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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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To prove the Wasserstein estimate (9.9), it is su¢ cient to observe that, for every globally Lipschitz<br />

function g such that kgk L 1, there exists a family fg " : " > 0g such that:<br />

(i) for each " > 0, the …rst <strong>and</strong> second derivatives of g " are bounded;<br />

(ii) for each " > 0, one has that kg " k Lip kgk L ;<br />

(iii) as " ! 0, kg " gk 1 # 0.<br />

For instance, we can choose g " (x) = E g(x + p "S) with S N d (0; I d ).<br />

Theorem 9.2 will be fully exploited in Section 10.2, where we will obtain bounds on the<br />

normal approximation of r<strong>and</strong>om vectors woth coordinates living in a …xed Wiener chaos.<br />

9.3 Gamma approximation<br />

We now state a result that can be obtained by combining <strong>Malliavin</strong> <strong>calculus</strong> with the Gamma<br />

approximations discussed in the second part of Section 8.2 (we shall use the same notation<br />

introduced therein). The proof (left to the reader) makes use of (7.34), <strong>and</strong> of arguments<br />

analogous to those displayed in the proof of Theorem 9.1.<br />

Theorem 9.3 Fix > 0 <strong>and</strong> let F () have a centered Gamma distribution with parameter .<br />

Let G 2 D 1;2 be such that E(G) = 0 <strong>and</strong> the law of G is absolutely continuous with respect to<br />

the Lebesgue measure. Then:<br />

d G1 (G; F ()) K 1 E[(2 + 2G hDG; DL 1 Gi H ) 2 ] 1=2 ; (9.11)<br />

<strong>and</strong>, if 1 is an integer,<br />

d G2 (G; F ()) K 2 E[(2 + 2G hDG; DL 1 Gi H ) 2 ] 1=2 ; (9.12)<br />

where G 1 <strong>and</strong> G 2 are de…ned in (8.11)–(8.12), K 1 , maxf1; 1= + 2= 2 g <strong>and</strong> K 2 , maxf p 2=;<br />

1= + 2= 2 g.<br />

We will come back to Theorem 9.3 in Section 10.3, where we will present some characterizations<br />

of non-central limit theorems on a …xed Wiener chaos.<br />

10 Limit Theorems on Wiener chaos<br />

Let X = fX (h) : h 2 Hg be an isonormal <strong>Gaussian</strong> process. In this section, we focus on the<br />

<strong>Gaussian</strong> <strong>and</strong> Gamma approximations of (vectors of) r<strong>and</strong>om variables of the type F = I q (f),<br />

where q 2 <strong>and</strong> f 2 H q . We recall that, according to the chaotic representation property<br />

stated in Proposition 6.1-3, r<strong>and</strong>om variables of this form are the basic building blocks of every<br />

square-integrable functional of X.<br />

In order to appreciate the subtelty of the issues faced in this section, we list some well-known<br />

properties of the laws of chaotic r<strong>and</strong>om variables.<br />

47

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