Paper VIReading edition

Gaussian transfer and Hermite packets

Reading tools
Reading libraryFind statementsInspect Lean
Switch work

Saved reading

Read side by side

Start reading

Resources & source

Original TeX with line links · Download TeX

The wording and mathematics follow the retained manuscript. This reading format does not add a proof review or extend Lean coverage.

Skip contents and start reading

E7 Gaussian transfer and Hermite packets

Let \(\gamma\) be the standard Gaussian probability measure on \({\mathbb R}\). For \(t\geq0\), define the Ornstein Uhlenbeck transfer

\[ ({\mathcal O}_t f)(x) = \int_{\mathbb R} f\left( {\mathrm e}^{-t}x+\sqrt{1-{\mathrm e}^{-2t}}\,y \right) \gamma({\,\mathrm d} y). \]

Let \(H_n\) be the probabilists' Hermite polynomial defined by

\[ \exp\left(ux-\frac{u^2}{2}\right) = \sum_{n=0}^\infty H_n(x)\frac{u^n}{n!}, \]

and set \(h_n=H_n/\sqrt{n!}\).

Theorem E7.1: Ornstein Uhlenbeck semigroup

The operators \(({\mathcal O}_t)_{t\geq0}\) form a positive Markov contraction semigroup on \(L^p(\gamma)\) for every \(1\leq p\leq\infty\). On \(L^2(\gamma)\), the semigroup is self adjoint and

\[ {\mathcal O}_t h_n={\mathrm e}^{-nt}h_n. \]

The family \((h_n)_{n\geq0}\) is an orthonormal basis of \(L^2(\gamma)\).

Proof of Theorem E7.1

Positivity and preservation of constants follow from the integral formula. If \(X\) and \(Y\) are independent standard Gaussian variables, then

\[ {\mathrm e}^{-s} \left( {\mathrm e}^{-t}x+\sqrt{1-{\mathrm e}^{-2t}}X \right) + \sqrt{1-{\mathrm e}^{-2s}}Y \]

has the same distribution as

\[ {\mathrm e}^{-(s+t)}x + \sqrt{1-{\mathrm e}^{-2(s+t)}}Z \]

with \(Z\) standard Gaussian. This proves the semigroup law. Jensen's inequality and invariance of \(\gamma\) give the \(L^p\) contraction. The joint Gaussian pair

\[ \left( X, {\mathrm e}^{-t}X+\sqrt{1-{\mathrm e}^{-2t}}Y \right) \]

is symmetric under interchange, which proves self adjointness.

Apply \({\mathcal O}_t\) to the Hermite generating function. Gaussian integration gives

\[ \begin{aligned} {\mathcal O}_t \exp\left(ux-\frac{u^2}{2}\right) &= \exp\left( {\mathrm e}^{-t}ux- \frac{{\mathrm e}^{-2t}u^2}{2} \right)\\ &= \sum_{n=0}^\infty {\mathrm e}^{-nt}H_n(x)\frac{u^n}{n!}. \end{aligned} \]

Comparison of coefficients proves the eigenvalue formula. The same generating function shows

\[ \int H_mH_n{\,\mathrm d}\gamma=n!\delta_{mn}. \]

The Hermite polynomials span all polynomials, and polynomials are dense in \(L^2(\gamma)\). Hence the normalized family is an orthonormal basis. See [Janson1997] for the general Gaussian Hilbert space setting.

Corollary E7.2: Hermite packet reconstruction

Let \(P_n\) be the orthogonal projection onto \({\mathbb C} h_n\). Then

\[ I=\sum_{n=0}^\infty P_n \]

in the strong operator topology and

\[ {\mathcal O}_t = \sum_{n=0}^\infty{\mathrm e}^{-nt}P_n. \]

For \(f\in L^2(\gamma)\),

\[ {\left\lVert{\mathcal O}_t f\right\rVert}_2^2 = \sum_{n=0}^\infty {\mathrm e}^{-2nt}{\left\lVert P_nf\right\rVert}_2^2. \]

Proof of Corollary E7.2

Apply Parseval's identity and the eigenvalue formula in Theorem E7.1.

Proposition E7.3: Generator and Dirichlet form

On the polynomial subspace, the infinitesimal generator of \(({\mathcal O}_t)\) is the differential operator

\[ {\mathcal L} f=f''-xf'. \]

It satisfies

\[ {\mathcal L} h_n=-nh_n. \]

For every polynomial \(f\),

\[ {\left\langle-{\mathcal L} f,f\right\rangle}_{L^2(\gamma)} = \int_{\mathbb R}{\left\lvert f'(x)\right\rvert}^2\gamma({\,\mathrm d} x). \]

Proof of Proposition E7.3

Write

\[ \rho_t={\mathrm e}^{-t}=1-t+O(t^2), \qquad \sigma_t^2=1-{\mathrm e}^{-2t}=2t+O(t^2). \]

For a polynomial \(f\), Taylor expansion at \(x\) and Gaussian integration give

\[ \begin{aligned} {\mathcal O}_tf(x) ={}&f(x) +f'(x)(\rho_t-1)x +\frac12f''(x)\sigma_t^2 +o(t)\\ ={}&f(x)+t\bigl(f''(x)-xf'(x)\bigr)+o(t). \end{aligned} \]

Every omitted term is a polynomial in the Gaussian variable multiplied by a quantity that is \(o(t)\), so the expansion may be integrated term by term. Therefore

\[ \left.\frac{{\,\mathrm d}}{{\,\mathrm d} t}{\mathcal O}_tf\right|_{t=0} =f''-xf'. \]

The Hermite eigenvalue identity also follows by differentiating \( {\mathcal O}_th_n={\mathrm e}^{-nt}h_n \) at zero. Gaussian integration by parts gives

\[ \int_{\mathbb R} f'(x)\overline{g(x)}\gamma({\,\mathrm d} x) = \int_{\mathbb R} f(x)\overline{xg(x)-g'(x)}\gamma({\,\mathrm d} x). \]

Set \(g=f'\) and rearrange.

Corollary E7.4: Gaussian spectral gap

If \(f\in L^2(\gamma)\) has mean zero, then

\[ {\left\lVert{\mathcal O}_tf\right\rVert}_2 \leq {\mathrm e}^{-t}{\left\lVert f\right\rVert}_2. \]

For every polynomial \(f\),

\[ {\operatorname{Var}}_\gamma(f) \leq \int_{\mathbb R}{\left\lvert f'(x)\right\rvert}^2\gamma({\,\mathrm d} x). \]

Proof of Corollary E7.4

A mean zero function has no \(h_0\) component, so every surviving Hermite multiplier is at most \({\mathrm e}^{-t}\). For a polynomial

\[ f-{\mathbb E}_\gamma f=\sum_{n\geq1}c_nh_n. \]

Then

\[ {\operatorname{Var}}_\gamma(f)=\sum_{n\geq1}{\left\lvert c_n\right\rvert}^2 \leq \sum_{n\geq1}n{\left\lvert c_n\right\rvert}^2 = {\left\langle-{\mathcal L} f,f\right\rangle}. \]

Apply Proposition E7.3.

Corollary E7.5: Fractional Hermite transfer

Let \(-{\mathcal L}\) be the nonnegative Ornstein Uhlenbeck number operator with

\[ -{\mathcal L} h_n=nh_n. \]

For every \(\alpha>0\),

\[ {\mathrm e}^{-t(-{\mathcal L})^\alpha}f = \sum_{n=0}^\infty {\mathrm e}^{-tn^\alpha}P_nf. \]

This is a contraction semigroup on \(L^2(\gamma)\).

Proof of Corollary E7.5

The spectral theorem applies to the orthonormal Hermite basis. Every multiplier has modulus at most one and obeys the scalar semigroup law.

Hermite packet multipliers for the Ornstein Uhlenbeck semigroup and two fractional powers of its number operator.
Hermite packet multipliers for the Ornstein Uhlenbeck semigroup and two fractional powers of its number operator.

View full-size figure (new tab)

Source and conversion record

Source SHA-256: 736e615131f57daf341b6cb0600761d58950450947c85d433206148cca228333

Unsupported prose commands stop the build. The mathematical expression sequence is checked against the source, with manuscript macros expanded for display.

Conversion records

Notation in Paper VI

Look up a symbol without leaving this chapter. Select text before opening help to search for it.

Search this work’s notation.

    Symbols can have different meanings in different passages. Read each result in its own context.

    Open the full notation index