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A compact diagonal model displays the Tikhonov bias-noise balance

Example

Assume Countable Choice and write N+={1,2,…}. Let A be the compact diagonal map on ℓ2(N+,R) given by Aen=n−1en. Fix N≥2 and 0<ν≤1, take w=e1+eN, source target x†=(A∗A)νw, noise e=−N−(2ν+1)eN, and λ=N−2. Then ∥w∥=2, the noise level is δ=N−(2ν+1), and the exact Tikhonov bias and filtered noise each contribute 12N−2ν in the eN direction. The total error is of order N−2ν, while the balancing parameter is comparable to (δ/2)2/(2ν+1). The same operator also exhibits saturation: for any μ>1, the unit source w=e1 gives x†=e1 and exact-data bias λ/(1+λ), which is not O(λμ).

Facts & Assumptions

Given: Countable Choice, the real sequence Hilbert space ℓ2(N+,R), its standard basis (en), the diagonal map Aen=n−1en, an integer N≥2, an exponent 0<ν≤1, and the data and parameter in the Statement; for the separate saturation calculation, also fix any exponent μ>1.

[F1]

Square-summable families on an arbitrary index set and the space ℓ2(I): The canonical sequence norm is ∥x∥22=∑n∣xn∣2, and (en) is orthonormal.

[F2]

The real square-summable sequence space is complete: The real ℓ2 sequence space is complete.

[F3]

Hilbert space: A complete real inner-product space is a real Hilbert space.

[F4]

Bounded finite rank operators are compact: Bounded finite-rank maps are compact.

[F5]

Norm limit of compact operators is compact: A norm limit of compact operators into a Banach space is compact.

[F6]

Compact spectral filters, source conditions, and qualification: The source condition Sνw and Tikhonov filter use S=A∗A and gλ(t)=1/(t+λ).

[F7]

Hilbert-space Tikhonov amplifies data by at most 1/(2λ): The filtered noise norm is bounded by ∥e∥/(2λ).

[F8]

Tikhonov source-condition rates balance noise at qualification one: For 0<ν≤1, source radius R gives error bound Rλν+δ/(2λ).

Verification

1.1givenF1F2F3F4F5algebra

Relabelling coordinates by k↦k+1 is an isometry from the complete space ℓ2(N,R) in [F2] to ℓ2(N+,R), so the latter is Hilbert. For M≥1, let AMen=n−1en for n≤M and AMen=0 for n>M. Since n−1≤1, both A and AM are bounded by one, and AM has finite rank. Also ∥(A−AM)x∥22=∑n>Mn−2∣xn∣2≤(M+1)−2∥x∥22, with equality at x=eM+1. Thus ∥A−AM∥=1/(M+1)→0. By [F3]–[F5], A is a bounded compact operator on a Hilbert space.

1.2givenF1F6algebra

For every x∈ℓ2, the coordinate inner product gives ⟨Ax,en⟩=n−1xn=⟨x,n−1en⟩, so the adjoint identity yields A∗en=n−1en and Sen=n−2en. Thus the source target is x†=e1+N−2νeN. Its forward image is y=e1+N−(2ν+1)eN. The chosen noise cancels the eN datum, so yδ=y+e=e1 and ∥e∥=δ=N−(2ν+1).

2.1F6step 1.2algebra

The Tikhonov filter applied to yδ=e1 gives xλδ=(1+λ)−1e1. Hence x†−xλδ=λ1+λe1+N−2νeN, and, at λ=N−2, ∥x†−xλδ∥2=(N2+1)−2+N−4ν. The exact-data bias in the eN coordinate is λN−2ν/(N−2+λ)=12N−2ν; the noise output in that coordinate is (1/N)(N−2+λ)−1(−N−(2ν+1))=−12N−2ν. Their contributions to solution error add.

3.1F7F8step 1.2step 2.1algebra

For 0<ν≤1, N−2≤N−2ν, so the displayed error lies between N−2ν and 2N−2ν. Also δ/(2λ)=12N−2ν and (δ2)2/(2ν+1)=N−22−1/(2ν+1), so the selected λ=N−2 differs from the balancing value by a factor between 1 and 2. These exact coordinates exhibit the stated bias-noise balance.

4.1F1F6step 1.1step 1.2algebra∎

For the separate exponent μ>1, take the unit source w=e1. Since Se1=e1 by step 1.2, the source target is x†=Sμw=e1 and the exact datum is y=Ae1=e1. For every x, ⟨Ax,e1⟩=x1=⟨x,e1⟩, so the adjoint identity gives A∗e1=e1. The Tikhonov solution is therefore xλ=(1+λ)−1e1. Hence ∥x†−xλ∥λμ=λ1−μ1+λ⟶+∞(λ↓0). This unit source therefore has bias not O(λμ).

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