Stein's method, Malliavin calculus and infinite-dimensional Gaussian
Stein's method, Malliavin calculus and infinite-dimensional Gaussian
Stein's method, Malliavin calculus and infinite-dimensional Gaussian
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Proposition 6.1 1. For every q 1, the qth Wiener chaos C q (X) is a Hilbert subspace of<br />
L 2 (P), <strong>and</strong> the application<br />
h 7! I q (h) , h 2 H q ,<br />
de…nes a Hilbert space isomorphism between H q , endowed with the scalar product q! h; i H q,<br />
<strong>and</strong> C q (X).<br />
2. For every q; q 0 0 such that q 6= q 0 , the spaces C q (X) <strong>and</strong> C q 0 (X) are orthogonal in<br />
L 2 (P) :<br />
3. Let F be a functional of the isonormal <strong>Gaussian</strong> process X satisfying E[F (X) 2 ] < 1:<br />
then, there exists a unique sequence ff q : q 1g such that f q 2 H q , <strong>and</strong><br />
F = E (F ) +<br />
1X<br />
I q (f q ) =<br />
q=1<br />
1X<br />
I q (f q ) , (6.6)<br />
q=0<br />
where we have used the notation I 0 (f 0 ) = E (F ), <strong>and</strong> the series converges in L 2 (P).<br />
4. Suppose that H = L 2 (Z; Z; ), where is -…nite <strong>and</strong> non-atomic. Then, for q 2,<br />
the symmetric power H q can be identi…ed with L 2 s (Z q ; Z q ; q ) <strong>and</strong>, for every f 2 H q ,<br />
the r<strong>and</strong>om variable I q (f) coincides with the Wiener-Itô integral of f with respect to the<br />
<strong>Gaussian</strong> measure given by A 7! X (1 A ), A 2 Z .<br />
Remark. The combination of Point 1 <strong>and</strong> Point 2 in the statement of Proposition 6.1<br />
implies that, for every q; q 0 1,<br />
E I q (f) I q 0 f 0 = 1 q=q 0q! f; f 0 H q :<br />
From the previous statement, one also deduces the following Hilbert space isomorphism:<br />
L 2 ( (X)) '<br />
1M<br />
H q , (6.7)<br />
q=0<br />
where ' st<strong>and</strong>s for a Hilbert space isomorphism, <strong>and</strong> each symmetric power H q is endowed<br />
with the modi…ed scalar product q! h; i H q. The direct sum on the RHS of (6.7) is called the<br />
symmetric Fock space associated with H.<br />
6.3 Contractions <strong>and</strong> products<br />
We start by introducing the notion of contraction in the context of powers of Hilbert spaces.<br />
De…nition 6.3 Consider a real separable Hilbert space H, <strong>and</strong> let fe i : i 1g be an orthonormal<br />
basis of H. For every n; m 1, every r = 0; :::; n ^ m <strong>and</strong> every f 2 H n <strong>and</strong> g 2 H m , we<br />
de…ne the contraction of order r, of f <strong>and</strong> g, as the element of H n+m 2r given by<br />
f r g =<br />
1X<br />
i 1 ;:::;i r=1<br />
<strong>and</strong> we denote by f e r g its symmetrization.<br />
hf; e i1 e ir i H r hg; e i1 e ir i H r ; (6.8)<br />
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