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ULA's Gaussian kernel satisfies an exponential drift bound

Statement

Assume AC. Let d≥1, U∈C2(Rd), and suppose ∇U is L-Lipschitz for L>0. Let x⋆ be a global minimizer with U(x⋆)=0. Suppose that for ρ>0, α∈(1,2], and Mρ≥0, ⟨∇U(x),x−x⋆⟩≥ρ∥x−x⋆∥αif ∥x−x⋆∥≥Mρ. For 0<γ<L−1, define Kγ:=max⁡{Mρ,(2d[−log⁡(1−Lγ)]/γ+4ρ2)1/(2(α−1))},V(x):=eU(x)/2, and let Pγ be the ULA proposal kernel. Then PγV(x):=∫V(y)Pγ(x,dy)≤e−γV(x)+eLKγ2/4(1−Lγ)−d/21{∥x−x⋆∥≤Kγ}.

Facts & Assumptions

Given: AC; d,L,U,x⋆,ρ,α,Mρ,γ as in the Statement; and the ULA update.

[A1]

U is twice continuously differentiable, has L-Lipschitz gradient, has the stated global minimizer and radial drift, and is normalized by U(x⋆)=0. The Jacobian matrix of partial derivatives and the gradient in the scalar-valued case

[F1]

At a differentiable local minimum in Euclidean space, the gradient is zero. Fermat's theorem: an interior differentiable local extremum has zero gradient

[F2]

The derivative of a composition with a differentiable path is given by the total-derivative chain rule, and a continuous derivative integrates to its endpoint difference. The chain rule for total derivatives: D(g∘f)(a)=Dg(f(a))∘Df(a) Newton–Leibniz needs only continuity on [a,b], differentiability on (a,b), and a Riemann-integrable extension of the interior derivative

[F6]
[F7]

Finite-dimensional Lebesgue measure is the finite product of one-dimensional Lebesgue measures on Borel sets, and Tonelli factors nonnegative product-measurable integrals. On Borel subsets of R^{m+n}, the product lambda_m times lambda_n agrees with lambda_{m+n} Tonelli's theorem for nonnegative measurable functions on a sigma-finite product

[F8]

Under [A1], U(x)≥c∥x−x⋆∥α−aα, where c=ρ/(α+1)>0 and aα is finite. Radial gradient drift forces potential coercivity

[F9]

Under countable choice, ∫Re−∣z∣ dz<∞. The real-line exponential tail is Lebesgue integrable

Proof

Given: The hypotheses in the Statement.

1.1A1F1F2F3

By [F1], ∇U(x⋆)=0. For h=y−x, apply [F2] to t↦U(x+th) and subtract ⟨∇U(x),h⟩ from the endpoint difference. The remaining integral is ∫01⟨∇U(x+th)−∇U(x),h⟩ dt≤∫01Lt∥h∥2 dt=L2∥h∥2, by [A1] and [F3]. Thus U(y)≤U(x)+⟨∇U(x),y−x⟩+L∥y−x∥2/2 for all x,y.

1.2A1F3algebra

Put r=∥x−x⋆∥. If r≥Mρ and r>0, the radial condition and [F3] give ρrα≤⟨∇U(x),x−x⋆⟩≤∥∇U(x)∥r, so ∥∇U(x)∥≥ρrα−1.

1.3F4F6F7

For c<1/2 and β∈R, completing the square and applying [F6] gives 12π∫Re−(1/2−c)z2+βz dz=(1−2c)−1/2eβ2/(2(1−2c)). For b∈Rd, apply this with β=bi for each i<d. The product density in [F4], Lebesgue product identification, and Tonelli's theorem [F7] therefore give, for Z∼Nd(0,Id), Eec∥Z∥2+⟨b,Z⟩=(1−2c)−d/2exp⁡ ⁣(∥b∥22(1−2c)).

1.4A1F3F5F6F7F8F9step 1.1algebra

Verify the target normalizer before using the proposal-kernel conclusion of [F4]. Put r=∥x−x⋆∥, c=ρ/(α+1), and k=c/d>0. Since rα≥r−1 for r≥0 and ∑i<d∣xi−x⋆,i∣≤d r by [F3], [F8] gives e−U(x)≤eaα+ce−cr≤eaα+c∏i<de−k∣xi−x⋆,i∣. Translation and scaling [F6], followed by [F7] and [F9], show that the right-hand side has finite integral. Step 1.1 also gives U(x)≤Lr2/2, so [F6]–[F7] imply ∫Rde−U(x) dx≥∫Rde−L∥x−x⋆∥2/2 dx=(2π/L)d/2>0. Continuity supplies Borel measurability as in [F5]. Thus all target hypotheses of the ULA algorithm and its proposal-kernel lemma hold.

2.1A1F4F5step 1.1step 1.3step 1.4algebra

Write g=∇U(x) and Y=x−γg+2γZ, the ULA update. Step 1.1 and [F4] imply EV(Y)V(x)≤Eexp⁡ ⁣(12⟨g,−γg+2γZ⟩+L4∥−γg+2γZ∥2). In step 1.3 take c=Lγ/2 and b=2γ(1−Lγ)g/2. Since 1−2c=1−Lγ>0, expanding the exponent and collecting its ∥g∥2 terms gives PγV(x)≤V(x)(1−Lγ)−d/2exp⁡ ⁣(−γ∥g∥24).

3.1A1step 1.2step 2.1algebra

If r≥Kγ, then step 1.2 and the definition of Kγ give d2[−log⁡(1−Lγ)]−γ∥g∥24≤d2[−log⁡(1−Lγ)]−γρ2Kγ2(α−1)4≤−γ. Step 2.1 therefore yields PγV(x)≤e−γV(x) on this region.

4.1A1F1step 1.1step 2.1step 3.1algebra∎

If r≤Kγ, use step 1.1 with starting point x⋆ and [F1] to obtain U(x)≤Lr2/2, so V(x)≤eLKγ2/4. Bounding the exponential factor in step 2.1 by one gives PγV(x)≤eLKγ2/4(1−Lγ)−d/2. Together with step 3.1, this proves the asserted drift inequality on both regions.

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