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Jean-François Le Gall - Brownian Motion, Martingales, and Stochastic Calculus

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Jean-François Le Gall Brownian Motion, Martingales, and Stochastic Calculus
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Springer International Publishing Switzerland 2016
Jean-Franois Le Gall Brownian Motion, Martingales, and Stochastic Calculus Graduate Texts in Mathematics 10.1007/978-3-319-31089-3_1
1. Gaussian Variables and Gaussian Processes
Jean-Franois Le Gall 1
(1)
Dpartement de Mathmatiques, Universit Paris-Sud, Orsay Cedex, France
Gaussian random processes play an important role both in theoretical probability and in various applied models. We start by recalling basic facts about Gaussian random variables and Gaussian vectors. We then discuss Gaussian spaces and Gaussian processes, and we establish the fundamental properties concerning independence and conditioning in the Gaussian setting. We finally introduce the notion of a Gaussian white noise, which will be used to give a simple construction of Brownian motion in the next chapter.
1.1 Gaussian Random Variables
Throughout this chapter, we deal with random variables defined on a probability space Brownian Motion Martingales and Stochastic Calculus - image 1 . For some of the existence statements that follow, this probability space should be chosen in an appropriate way. For every real p 1, Brownian Motion Martingales and Stochastic Calculus - image 2 , or simply L p if there is no ambiguity, denotes the space of all real random variables X such that| X | p is integrable, with the usual convention that two random variables that are a.s. equal are identified. The space L p is equipped with the usual norm.
A real random variable X is said to be a standard Gaussian (or normal ) variable if its law has density
with respect to Lebesgue measure on The complex Laplace transform of X is - photo 3
with respect to Lebesgue measure on The complex Laplace transform of X is then given by To get this formula and - photo 4 . The complex Laplace transform of X is then given by
To get this formula and also to verify that the complex Laplace transform is - photo 5
To get this formula (and also to verify that the complex Laplace transform is well defined), consider first the case when This calculation ensures that E e zX is well-defined for every and - photo 6 :
This calculation ensures that E e zX is well-defined for every and - photo 7
This calculation ensures that E [e zX ] is well-defined for every Brownian Motion Martingales and Stochastic Calculus - image 8 , and defines a holomorphic function on Brownian Motion Martingales and Stochastic Calculus - image 9 . By analytic continuation, the identity Brownian Motion Martingales and Stochastic Calculus - image 10 , which is true for every Picture 11 , must also be true for every Picture 12 .
By taking Brownian Motion Martingales and Stochastic Calculus - image 13 , Brownian Motion Martingales and Stochastic Calculus - image 14 , we get the characteristic function of X :
Brownian Motion Martingales and Stochastic Calculus - image 15
From the expansion
as this expansion holds for every n 1 when X belongs to all spaces L p - photo 16
as Brownian Motion Martingales and Stochastic Calculus - image 17 (this expansion holds for every n 1 when X belongs to all spaces L p , Brownian Motion Martingales and Stochastic Calculus - image 18 , which is the case here), we get
Brownian Motion Martingales and Stochastic Calculus - image 19
and more generally, for every integer n 0,
If and we say that a real random variable Y is Gaussian with - photo 20
If Picture 21 and Picture 22 , we say that a real random variable Y is Gaussian with Brownian Motion Martingales and Stochastic Calculus - image 23 -distribution if Y satisfies any of the three equivalent properties:
(i)
Brownian Motion Martingales and Stochastic Calculus - image 24 , where X is a standard Gaussian variable (i.e. X follows the -distribution ii the law of Y has density iii the characteristic - photo 25 -distribution);
(ii)
the law of Y has density
iii the characteristic function of Y is We have then B - photo 26
(iii)
the characteristic function of Y is
We have then By extension we say that Y is Gaussian with -distribution if Y - photo 27
We have then
By extension we say that Y is Gaussian with -distribution if Y m as - photo 28
By extension, we say that Y is Gaussian with Picture 29 -distribution if Y = m a.s. (property (iii) still holds in that case).
Sums of independent Gaussian variables
Suppose that Y follows the Brownian Motion Martingales and Stochastic Calculus - image 30 -distribution, Y follows the Brownian Motion Martingales and Stochastic Calculus - image 31 -distribution, and Y and Y are independent. Then Y + Y follows the Brownian Motion Martingales and Stochastic Calculus - image 32 -distribution. This is an immediate consequence of (iii).
Proposition 1.1
Let (X n ) n1 be a sequence of real random variables such that, for every n 1, X n follows the Picture 33
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