TheoremBase

Admissible Cylindrical Potentials on a Hilbert Space in the Noise Geometry

An admissible cylindrical potential is a twice continuously differentiable function of finitely many coordinates that is bounded below, semiconvex in the noise norm, has slope controlled by its value and weighted Laplacian controlled by its squared slope; its noise gradient is fixed alongside.

Statement

In the settings of A Diagonal Gaussian Reference Measure on the Noise Wasserstein Space, Rescaled Heads and Gaussian Tails: Standing Notation and Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation, with the coordinates xkx_{k} and the maps pn:X→Rnp_{n}:X\to\mathbb{R}^{n} of clause A Diagonal Gaussian Reference Measure on the Noise Wasserstein Space, Rescaled Heads and Gaussian Tails: Standing Notation §background of the first, the noise weights aa, the noise space XaX^{a} with norm ∣⋅∣a|\cdot|_{a} and orthonormal basis (fk)k∈N(f_{k})_{k\in\mathbb{N}}, and the orthonormal basis (ek)k∈N(e_{k})_{k\in\mathbb{N}} of XX, let d∈Nd\in\mathbb{N}; Rd\mathbb{R}^{d} is open by claim 1 of Euclidean Space is Open in Itself, and CkC^k Maps are Continuous. Let v:Rd→Rv:\mathbb{R}^{d}\to\mathbb{R} be of class C2C^{2} on Rd\mathbb{R}^{d} in the sense of C^k Maps on a Euclidean Open Set, with partial derivatives ∂kv\partial_{k}v and ∂j∂kv\partial_{j}\partial_{k}v (j,k∈[d]j,k\in[d]) as in Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation §derivatives. Let K∈RK\in\mathbb{R} be nonnegative.

(Admissible cylindrical potential) The function V=v∘pd:X→RV=v\circ p_{d}:X\to\mathbb{R} is an admissible cylindrical potential with head dimension dd, profile vv and semiconvexity constant KK in the noise norm if the following four conditions hold. Dependents say ``an admissible cylindrical potential V=v∘pdV=v\circ p_{d}'', meaning that the datum (d,v,K)(d,v,K) is fixed with it.

(a) (Lower bound) There is b∈Rb\in\mathbb{R} with −b≤v(u)-b\le v(u) for every u∈Rdu\in\mathbb{R}^{d}.

(b) (Semiconvexity in the noise norm) The Hessian of vv is bounded below by −K-K times the noise quadratic form: for all u,h∈Rdu,h\in\mathbb{R}^{d},

∑j=1d∑k=1d∂j∂kv(u) hjhk ≥ −K∑k=1dhk2ak.\sum_{j=1}^{d}\sum_{k=1}^{d}\partial_{j}\partial_{k}v(u)\,h_{j}h_{k}\ \ge\ -K\sum_{k=1}^{d}\frac{h_{k}^{2}}{a_{k}} .

(c) (Slope bound) There is C∈RC\in\mathbb{R} with

∑k=1dak(∂kv(u))2 ≤ C (1+∣v(u)∣)2for every u∈Rd.\sum_{k=1}^{d}a_{k}\bigl(\partial_{k}v(u)\bigr)^{2}\ \le\ C\,\bigl(1+|v(u)|\bigr)^{2}\qquad\text{for every }u\in\mathbb{R}^{d}.

(d) (Curvature small against the slope) For every positive ε∈R\varepsilon\in\mathbb{R} there is Cε∈RC_{\varepsilon}\in\mathbb{R} with

∑k=1dak ∂k∂kv(u) ≤ ε∑k=1dak(∂kv(u))2+Cε(1+∑k=1duk2)for every u∈Rd.\sum_{k=1}^{d}a_{k}\,\partial_{k}\partial_{k}v(u)\ \le\ \varepsilon\sum_{k=1}^{d}a_{k}\bigl(\partial_{k}v(u)\bigr)^{2}+C_{\varepsilon}\Bigl(1+\sum_{k=1}^{d}u_{k}^{2}\Bigr)\qquad\text{for every }u\in\mathbb{R}^{d}.

(Noise gradient) For such VV, the noise gradient of VV is the map ∇aV:X→Xa\nabla_{a}V:X\to X^{a},

∇aV(x)=∑k=1dak ∂kv(pd(x)) ek(x∈X),\nabla_{a}V(x)=\sum_{k=1}^{d}a_{k}\,\partial_{k}v\bigl(p_{d}(x)\bigr)\,e_{k}\qquad(x\in X),

a finite linear combination of the vectors eke_{k}; XaX^{a} is a linear subspace of XX by The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §hilbert and contains each ek=ak−1/2fke_{k}=a_{k}^{-1/2}f_{k} by The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §basis, so ∇aV(x)∈Xa\nabla_{a}V(x)\in X^{a}. For k∈Nk\in\mathbb{N} write ∂kV(x)=∂kv(pd(x))\partial_{k}V(x)=\partial_{k}v(p_{d}(x)) if k≤dk\le d and ∂kV(x)=0\partial_{k}V(x)=0 if k>dk>d. Here ∇aV\nabla_{a}V and ∂kV\partial_{k}V are notations for the displayed functions.

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