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Lemma

Proposition

Probability Theory · probability.tex
Stein's Equation All solutions of Stein's Equation are of the form \[ f(x) = Ce^{x^2/2} + e^{x^2/2}\int_{-\infty}^x [h(y)-\mathbb{E}(h(N))]e^{y^2/2} dy \] In particular, denote by \[ f_h(x) = e^{x^2/2}\int_{-\infty}^x [h(y)-\mathbb{E}(h(N))]e^{y^2/2} dy \] In particular, $f_h$ is he only solution such that \[ \lim_{x \to \infty} e^{x^2/2} f_h(x) = 0 \]
Proof
$ \sqrt{2\pi}\int_{-\infty}^x h(y) \frac{e^{y^2/2}}{\sqrt{2\pi}} - \mathbb{E}(h(N))\int_{-/infty}^\infty \gamma(dx) = 0$
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