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A centered Gaussian minimizes bounded symmetric quasi-convex loss

Statement

Assume AC. Let X∼Nd(m,Σ) with positive-definite covariance Σ. Let L:Rd→[0,M] be Borel measurable and symmetric, L(−x)=L(x), and quasi-convex, meaning each sublevel set {x:L(x)≤t} is convex. Then for every a∈Rd, EL(X−a)≥EL(X−m). Thus the Gaussian center m minimizes expected loss. The result includes quasi-convex losses whose sublevel sets are not closed.

Facts & Assumptions

Given: AC; a finite-dimensional nondegenerate Gaussian vector; and a bounded Borel measurable symmetric loss with convex sublevel sets.

[A1]

The Axiom of Choice: AC is assumed for the finite-dimensional multivariate normal construction and characteristic laws used here.

[F1]

Brunn–Minkowski inequality for compact convex sets: For nonempty compact convex U,V⊂Rd, λd(U+V)1/d≥λd(U)1/d+λd(V)1/d.

[F2]

The boundary of a convex set is Lebesgue null: A convex set and its closure differ only by a Lebesgue-null boundary; lower-dimensional convex sets are null.

[F3]

Multivariate normal law, including singular covariance, Standard normal and normal laws, and The standard normal density has total mass one: A nondegenerate Gaussian is an invertible affine image of a standard Gaussian vector with density (2π)−d/2e−∥z∥22/2. The Euclidean norm is the one in The Euclidean inner product ⟨x,y⟩=∑k<nxkyk on Rn.

[F4]

Tonelli's theorem for nonnegative measurable functions on a sigma-finite product: Nonnegative measurable integrands may be integrated in either order.

[F5]

A linear map T of Rn sends Lebesgue measurable sets to Lebesgue measurable sets, with λn(T[E])=∣det⁡T∣ λn(E) when T is invertible and T[E] Lebesgue null when it is not: An invertible linear map scales Lebesgue measure by the absolute determinant. In particular, reflection x↦−x preserves volume and scaling by 1/2 multiplies it by 2−d. Thus the unweighted inequality in [F1], applied to U,V, gives λd((U+V)/2)1/d≥λd(U)1/d+λd(V)1/d2.

[F6]

Lebesgue outer measure, Lebesgue measurability and Lebesgue measure are unchanged by translation: Translation preserves Lebesgue measure; accordingly, translating the variable in a Lebesgue integral does not change the integral after the integrand is translated.

[F7]

Heine-Borel in Rn: with the Euclidean metric a subset of Rn is compact if and only if it is closed and bounded, and the proof by bisection uses no choice principle; the same holds on the real line: Closed bounded subsets of Rd are compact. Thus intersections of the closed set C with the closed balls used below are compact and measurable.

Proof

Proof technique: prove the Gaussian shift inequality for convex level sets by Brunn–Minkowski, then integrate their indicators.

1.1F5F7givenalgebra

First let C⊆Rd be closed, symmetric, and convex. For each radius r>0 and shift v, put U=C∩(v+B‾(0,r)),V=C∩(−v+B‾(0,r)). They are compact convex sets by [F7], and V=−U, so they have equal volume by [F5]. For u∈U and w∈V, symmetry and convexity put (u+w)/2 in C, while u−v and w+v lie in the radius-r ball, so ∥(u+w)/2∥2=∥(u−v+w+v)/2∥2≤r. Thus (U+V)/2⊆C∩B‾(0,r). This sets up the Brunn–Minkowski comparison.

2.1F1F5step 1.1algebra

If U has positive volume, [F1] and its derived weighted form [F5] give λd(C∩B‾(0,r))≥λd((U+V)/2)≥λd(U), since λd(V)=λd(U). If U has zero volume the same inequality follows from nonnegativity. Therefore λd(C∩(v+B‾(0,r)))≤λd(C∩B‾(0,r)). This is the required shifted-volume inequality.

3.1F3F4F5F6step 2.1algebra

Let Z∼Nd(0,Id). Its density is a positive constant times e−∥z∥22/2. For any shift v, translation invariance [F6] and symmetry of C (using the reflection in [F5]) give P(Z∈C+v)=cd∫Ce−∥z+v∥22/2dz=cd∫Ce−∥z−v∥22/2dz, where cd>0 is the normalizing constant. The identity e−∥z−v∥22/2=∫0∞e−t1{∥z−v∥22/2≤t}dt and [F4] express the latter integral as cd∫0∞e−tλd(C∩(v+B‾(0,2t)))dt. By step 2.1, this is at most the same expression at shift zero. Hence P(Z∈C+v)≤P(Z∈C). This proves the Gaussian shift inequality.

4.1F2F6step 3.1given

If C is convex, symmetric, but not closed, replace it by C‾. The difference is contained in ∂C, which is null by [F2]; its translate is also null by [F6]. Thus the probability inequality in step 3.1 holds for every convex symmetric Borel set. If C has empty interior, [F2] makes both probabilities zero, which also covers this boundary case.

5.1A1F2F3step 4.1algebra

Write X=m+AZ with A=Σ1/2 invertible. For any symmetric convex Borel set C, the event X−a∈C is Z∈A−1C+A−1(a−m). The set A−1C is again symmetric convex, so step 4.1 gives P(X−a∈C)≤P(X−m∈C). Apply this to every sublevel set Ct={x:L(x)≤t}. This gives the comparison for each loss sublevel.

6.1F4step 5.1givenalgebra∎

For any random variable Y with 0≤Y≤M, EY=∫0MP(Y>t)dt, by [F4]. Step 5.1 says P(L(X−a)≤t)≤P(L(X−m)≤t) for each t, hence the corresponding tail probabilities are ordered in the reverse direction. Integrating them gives EL(X−a)≥EL(X−m). This proves the statement without requiring closed loss sublevels.

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