TheoremBase

Moment and Tail Bounds on the Wiener Chaos up to a Given Order

Every FF in the Wiener chaos up to order mm has finite moments of all orders, with ∥F∥q≤(q−1)m/2∥F∥2\lVert F\rVert_q\le(q-1)^{m/2}\lVert F\rVert_2 for q≥2q\ge2; and, for m≥1m\ge1 and ∥F∥2≤σ\lVert F\rVert_2\le\sigma, it has the tail bound γc(∣F∣≥s)≤exp⁡(−m2e(s/σ)2/m)\gamma_c(|F|\ge s)\le\exp(-\frac{m}{2e}(s/\sigma)^{2/m}) for s≥(2e)m/2σs\ge(2e)^{m/2}\sigma.

Statement

In the setting of Gaussian Analysis Relative to a Diagonal Gaussian Reference Measure with Noise Weights: Standing Notation, with the Lebesgue spaces Lp(γc)L^{p}(\gamma_{c}) and norms ∥⋅∥p\lVert\cdot\rVert_{p} of Gaussian Analysis Relative to a Diagonal Gaussian Reference Measure with Noise Weights: Standing Notation §lebesgue and the chaos up to order mm H≤m\mathcal{H}_{\le m} of The Wiener Chaoses of a Diagonal Gaussian Measure on a Hilbert Space. exp⁡\exp is the exponential function, e=exp⁡(1)\mathrm{e}=\exp(1), and powers of positive real numbers with real exponents are those of Real Power of a Positive Real Number. Let m∈N0m\in\mathbb{N}_{0} and F∈H≤mF\in\mathcal{H}_{\le m}, and let f:X→Rf:X\to\mathbb{R} be a Borel function in the class FF.

1. (Moment bounds) For every real q≥2q\ge2, ∫X∣f∣q dγc<∞\int_{X}|f|^{q}\,d\gamma_{c}<\infty, so that F∈Lq(γc)F\in L^{q}(\gamma_{c}), and

∥F∥q≤(q−1)m/2 ∥F∥2,\lVert F\rVert_{q}\le(q-1)^{m/2}\,\lVert F\rVert_{2},

where (q−1)0=1(q-1)^{0}=1.

2. (Tail bound) Suppose m≥1m\ge1, and let σ∈R\sigma\in\mathbb{R} be positive with ∥F∥2≤σ\lVert F\rVert_{2}\le\sigma. Then for every real s≥(2e)m/2σs\ge(2\mathrm{e})^{m/2}\sigma,

γc({x∈X:∣f(x)∣≥s})≤exp⁡(−m2e(sσ)2/m).\gamma_{c}\bigl(\{x\in X:|f(x)|\ge s\}\bigr)\le\exp\Bigl(-\frac{m}{2\mathrm{e}}\Bigl(\frac{s}{\sigma}\Bigr)^{2/m}\Bigr).

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