Function Spaces, Inverse Problems, and Risk Certificates · Chapter III-13

Hilbert Target Operators and Distribution States

A finite-dimensional perturbation can affect an entire response curve. Mapping the perturbation into a Hilbert space of targets yields an integrated Gram operator whose spectrum ranks policy-relevant directions. When the state itself is a distribution, tangent restrictions and sieve approximations determine which perturbations the calculation represents.

Conceptual map

  1. III-13.01Finite-to-integrated targets
  2. III-13.02Integrability
  3. III-13.03Spectra of target operators
  4. III-13.04Distribution tangents
  5. III-13.05Sieve approximation

1. A continuum of targets defines one operator

When a finite state perturbation changes an entire policy-response curve, the relevant object maps a direction into a function. Its Gram operator summarizes integrated sensitivity across the declared target measure.

Let (\(T,\mu\)) be a finite measure space and \(g:T\to \mathbb{R}^{d}\) a measurable response gradient with \(\int\lVert g(t)\rVert^{2}\,d\mu(t)<\infty\). Define \(B:\mathbb{R}^{d}\to L^{2}(\mu)\) by \((Bv)(t)=g(t)^{\top}v\). Its target Gram matrix is

\[G=B^{*}B=\int _{T}g(t)g(t)^{\top }d\mu (t).\](1)
Proposition 1 · Integrated response identity

The matrix \(G\) is positive semidefinite and

\[v^{\top }Gv=\int |g(t)^{\top }v|^{2}d\mu (t), \quad \operatorname{tr}(G)=\int \lVert g(t)\rVert ^{2}d\mu (t).\](2)

Proof. Move the finite sum in the quadratic form through the integral to obtain the first identity. Its integrand is nonnegative. Summing the diagonal entries of (1) gives the trace identity. ∎

2. A response curve on the unit interval

Take \(T\)=[0,1] with uniform measure and \(g(t)=(1,t)^{\top}\). Then

\[G=\begin{bmatrix}1 & \frac{1}{2} \\ \frac{1}{2} & \frac{1}{3}\end{bmatrix}.\](3)

The eigenvalues are \((4\pm \sqrt{13})/6\), approximately 1.26759 and 0.06574. Their sum 4/3 equals \(\int _{0}^{1}(1+t^{2})\,dt\). The leading eigenvector identifies the state direction with the largest integrated squared response under the chosen uniform weighting. A different target measure changes that economic ranking.

Approximating (3) on a grid with positive quadrature weights gives \(G_{K}=\sum _{j}w_{j}g(t_{j})g(t_{j})^{\top}\). Positivity survives at every grid size because each summand is positive semidefinite.

3. Distribution states and score directions

Let \(P\) have density \(p\) and let {\(P_{\varepsilon}\)} be a regular dominated submodel whose density is differentiable in \(L^{1}\) at zero with derivative \(p s\). Then \(E_{P}[s]=0\); assume also \(s\in L^{2}(P)\). The score \(s\) is a tangent direction, and the Fisher metric is \(\langle s_{1},s_{2}\rangle=E_{P}[s_{1}s_{2}]\). For a square-integrable query \(q\),

\[d/d\varepsilon E_{P_{\varepsilon }}[q]|_{\varepsilon =0}=E_{P}[(q-E_{P}q)s].\](4)

The centered query is the Riesz representer of this derivative on the mean-zero tangent space. Restrictions on admissible scores replace that space by a subspace and project the representer accordingly.

4. Finite-rank approximation and spectral gaps

In a general Hilbert domain, a Hilbert–Schmidt response map \(B\) has a positive trace-class Gram operator \(B^{*}B\). If finite-rank maps \(B_{K}\) converge in operator norm, then

\[\lVert B_{K}^{*}B_{K}-B^{*}B\rVert \le (\lVert B_{K}\rVert +\lVert B\rVert )\lVert B_{K}-B\rVert .\](5)

Eigenvalues then converge. Eigenspace stability additionally needs separation between the target eigenvalue cluster and the rest of the spectrum. A small gap makes the reported direction sensitive even when the Gram operator itself is estimated accurately.

Failure case · Matrix SVD used as an operator theorem

A finite grid produces a finite matrix and an SVD. Compactness, trace class, operator convergence, and eigenspace stability require integrability and approximation conditions beyond that computation.

5. Implementation, exercises, and sources

Normalize the target measure, use nonnegative quadrature weights, and check the trace identity against the summed gradient norm. Report spectral tails and eigenvalue gaps as the policy grid and state sieve expand.

Download the volume verification script →

Exercises

  1. Derive the exact eigenvalues in (3) and compute normalized eigenvectors.
  2. Approximate (3) with midpoint grids of sizes 5, 10, and 100; report operator-norm error and leading-direction error.
  3. For a three-point distribution, write the mean-zero score space and calculate the Riesz representer of one event probability.
Partial solutions

1. The characteristic polynomial of (3) is \(\lambda ^{2}-(4/3)\lambda+1/12\). Its roots are \((4\pm \sqrt{13})/6\). For either root, a direction proportional to \((1,2(\lambda-1))\) solves the eigenvector equation. 3. For probabilities \(p_{i}\), scores satisfy \(\sum p_{i}s_{i}=0\). The event-\(\{1\}\) derivative has representer \(1\{i=1\}-p_{1}\) under the Fisher inner product.

  1. John B. Conway, A Course in Functional Analysis, Chapters II, IX.Compact positive operators and spectral representation.
  2. Aad van der Vaart, Asymptotic Statistics, Chapter 25.Tangent spaces and pathwise derivatives.
  3. Tosio Kato, Perturbation Theory for Linear Operators.Spectral perturbation and separated eigenspaces.

6. Audit checkpoint

State the target measure, Hilbert spaces, integrability condition, state metric, quadrature rule, trace check, spectral tail, and relevant eigenvalue gaps. Identify which claims are finite-dimensional and which survive the limiting operator.

7. Scope boundary

The chapter develops Hilbert-valued target derivatives, integrated Gram operators, score tangents, and sieve diagnostics. General geometry of probability measures and PDE function spaces lie outside scope.

Prerequisites