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Stein's method, Malliavin calculus and infinite-dimensional Gaussian

Stein's method, Malliavin calculus and infinite-dimensional Gaussian

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denote by F t the …ltration generated by W <strong>and</strong> by the P-null sets of (G), <strong>and</strong> we say that<br />

a stochastic process u (t; !) is adapted, if u (t) 2 F t for every t 2 [0; 1]. If u is adapted <strong>and</strong><br />

R <br />

1<br />

E<br />

0 u (t)2 dt < 1, then the Itô stochastic integral R 1<br />

0 u (t) dW t is a well-de…ned element of<br />

L 2 ( (X)). Moreover, in this case one has that<br />

(u) =<br />

Z 1<br />

0<br />

u (t) dW t<br />

(see [65, Proposition 1.3.11]).<br />

7.2.3 A formula on products<br />

We conclude with a general (useful) formula involving products of <strong>Malliavin</strong> di¤erentiable r<strong>and</strong>om<br />

variables <strong>and</strong> elements of dom (). The framework is that of a general isonormal process<br />

X = fX (h) : h 2 Hg.<br />

Proposition 7.5 Let F 2 D 1;2 <strong>and</strong> u 2 dom () be such that: (i) F u 2 L 2 ( (X) ; H), (ii)<br />

F (u) 2 L 2 ( (X)), <strong>and</strong> (iii) hDF; ui H<br />

2 L 2 ( (X)). Then, F u 2 dom (), <strong>and</strong> also<br />

(F u) = F (u) hDF; ui H<br />

: (7.20)<br />

Proof. Consider a r<strong>and</strong>om variable G equal to the RHS (7.2), with f 2 C0<br />

1<br />

E <br />

hDG; F ui H<br />

= E <br />

hF DG; ui H = E hD (F G) GDF; uiH<br />

= E <br />

F (u) hDF; ui H G .<br />

(Rm ). Then,<br />

Since r<strong>and</strong>om variables such as G generate (X), the conclusion is obtained.<br />

7.3 The Ornstein-Uhlenbeck Semigroup <strong>and</strong> Mehler’s formula<br />

7.3.1 De…nition, Mehler’s formula <strong>and</strong> vector-valued Markov processes<br />

Let X = fX (h) : h 2 Hg be an isonormal <strong>Gaussian</strong> process over some real separable Hilbert<br />

space H.<br />

De…nition 7.4 The Ornstein-Uhlenbeck semigroup fT t : t 0g is the set of contraction<br />

operators de…ned as<br />

T t (F ) = E (F ) +<br />

1X<br />

e qt I q (f q ) =<br />

q=1<br />

1X<br />

e qt I q (f q ) ; (7.21)<br />

q=0<br />

for every t 0 <strong>and</strong> every F 2 L 2 ( (X)) as in (6.6):<br />

The Ornstein-Uhlenbeck semigroup plays a fundamental role in our theory. Its relevance for<br />

Stein’s <strong>method</strong> is not new: see for instance the so-called “Barbour-Götze generator approach”,<br />

introduced in [2] <strong>and</strong> [29] (see [80] for a survey). As another example, see [57], [62] <strong>and</strong> the<br />

discussion contained in Section 9, where it is shown that the use of the semigroup fT t g leads<br />

31

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