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Correct-scale slab bound for multivariate trimming

Statement

Let X be an absolutely continuous random vector in Rd with mean μ and finite covariance matrix Σ as defined in Basic finite covariance matrix identities for robust mean bounds. Let X1,…,XN,Y1,…,YN be 2N iid clean copies and let their observed replacement sample have at most ⌊2ηN⌋ changed coordinates in total. Assume 0≤η≤1/10, 0<δ<1, N≥2560log⁡(2/δ), and ε=max⁡{10η,2560log⁡(2/δ)/N}≤1. If tr⁡Σ>0, put

Q0=max⁡{256εtr⁡ΣN, 16λmax⁡(Σ)ε}.

For the slabs and tail intersections in Adaptive multivariate trimmed mean, Every positive real lies below a dyadic scale less than twice as large supplies an integer i0 with 2i0∈[2Q0,4Q0). Then, with probability at least 1−δ, Ki0=⋂i≥i0Γ(2i) is nonempty and every z∈Ki0 satisfies ∥z−μ∥≤16εQ0. The positive-trace condition is required to make Q0>0.

Facts & Assumptions

Given: The clean iid halves, replacement budget and parameter domain in the Statement, with positive covariance trace.

[F1]

A variance-sensitive bound for bounded empirical suprema: for bounded ∣f∣≤B with Pf2≤s2, the centered supremum Z satisfies Z≤EZ+2(8EW+4Ns2)x+8Bx outside probability e−x, where W=sup⁡f∑if(Xi)2.

[F2]

Independent-process symmetrization for convex moments and One-sided coordinate Rademacher contraction supply ghost-sample symmetrization and coordinate contraction. In the proof below their one-sided forms are derived directly to keep the constants explicit.

[F3]

Basic finite covariance matrix identities for robust mean bounds gives E∥X−μ∥2=tr⁡Σ and E⟨X−μ,v⟩2≤λmax⁡(Σ) for unit v. Cauchy–Schwarz: ∣⟨x,y⟩∣≤∥x∥ ∥y∥, with equality exactly for dependent pairs and Markov's inequality for random variables give the norm and tail bounds used below.

[F4]

Adaptive multivariate trimmed mean defines the directional quantiles, clipped centers and slabs; Adversarial sample replacement permits at most 2ηN changes in either half, including sample-dependent choices.

[F5]

Dominated convergence passes bounded pointwise limits under integration. The iid finite product law is Independent random elements have product joint law; Every positive real lies below a dyadic scale less than twice as large gives the stated dyadic index.

[F6]

Since tr⁡Σ>0, d≥1, and Qd is countable and dense in Rd (Qn is a countable dense subset of Rn, and rational open boxes form a countable basis); normalizing its nonzero elements gives a countable dense subset of Sd−1 because normalization is continuous away from zero and every unit vector is nonzero.

Proof

Given: The objects in the Statement. Write r=tr⁡Σ/N, λ=λmax⁡(Σ) and x=εN/1280.

1.1F2F3F5F6algebra

Put D={q/∥q∥2:q∈Qd∖{0}} and include the zero vector. By [F6], D is countable and dense in Sd−1: rational vectors approximate every unit vector, and normalization is continuous at nonzero vectors. For each bounded continuous scalar map used below, the sample sums and their population expectations are continuous in direction, the latter by [F5]. Thus their suprema over D∪{0} equal the full directional suprema and are measurable. For any such class gv, use the independent clean half Y1,…,YN as the ghost copy of X1,…,XN; its product law and independence follow from [F5] and the iid hypothesis. When the same argument is applied to the Y half, swap the roles of the two clean halves. Jensen gives Esup⁡v∑i(gv(Xi)−Pgv)≤Esup⁡v∑i(gv(Xi)−gv(Yi)). Pair swapping inserts independent signs; separating the two halves gives at most 2Esup⁡v∑iσigv(Xi). For an L-Lipschitz scalar map ψ, averaging one sign with arbitrary remaining offsets Av gives 12sup⁡v,w(Av+Aw+ψ(tv)−ψ(tw))≤12sup⁡v,w(Av+Aw+L∣tv−tw∣). Swapping v,w shows that the final supremum equals the one with L(tv−tw); successive coordinate replacements prove one-sided contraction with factor L. Countable limits follow by monotone convergence after subtracting one fixed candidate, or bounded convergence on the finite sign space for a fixed sample. Finally set S=∑iσi(Xi−μ). Independence of the signs gives E∥S∥2=Ntr⁡Σ. Since u≤1+u2 for u≥0, E∥S∥<∞; then 0≤E(∥S∥−E∥S∥)2=E∥S∥2−(E∥S∥)2 gives E∥N−1S∥≤r.

2.1F1F3step 1.1algebra

Put h(t)=min⁡{1,(2∣t∣/Q0−1)+}. It is 2/Q0-Lipschitz, vanishes at zero and majorizes 1{∣t∣≥Q0}. By [F3], Ph(⟨X−μ,v⟩)≤4λ/Q02≤ε/64. For its centered supremum, step 1.1 gives EZ/N≤4r/Q0≤ε/64. Since h2≤h, EW/N≤ε/32, and its second moment is at most ε/64. Apply [F1] separately to each clean half with B=1. Except on probability e−x for each half, its maximal empirical h average is at most ε/32+25εx/(16N)+8x/N=ε/16+8ε/1280<ε/8. Thus each clean half has fewer than εN/8 projections of centered absolute value at least Q0, uniformly in direction.

2.2F1F3step 1.1algebra

Fix Q=2i0∈[2Q0,4Q0). Put gv(z)=ϕ−Q,Q(⟨z−μ,v⟩) and WQ(v)=N−1∑igv(Xi). Antipodal directions and odd clipping make the absolute centered supremum equal its one-sided counterpart. Step 1.1 gives EZ/N≤2r. The square of clipping is 2Q-Lipschitz and vanishes at zero, so the same symmetrization/contraction argument yields EW/N≤λ+4Qr for the squared-class supremum. Here ∣gv∣≤Q and Pgv2≤λ. Since r≤εQ/512 and λ≤εQ2/1024, [F1] bounds sup⁡v∣WQ(v)−PWQ(v)∣ outside probability e−x by 2r+219εQ2x/(256N)+8Qx/N<εQ/32. Also ∣Pgv∣≤E[∣⟨X−μ,v⟩∣1{∣⟨X−μ,v⟩∣>Q}]≤λ/Q≤εQ/1024, since the unclipped projection is centered.

3.1F4step 2.1algebra

Each observed half has at most 2ηN≤εN/5 changes. On both events of step 2.1, fewer than 13εN/40<εN/2 projections in either observed half are outside [⟨μ,v⟩−Q0,⟨μ,v⟩+Q0]. Both directional quantile ranks k=⌈εN/2⌉ and k=⌈(1−ε/2)N⌉ satisfy k≥εN/2 and N−k+1≥εN/2; in the potentially integral boundary the strict count inequality suffices. Hence both quantiles lie in that interval, including at ε=1. Write av=αv−⟨μ,v⟩ and bv=βv−⟨μ,v⟩, so −Q0≤av≤bv≤Q0.

4.1F4step 2.1step 3.1step 2.2algebra

For any clean centered projection t, the data-dependent clipping ϕav−Q,bv+Q(t) differs from ϕ−Q,Q(t) by at most Q0 and agrees with it when ∣t∣<Q−Q0. Since Q−Q0≥Q0, step 2.1 bounds the average difference by εQ0/8≤εQ/16. The data-dependent clipping interval has length at most 2Q+2Q0≤3Q, so first-half replacements change its average by at most 6ηQ≤3εQ/5. Combining these bounds with step 2.2 gives sup⁡v∣UQ(v)−⟨μ,v⟩∣≤(3/5+1/16+1/32+1/1024)εQ=3557εQ/5120<εQ. Thus μ∈Γ(Q) and every z∈Γ(Q) has ∥z−μ∥≤3εQ<12εQ0≤16εQ0.

5.1F4step 2.1step 2.2step 3.1step 4.1algebra∎

On the same events, for every R≥Q the clips at expanded intervals [av−R,bv+R] and [av−2R,bv+2R] differ by at most R. They differ only on observed centered projections with absolute value at least R−Q0≥Q0. Their observed number is less than 13εN/40 by step 3.1, so ∣U2R(v)−UR(v)∣≤13εR/40<2εR. Consequently Γ(R)⊆Γ(2R), and Ki0=Γ(Q) is nonempty with the required radius. The three exceptional events in steps 2.1 and 2.2 have total probability at most 3e−x≤3(δ/2)2≤δ, because εN≥2560log⁡(2/δ) and 0<δ<1. This proves the proposition simultaneously for every admissible replacement of the clean samples.

Remarks

The constant 4εQ0 in the former statement and source Proposition 1 is false because the slab width scales with the chosen dyadic Q, not Q0. The four-Q0 trimming slab radius is false gives an explicit continuous counterexample. The corrected bound preserves the main theorem's universal-constant rate. The zero-trace branch is Exact recovery by the multivariate trimmed mean at zero covariance.

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