it suffices for us to compute An Introduction to Markov Processes - image 27 . For this purpose, note that for any E {1,1} n 1 with S n 1( E )= a 1, the event {( B 1,, B n 1)= E } has probability An Introduction to Markov Processes - image 28
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