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Certifying quantities of interest from aggregate approximation guarantees

Methods note: a coverage-aware, finite-tolerance theory of how approximation contracts constrain errors in derived scientific quantities. Compact U(1) spectral inference, graph sparsification, and a POD hot-spot example provide qualified reference applications; numerical values belong only to their stated instances.

Main contribution. The note distinguishes the full fidelity modulus, a certification-restricted modulus, and a family-restricted computable floor. It identifies when a searched family yields an exact certificate, when it yields only a one-sided condemnation result, and when local condition-number reasoning has already failed at the operating tolerance.

Supporting structure. Elementary order properties organize the admissible guarantees and restrictions. They are used as bookkeeping and composition tools, not claimed as the principal mathematical novelty.


1. Problem

Approximations are validated in norms that aggregate error over the state space; conclusions are drawn from a small set of derived quantities. A reduced-order model is accepted on residual error and read for a stability margin; a surrogate is accepted on held-out loss and read for a decay rate. The validated quantity and the relied-on quantity differ, and nothing in the validation says whether the first controls the second.

This note studies what can be certified at an operating tolerance, not merely in the infinitesimal limit. It separates the full admissible discrepancy from the discrepancy remaining after certification gates and from the value found by a searched perturbation family. The main questions are whether that search has coverage, whether local conditioning remains predictive at the tolerance in use, and whether the resulting restricted modulus can be computed with a certified numerical error.

1.1 Closest prior work and the remaining gap

The premise that global or aggregate approximation error need not control a specific output is established prior art. Goal-oriented a posteriori error estimation, including the dual-weighted residual method, estimates error in a user-declared functional rather than only in an energy or residual norm (Becker and Rannacher, 2001; Oden and Prudhomme, 2001; Prudhomme and Oden, 1999). Certified reduced-basis methods likewise provide rigorous output bounds for parametrized models and use those bounds to drive efficient approximation (Patera and Rozza, 2007; Rozza, Huynh, and Patera, 2008). TransferMod therefore does not claim to discover the distinction between state error and output error.

Optimal Uncertainty Quantification (OUQ) is the closest optimization-level relative. OUQ places the objective and the assumptions/information set at the center and computes optimal bounds by extremizing over compatible scenarios (Owhadi et al., 2013). The fidelity modulus has the same broad max-over-an- admissible-set form. The difference is one of declared object and operational use: here the admissible set is induced by an approximation contract and, optionally, by certification gates; the objective is discrepancy in a specified quantity of interest at a finite operating tolerance; and an incomplete search is reported explicitly as a family-restricted lower bound rather than as the full optimum.

Backward error analysis supplies another close conceptual precedent. It asks whether a computed answer is exact for a nearby problem, while conditioning translates that nearby-problem statement into forward error. TransferMod begins from the corresponding approximation neighborhood and studies the complete finite-tolerance output discrepancy, including regimes in which the local condition number is finite but no longer predictive.

The contribution claimed here is consequently narrower:

  1. a single notation separating the full modulus ω, the gate-restricted modulus ω_D, and a computable family-restricted value ω_{D,Θ};
  2. a coverage criterion distinguishing exact certification from a certified one-sided floor;
  3. finite-tolerance diagnostics for the regime in which first-order conditioning has failed;
  4. gates treated as restrictions of the admissible family, with Silent Risk as a measure-qualified summary of admitted decision-corrupting alternatives;
  5. constructive and empirical reference cases that report negative as well as positive findings.

Classical UQ, robust optimization, and adversarial robustness remain relevant but are not the closest novelty comparators. Classical probabilistic UQ propagates a distribution, posterior, or ensemble to output uncertainty. Robust optimization chooses a decision under an uncertainty set. Adversarial examples construct small perturbations that alter a classifier. TransferMod instead asks for the sharpest finite-tolerance implication from a declared approximation and certification contract to a declared scientific conclusion. A probabilistic credible set may define the admissible family, and a goal-oriented estimator may supply an upper bound, but neither identification changes the epistemic status of an uncovered family search.

1.2 Roadmap of the substantive results

Section 2 fixes notation and only the structural facts needed later. Section 3 separates four finite-tolerance regimes and identifies the crossover beyond which first-order conditioning is no longer predictive. Sections 4–6 develop restricted moduli, coverage-aware certification, and effective computation. Section 7 tests those claims on constructed and empirical references, including negative results. The exact structured cases then show where coverage can be proved rather than assumed.

2. Transfer guarantees and the fidelity modulus

2.0 Declared decision geometry

The general inferential object is specified by an approximation seminorm, a decision functional Q, a target u, and a declared discrepancy ℓ : Y × Y → [0,∞] on the decision space. Define

ω_{Q,ℓ}(ε;u) = sup{ ℓ(Q(u′),Q(u)) : ‖u′−u‖_A ≤ ε }.

For fixed , a transfer guarantee is any g that dominates every displayed discrepancy on each approximation ball. The proof of Proposition 2.1 uses only the least-upper-bound property and therefore carries over verbatim: ω_{Q,ℓ} is the pointwise-minimal transfer guarantee. Admissible-set restriction is also geometry-agnostic.

The choice of is substantive. Absolute, relative, and stabilized-relative geometries encode different decision semantics. Relative discrepancy is ill-conditioned near a zero reference and must not be treated as universal. Composition, naturality, and differential claims require assumptions appropriate to the chosen geometry. In particular, the condition-number results below are statements about the relative specialization.

A reference-free companion is the decision diameter

diam_{Q,ℓ}(D)=sup{ℓ(Q(u′),Q(u″)):u′,u″∈D}.

It measures variation across the admissible family rather than deviation from a declared center.

2.1 Relative-error specialization used in the reference application

Let X be a normed space, ‖·‖_A a seminorm on X (the approximation seminorm), Q : X → ℝ a quantity of interest, and u ∈ X a target. This section specializes to ℓ_rel(q,q₀)=|q-q₀|/|q₀|, so the standing assumption is Q(u) ≠ 0.

‖·‖_A is a seminorm and its kernel is central, not technical: if Q is non-constant on {u′ : ‖u′ − u‖_A = 0} then ω(ε) ≥ c > 0 for every ε, so Q is uncertifiable by Corollary 3.2. Continuity in Theorem 3.1 is continuity on the pseudometric space (X, d_A), equivalently on X/∼_A: Q is certifiable only if it is constant, or approximately controlled, on observational equivalence classes.

Definition 2.1 (transfer guarantee). g : (0,∞) → [0,∞] is a transfer guarantee for (Q, ‖·‖_A) at u if ‖u′ − u‖_A ≤ ε ⟹ |Q(u′) − Q(u)|/|Q(u)| ≤ g(ε) for all u′, ε. These form a set 𝒢 ordered pointwise; smaller is stronger. 𝒢 is never empty — g ≡ ∞ belongs to it — so asking for a least element is not vacuous.

A transfer guarantee is exactly what licenses "validated to aggregate accuracy ε, therefore the conclusion is accurate to g(ε)".

Definition 2.2 (fidelity modulus). ω(ε) = sup{ |Q(u′) − Q(u)|/|Q(u)| : ‖u′ − u‖_A ≤ ε }.

Intuition — an exchange rate between errors.
Think of (\omega(\varepsilon)) as the worst-case exchange rate between validation currency and conclusion currency. If validation permits (\varepsilon) units of error, (\omega(\varepsilon)) is the greatest downstream discrepancy still compatible with that contract. Proposition 2.1 shows that no uniformly smaller guarantee can be valid.

Remark. In the general formulation, ω depends on four declared objects — the approximation relation, the quantity of interest, the decision discrepancy, and the reference point u — and is independent of any certification procedure. This relative specialization fixes the discrepancy and therefore displays only the other three. The restriction ω_D of §4 adds a fourth, the certified set D.

Definition 2.3 (certifiability). Q is (ε₀, τ)-certifiable by ‖·‖_A at u if ω(ε₀) ≤ τ.

Proposition 2.1 (least guarantee and finite-locus slack). The complete lattice of transfer guarantees is the principal upper set

𝒢 = {g : g ≥ ω}.

Hence ω ∈ 𝒢 and is the unique least transfer guarantee. On the finite locus

F_g = {ε : ω(ε) < ∞ and g(ε) < ∞},

each g ∈ 𝒢 has the unique additive decomposition g(ε)=ω(ε)+s_g(ε) with s_g(ε)=g(ε)-ω(ε) ≥ 0.

Proof. For g ∈ 𝒢, g(ε) is an upper bound for the set defining ω(ε). Because a supremum is the least upper bound, ω(ε)≤g(ε) for every ε. Conversely, every g≥ω dominates every admissible decision discrepancy and is therefore a transfer guarantee. Thus 𝒢={g:g≥ω}, and antisymmetry gives uniqueness of its least element. Where both values are finite, ordinary subtraction defines the unique non-negative slack. No unique additive slack is claimed at points with extended-real value , where ∞-∞ is undefined. ∎

Corollary 2.1 (minimal transfer assignment). Let T′ assign to each quantity of interest a transfer guarantee for (Q, ‖·‖_A) at u, and require that T′(Q) be the least element of 𝒢(Q) for every Q. Then T′ = T.

Proof. Least elements of a partial order are unique, and Proposition 2.1 identifies that of 𝒢(Q) as ω_Q. ∎

So T is canonical, not merely convenient — but the uniqueness is relative to minimality. Drop that requirement and other operators into 𝒢 exist: Q ↦ 2ω_Q assigns a valid transfer guarantee to every Q, and satisfies several items of Proposition 2.2. What singles out T is that its value is the least valid guarantee at each Q, which is exactly what Proposition 2.1 supplies. Whether the structural axioms alone — without reference to 𝒢 — pin T down is the open question of §9.

Interpretation. Proposition 2.1 is an organizing fact: ω is the smallest valid guarantee, and any finite alternative guarantee differs from it by non-negative slack. The paper does not claim this supremum argument as its main novelty; it fixes the reference object used in the finite-tolerance and coverage results below.

Basic properties used later

The transfer operator is the canonical assignment sending each quantity of interest to the least transfer guarantee compatible with the approximation geometry:

T : Q ↦ ω_Q, at fixed u and ‖·‖_A.

Write also R : D ↦ ω_D for the map sending an admissible set to the modulus restricted to it. The items below are properties of these two operators, collected into one theorem because they describe one object, not six.

Proposition 2.2 (basic properties). The following elementary properties are collected for later use. Items (7) and (8) are the substantive composition and product estimates; the remaining items follow directly from the definition as a supremum over nested or restricted sets.

(a) Dependence on the tolerance.

  1. ω is non-decreasing in ε; hence ω(0⁺) := lim_{ε↓0} ω(ε) = inf_ε ω(ε) exists in [0,∞] and ω has at most countably many discontinuities.
  2. ω(0⁺) = 0 iff Q is ‖·‖_A-continuous at u (Theorem 3.1).

(b) Dependence on the data. 3. T(αQ) = T(Q) for α ≠ 0; T is not translation invariant, ω[Q + β] rescaling by |Q(u)|/|Q(u) + β|. 4. If ‖·‖_A ≤ K‖·‖_{A′} then ω_{A′}(ε) ≤ ω_A(Kε): a stronger validation seminorm can only shrink the modulus.

  1. ω|_{(0,ε₀]} depends only on Q|_{B_{ε₀}}.
  2. If Q′(u) = Q(u) and sup_{B_ε}|Q′ − Q| ≤ η then |ω′(ε) − ω(ε)| ≤ η/|Q(u)|: T is 1-Lipschitz in Q under the sup-norm on the ball.

(c) Operations on problems. 7. Composition. ω̂[id](ε) = ε, and with V_ε = Q₁({u′ : ‖u′ − u‖_A ≤ ε}),

 `ω̂[Q₂ ∘ Q₁](ε) ≤ sup_{v ∈ V_ε} ω̂[Q₂, ‖·‖_B, v]( ω̂[Q₁](ε) )`,

which reduces to ω̂₂ ∘ ω̂₁ when ω̂[Q₂] is uniform over V_ε. So T is lax functorial, the failure of strictness being the composition slack. 8. 1 + ω_{Q₁⊗Q₂} ≤ (1 + ω_{Q₁})(1 + ω_{Q₂}); equivalently log(1 + ω) is subadditive under tensor products.

  1. R is monotone: D ⊆ D′ ⟹ ω_D ≤ ω_{D′}, with ω_X = ω.
  2. R preserves joins exactly and meets only laxly: ω_{D ∪ D′} = ω_D ∨ ω_{D′} but in general ω_{D ∩ D′} ≤ ω_D ∧ ω_{D′}, with strict inequality possible.

Proof. (1) balls nest. (2) Theorem 3.1. (3) the ratio is unchanged under scaling of Q; under translation the numerator is unchanged and the denominator becomes |Q(u) + β|. (4) the ‖·‖_{A′}-ball of radius ε sits inside the ‖·‖_A-ball of radius . (5) B_ε ⊆ B_{ε₀}. (6) |Q′(u′) − Q′(u)| ≤ |Q(u′) − Q(u)| + η and symmetrically. (7) ‖u′ − u‖_A ≤ ε gives ‖Q₁u′ − Q₁u‖_B ≤ ω̂[Q₁](ε), so Q₁u′ lies in the ω̂[Q₁](ε)-ball about Q₁u ∈ V_ε; apply the definition of ω̂[Q₂] at that base point and take the supremum over V_ε. (8) |Q₁′Q₂′ − Q₁Q₂| ≤ |Q₁′ − Q₁||Q₂′| + |Q₁||Q₂′ − Q₂|, divided by |Q₁Q₂|. (9) a supremum over a subset is no larger. (10) sup_{D ∪ D′} = max(sup_D, sup_{D′}) exactly, whereas sup_{D ∩ D′} is bounded by each and may be strictly below both. ∎

The proposition is included to make later dependencies explicit. In particular, restriction of an admissible set cannot increase the modulus, while composition produces a generally non-tight upper bound whose slack is analyzed next.

Corollary 2.2 (why stage-wise certification helps). Item 10 is the structural reason gates compose usefully. Adding a test intersects admissible sets, and intersection can drive the modulus strictly below the minimum of the two component moduli — a stricter guarantee than either test provides alone. Union, by contrast, gives nothing: certifying against a wider family is exactly as weak as its weakest part. This is a geometric statement about restriction of the admissible set, not a probabilistic statement about independence among tests. Two gates derived from the same information basis can tighten the restricted modulus without constituting independent confirmations.

Proposition 2.3 (reparameterisation of Q). Let h : ℝ → ℝ with h(Q(u)) ≠ 0, and write T(Q) = ω_Q.

  1. Affine h, exactly. If h(y) = ay + b with a ≠ 0 then T(h ∘ Q) = c · T(Q) with c = |a| |Q(u)| / |aQ(u) + b|. Proposition 2.2(3) is the case b = 0, where c = 1.
  2. Lipschitz h, laxly. If h is L-Lipschitz near Q(u) then T(h ∘ Q) ≤ (L |Q(u)| / |h(Q(u))|) · T(Q).
  3. Differentiable h, asymptotically. If h is near Q(u) with h′(Q(u)) ≠ 0 and Q is ‖·‖_A-continuous at u, then ω_{h∘Q}(ε) / ω_Q(ε) → |h′(Q(u))| |Q(u)| / |h(Q(u))| as ε ↓ 0.

Proof. (1) |h(Q(u′)) − h(Q(u))| = |a| |Q(u′) − Q(u)|, and the denominator is the constant |aQ(u) + b|; the ratio is a fixed multiple of e_Q pointwise, so the suprema over the same ball scale by that multiple. (2) replace |a| by the Lipschitz bound. (3) h(Q(u′)) − h(Q(u)) = h′(Q(u))(Q(u′) − Q(u)) + o(|Q(u′) − Q(u)|), uniformly over B_ε because Q(B_ε) → Q(u) by continuity; divide and take suprema. ∎

So T is natural in the quantity of interest: exactly under affine reparameterisation, laxly under Lipschitz, and asymptotically under . This is the T(F(Q)) = Φ(T(Q)) law for post-composition, with Φ multiplication by the relative derivative |h′(Q(u))| |Q(u)| / |h(Q(u))|. The corresponding pre-composition law — Q ∘ G for a map G of the space — is Proposition 2.2(7), and is only lax; exactness there would require the worst directions of G and Q to align, which is the composition slack of §5.1.

Proposition 2.4 (a-priori bound on composition slack). Say Q₁ is c-open at u (0 < c ≤ 1) if for all small ε the image Q₁(B_ε) contains the ‖·‖_B-ball of radius c · ω̂[Q₁](ε) about Q₁u. Then

ω̂[Q₂]( c · ω̂[Q₁](ε) ) ≤ ω̂[Q₂ ∘ Q₁](ε) ≤ ω̂[Q₂]( ω̂[Q₁](ε) ),

so the slack in Proposition 2.2(7) is at most ω̂[Q₂](ω̂₁) / ω̂[Q₂](c·ω̂₁). If ω̂[Q₂] is exactly positively homogeneous of degree one, this ratio is at most 1/c, and the bound can be attained. If instead ω̂[Q₂](η)=κη+o(η) with κ>0, the displayed ratio tends to 1/c as η→0; this is an asymptotic statement, not a finite-scale homogeneous bound.

Proof. The upper bound is Proposition 2.2(7). For the lower, c-openness puts the c·ω̂₁(ε)-ball inside the image, and ω̂[Q₂∘Q₁](ε) is the supremum of Q₂'s displacement over that image, hence at least its supremum over the contained ball, which is ω̂[Q₂](c·ω̂₁(ε)). Exact degree-one homogeneity gives the ratio 1/c. Attainment: Q₁ = diag(1, c) on Euclidean ℝ², with the unit input ball and Q₂ the second coordinate, gives ω̂₁ = 1, ω̂[Q₂∘Q₁] = c, upper bound 1. ∎

Alignment, characterised. The slack is governed by how much the image Q₁(B_ε) fails to fill the ball containing it, in the directions Q₂ is most sensitive to. Tightness is c = 1 along the worst direction of Q₂ — the alignment condition, now a quantity rather than a description. The measured 3.6–4.5× slack corresponds to an effective c ≈ 0.22–0.28 for that pair.

Proposition 2.5 (restriction criterion). Let 𝒟 be the poset of admissible sets ordered by inclusion and 𝒢↑ the poset of non-decreasing transfer guarantees ordered pointwise. Define

R : 𝒟 → 𝒢↑, R(D) = ω_D, Σ : 𝒢↑ → 𝒟, Σ(g) = { u′ ∈ X : e_Q(u′, u) ≤ g(‖u′ − u‖_A) }.

Both are monotone, and for all D ∈ 𝒟, g ∈ 𝒢↑

ω_D ≤ g ⟺ D ⊆ Σ(g).

Equivalently, this relation induces a closure operator on admissible sets. The order-theoretic formulation is recorded for completeness; operationally, the criterion says exactly when a gate-admissible family supports a proposed transfer guarantee.

Proof. (⇒) Let u′ ∈ D and put ε = ‖u′ − u‖_A. Then u′ ∈ D_ε, so e_Q(u′, u) ≤ ω_D(ε) ≤ g(ε), i.e. u′ ∈ Σ(g). (⇐) Fix ε and u′ ∈ D_ε. Then u′ ∈ Σ(g) gives e_Q(u′, u) ≤ g(‖u′ − u‖_A) ≤ g(ε), using that g is non-decreasing; take the supremum over D_ε. Monotonicity of R is Proposition 2.2(9); monotonicity of Σ is immediate. The composite Σ ∘ R is inflationary (D ⊆ Σ(ω_D) by (⇒) with g = ω_D), monotone, and idempotent, hence a closure operator. ∎

Corollary 2.3 (closure-equivalent certification procedures). Σ(ω_D) is the largest admissible set with modulus no greater than ω_D, so replacing D by its closure changes nothing certifiable. Two procedures with the same closure are indistinguishable by any transfer guarantee; the closure is the invariant content of a gate.

Corollary 2.4 (certification in restriction form). |𝓑(τ)| = 0 says ω_D ≤ τ pointwise on the relevant range, which by Proposition 2.5 is D ⊆ Σ(τ) — the accepted set lies inside the τ-tolerant set. Certification is thus an operation on the family of transfer guarantees rather than a separate apparatus: gating moves D down 𝒟, and R carries that motion to a smaller element of 𝒢↑.


2.2 Contribution boundary

The worst-case sensitivity ω(ε) and the distinction between state error and output error are established ideas. Proposition 2.1 and Proposition 2.5 organize that familiar object but are not presented as deep standalone discoveries.

The paper's substantive claims begin at finite tolerance:

  • local conditioning can be finite yet unusable at the accepted tolerance;
  • a certification gate changes the admissible set and therefore the relevant restricted modulus;
  • a searched perturbation family yields the full restricted modulus only under a coverage argument, and otherwise yields a one-sided floor;
  • under effective directional regularity, the restricted modulus can be enclosed with a certified finite computation;
  • Silent Risk summarizes the measure of gate-admitted alternatives that violate a declared decision tolerance.

The remainder of the paper is organized around those claims. The order language is retained only where it shortens proofs or clarifies how gates and pipelines compose.


3. Characterisation

Theorem 3.1 (continuity criterion). ω(ε) → 0 as ε → 0 iff Q is ‖·‖_A-continuous at u.

Proof. (⇒) Given δ > 0, pick ε with ω(ε) ≤ δ. If ‖u′ − u‖_A ≤ ε then the ratio lies in S(ε), so |Q(u′) − Q(u)| ≤ ω(ε)|Q(u)| ≤ δ|Q(u)|: continuity at u. (⇐) Given δ > 0, continuity supplies ε with |Q(u′) − Q(u)| ≤ δ|Q(u)| for all u′ in the ε-ball, so δ is an upper bound for S(ε) and ω(ε) ≤ δ by leastness of the supremum. Since ω is non-decreasing, ω(ε′) ≤ δ for ε′ ≤ ε. ∎

Corollary 3.1 (Lipschitz sufficient condition). If Q is L-Lipschitz in ‖·‖_A near u then ω(ε) ≤ Lε/|Q(u)|, so Q is (ε₀, τ)-certifiable whenever ε₀ ≤ τ|Q(u)|/L.

Proof. Every ratio in S(ε) is at most L‖u′ − u‖_A/|Q(u)| ≤ Lε/|Q(u)|, which is therefore an upper bound; apply leastness. ∎

Lipschitz continuity is sufficient but not necessary: Hölder continuity of order α gives ω(ε) ≤ Cε^α/|Q(u)| → 0, and by Theorem 3.1 bare continuity suffices for the asymptotic statement.

Corollary 3.2 (discontinuity obstruction). If Q is ‖·‖_A-discontinuous at u then ω(ε) ≥ c > 0 for all ε, and Q is (ε₀, τ)-certifiable for no τ < c at any ε₀.

Proof. Contrapositive of Theorem 3.1: if ω(ε) → 0 fails then, ω being non-decreasing, inf_ε ω(ε) = c > 0. Certifiability at τ < c would force ω(ε₀) ≤ τ < c. ∎

Theorem 3.1 is a restatement of continuity and is not itself a contribution; its role is to identify the governing object. It also settles only the limit, and the practical question is finite-ε — a pair can satisfy Theorem 3.1 and be useless at every ε a practitioner would accept, which is what §§4–5 address.

3.1 Differentiability of the fidelity modulus

Fréchet differentiability of Q implies a first-order expansion of ω at zero; the converse need not hold. Its resulting right derivative is a quantity numerical analysis already names. The classical relative condition number is the differential of the fidelity modulus at zero — not an object the theory extends, but the infinitesimal shadow of the more fundamental one.

Theorem 3.2 (differentiability at zero). If Q is Fréchet differentiable at u with respect to ‖·‖_A, then

ω(ε) = κ_rel · ε + o(ε), where κ_rel = ‖DQ(u)‖_* / |Q(u)|,

so ω is right-differentiable at 0 with ω′(0⁺) = κ_rel.

Corollary 3.3 (condition numbers). The classical relative condition number of Q at u is κ = ‖u‖_A · ω′(0⁺). It is therefore a derived quantity: the first-order coefficient of ω, carrying no information ω does not.

Proof. Differentiability gives Q(u′) − Q(u) = DQ(u)[u′ − u] + o(‖u′ − u‖_A). Taking the supremum over the ε-ball, sup |DQ(u)[v]| = ε‖DQ(u)‖_* by homogeneity, and the remainder is o(ε). Divide by |Q(u)|. The stated identity with κ is the definition of the relative condition number, in which the perturbation is measured relative to ‖u‖_A. ∎

Corollary 3.4 (finite-tolerance regimes). Let ε₀ be the operating tolerance and τ the required accuracy.

  • If κ_rel < ∞ and the linearisation is still valid at ε₀, then κ_rel ε₀ ≲ τ certifies — row 1.
  • If κ_rel < ∞ but ε₀ ≫ 1/κ_rel, the condition number exists and is not predictive at the tolerance actually used — row 2.
  • Row 3 implies that no finite condition-number linearisation can certify the quantity. The converse is false.

The converse fails because an infinite or undefined κ_rel does not imply discontinuity. Take Q(x) = 1 + √|x| on at u = 0, where Q(u) = 1: then ω(ε) = √ε → 0, so Q is continuous and asymptotically certifiable by Theorem 3.1, while ω(ε)/ε = ε^{-1/2} → ∞, so no finite first-order condition number exists. Continuous-but-non-Lipschitz transfer is a distinct regime.

So the classification by condition number is four-fold, not three-fold:

regime ω(ε) → 0? κ_rel certifiable?
well-conditioned, in the linear regime yes, ∼ κ_rel ε finite by κ_rel alone
finite κ_rel, outside the linear regime yes finite only by computing ω
continuous but non-Lipschitz yes, sublinearly ∞ or undefined only by computing ω
discontinuous / unidentifiable no never

The third row is the sharpest case for the theory: a classical condition number cannot even classify it correctly — it reports , the same answer it gives for genuine discontinuity — while ω distinguishes the two and certifies the Hölder case at a computable tolerance.

In the reference application. Directional condition numbers along the perturbation family:

ρ 0.9 0.6 0.3 0.1 0.01
κ_rel 4.3e1 3.9e3 2.0e5 2.0e6 4.4e6
1/κ_rel 2.3e-2 2.6e-4 5.1e-6 5.0e-7 2.3e-7
L(5e-3) 3.4e-1 2.0e-2 7.2e-4 8.9e-5 4.5e-5

sup_ρ κ_rel ≈ 4.4 × 10⁶, so the linear regime extends only to ε ≲ 2.3 × 10⁻⁷ — and the acceptance floor of 5 × 10⁻³ sits four orders of magnitude beyond it. The pair is row 2 by Corollary 3.4, and the condition number, though finite, is inapplicable by a factor of 2.2 × 10⁴ at the tolerance in use. Computed by transfermod.modulus.condition_number and linearity_ratio.

The quantity a practitioner needs from second order is not the coefficient but the scale at which first-order reasoning stops applying. Define the crossover

ε_× = κ_rel / |κ₂|,

where κ₂ is the second-order coefficient below. For ε ≪ ε_× the linearisation of Theorem 3.2 governs; for ε ≫ ε_× it does not, and ω must be computed. The expansion exists to justify and compute ε_×.

Why this is not stated as the primary asymptotic result, with Theorem 3.2 as its corollary: Theorem 3.3 needs twice-differentiability and a unique non-degenerate first-order maximiser, strictly more than Theorem 3.2, which needs only Fréchet differentiability. Deriving Theorem 3.2 from it would import hypotheses it does not require.

Theorem 3.3 (second-order expansion, full modulus). Suppose Q is twice Fréchet differentiable at u and the first-order maximiser v* of |DQ(u)[v]| over the unit sphere is unique up to sign and non-degenerate. Write κ_rel = ‖DQ(u)‖_*/|Q(u)| and β = D²Q(u)[v*, v*] / (2|Q(u)|). Then

ω(ε) = κ_rel ε + |β| ε² + o(ε²).

Proof qualification. The displayed expansion is immediate along the two rays ±v*. Equality with the full supremum additionally requires a smooth constrained maximum: the unit sphere must be smooth near ±v*, the first-order maximum must be isolated with a negative-definite tangential Hessian, and the Taylor remainder must be uniform on the unit sphere. Under those conditions the maximizing direction varies smoothly by O(ε) and the envelope expansion gives the stated coefficient. In a general normed space, or without this isolation condition, the ray calculation remains a lower bound and the theorem should not be invoked. ∎

The second-order coefficient of the full modulus is therefore non-negative in the scalar case: symmetry of the ball forecloses cancellation. A signed quadratic coefficient is a property of a one-sided family, not of ω.

Proposition 3.1 (second-order expansion, one-sided ray). (Not a consequence of Theorems A–B: those describe how ω behaves under operations and restriction, and carry no asymptotic content. This needs twice-differentiability along the ray.) For a fixed parameterised ray u_w, w ≥ 0, with Q twice differentiable along it,

ω_θ(ε) = κ_θ ε + κ_{2,θ} ε² + o(ε²),

and κ_{2,θ} may have either sign, since only w ≥ 0 is admissible. The crossover scale is ε_×^θ = κ_θ / |κ_{2,θ}|, and L_θ(ε) = 1 + (κ_{2,θ}/κ_θ)ε + o(ε).

Corollary 3.5 (where first-order conditioning stops working). Row 2 of the trichotomy is, quantitatively, κ_rel < ∞ and ε₀ ≫ ε_×; row 1 is ε₀ ≪ ε_× with κ_rel ε₀ ≤ τ.

Measured — for the ray-restricted modulus ω_θ, not for ω. Fitting ω_θ(ε) = aε + bε² on each ray, and locating the half-linearity point L_θ(ε) = ½ independently by bisection:

| ρ | κ_θ = a | κ_{2,θ} = b | ε_×^θ = a/|b| | L_θ = ½ at | ratio | |---|---|---|---|---|---| | 0.9 | 4.33e1 | −1.74e4 | 2.49e-3 | 2.54e-3 | 1.02 | | 0.6 | 3.85e3 | −5.28e7 | 7.30e-5 | 8.40e-5 | 1.15 | | 0.3 | 1.95e5 | −1.18e11 | 1.66e-6 | 2.07e-6 | 1.25 |

ε_×^θ predicts where the linearisation half-fails to within 25%, across three decades of conditioning. b < 0 on every ray, which is a statement about the one-sided family: the relative error saturates near 1 while the linear extrapolation does not, so along these rays first-order conditioning over-predicts — κ_θ ε₀ = 2.2 × 10⁴ against a true ω_θ(ε₀) = 0.95. By Theorem 3.3 the corresponding full-modulus coefficient is +|β|, so no such conservatism can be inferred for ω itself.

Computed by transfermod.modulus.second_order, which fits the ray expansion.

4. Restricted moduli

Let D ⊆ X be the certified set, defined by the procedure alone and not by ε, and put D_ε = D ∩ B_ε(u). With e_Q(u′,u) = |Q(u′) − Q(u)|/|Q(u)|,

ω_D(ε) = sup{ e_Q(u′, u) : u′ ∈ D_ε } ≤ ω(ε).

Restriction is monotone in the admissible set. If D ⊆ D′ then ω_D(ε) ≤ ω_{D′}(ε) for every ε, since the supremum is over a subset; taking D′ = X recovers ω_D ≤ ω. So D ↦ ω_D is an order-preserving map from the poset of admissible sets to the poset of transfer guarantees, and certification acts on ω by restriction along the inclusion D ↪ X rather than by replacing it.

Over a parameterised family, ω_{D,Θ}(ε) = sup{ e_Q(u_θ, u) : u_θ ∈ D_ε }. Every computed number below is a ω_{D,Θ} — exact for the family, a lower bound for ω_D — and no family is claimed extremal over D_ε.

Along a perturbation family u_w, w ≥ 0, with u_0 = u, write

A = { w : u_w ∈ D } (accepted), C(τ) = { w : |Q(u_w) − Q(u)| > τ|Q(u)| } (τ-corrupt),

and define w_det = sup A, w_corrupt(τ) = inf C(τ) (with the conventions sup ∅ = 0, inf ∅ = ∞). Defining the thresholds as a supremum and an infimum rather than as least elements avoids any question of whether the sets are open or closed at their endpoints. The log-amplitude Silent Risk is |𝓑(τ)| = log₁₀(w_det/w_corrupt(τ))⁺; the exposure is |𝓘| = log₁₀(w_agg/w_det)⁺, where w_agg = sup{ w : ‖u_w − u‖_A ≤ ε }.

4.1 Measure-qualified Silent Risk

For a general measure ν on alternatives and tolerance τ, let B_τ={x:x is admitted and ℓ(Q(x),Q₀)>τ}. Define

SR_{ν,τ}=ν(B_τ).

This is the umbrella definition of Silent Risk: the measure of admitted decision-corrupting alternatives. The one-parameter spectral construction uses logarithmic amplitude measure and reports a width in decades. A Bayesian construction may use posterior measure and report an exceedance probability. The measure must always be named.

5. Certification

Theorem 5.1 (family-restricted certification). For an arbitrary family {u_θ}_{θ∈Θ}, with A = {θ : u_θ ∈ D} and C(τ) = {θ : |Q(u_θ) − Q(u)| > τ|Q(u)|},

ω_{D,Θ} ≤ τA ∩ C(τ) = ∅.

Proof. ω_{D,Θ} is the supremum of the relative error over the accepted parameters A. It exceeds τ iff some θ∈A has relative error above τ, which is equivalent to A∩C(τ)≠∅. Negate. ∎

Coverage corollary. If condition (C1) proves that the family covers D, then ω_{D,Θ}=ω_D, and the same equivalence holds for the full restricted modulus.

Theorem 5.2 (scalar Silent Risk criterion). Suppose w ↦ |Q(u_w) − Q(u)| is continuous and non-decreasing, and the detection statistic is non-decreasing. Then |𝓑(τ)| = 0 ⟺ ω_{D,Θ} ≤ τ. Under (C1), this is also equivalent to ω_D≤τ.

Proof. Monotonicity of the detection statistic makes A a down-set in [0,∞): if w′ < w and u_w is accepted, so is u_{w′}. Monotonicity and continuity of the error make C(τ) = {w : error(w) > τ|Q(u)|} a relatively open up-set, so C(τ) = (w_corrupt(τ), ∞) and w_corrupt(τ) ∉ C(τ). Hence A ∩ C(τ) = ∅ iff A ⊆ [0, w_corrupt(τ)] iff w_det = sup A ≤ w_corrupt(τ), which is log₁₀(w_det/w_corrupt(τ)) ≤ 0, i.e. |𝓑(τ)| = 0. Apply Theorem 5.1. ∎

The continuity hypothesis is not removable. Without it the boundary case defeats the equivalence: if A = [0,1] and C(τ) = [1,∞) then w_det = w_corrupt(τ) = 1, so |𝓑(τ)| = 0, yet u_1 is accepted and τ-corrupt, so ω_D > τ. Monotonicity alone gives only A ∩ C(τ) = ∅ ⟹ w_det ≤ w_corrupt(τ) and the strict converse w_det < w_corrupt(τ) ⟹ A ∩ C(τ) = ∅. Every family computed in this note is analytic in w, so the hypothesis costs nothing there; it is stated because the scalar summary, not the equivalence of Theorem 5.1, is what needs it.

Theorem 5.1 shows the equivalence is set-theoretic; monotonicity enters only to make A and C(τ) intervals, so that disjointness collapses to a comparison of two numbers and the discrepancy to the single quantity |𝓑(τ)|. Monotonicity is therefore a hypothesis on the computable scalar summary, not on the result. This is the note's central claim: a certification procedure computes a family-restricted modulus; it computes the full restricted modulus only when coverage is proved. Without monotonicity only ω_{D,Θ} ≤ τ ⟹ |𝓑(τ)| = 0 survives, A need not be an interval.

Corollary 5.1 (limits of gating). If |Q(u_w) − Q(u)| ≥ c|Q(u)| for all w > 0, then any D with w_det > 0 has ω_D ≥ c.

Proof. Let c′ < c and take the constant guarantee g ≡ c′. By hypothesis no u_w with w > 0 lies in Σ(c′). Since w_det > 0, D contains such a u_w, so D ⊄ Σ(c′), and Proposition 2.5 gives ω_D > c′. Let c′ ↑ c. ∎

Gating therefore helps in the continuous but ill-conditioned regime, not the discontinuous one.

Trichotomy. Lipschitz with modest L → refinement certifies, gating unnecessary. Continuous with poor modulus → refinement fails at usable ε, gating certifies. Discontinuous → neither. The contribution lies in the middle row.

Composition, in brief. For a map F : (X, ‖·‖_A) → (X₂, ‖·‖_B) write the absolute modulus ω̂[F](ε) = sup{ ‖F(u′) − F(u)‖_B : ‖u′ − u‖_A ≤ ε }, so that the relative modulus of Definition 2.2 is ω = ω̂/|Q(u)|. Proposition 2.2(7) bounds ω̂[Q₂ ∘ Q₁] by ω̂₂ ∘ ω̂₁, and Proposition 2.4 bounds the slack of that bound by 1/c for a c-open upstream map. Consequences: pipelines compose multiplicatively, so a single flat-modulus stage caps the chain; stage-wise gating bounds what end-to-end validation does not, though the measured 3.6–4.5× slack means it bounds rather than budgets; and composition preserves validity but not minimality — the slack is well defined precisely because Proposition 2.1 pins the target.

6. Computation

ω is a supremum over an infinite-dimensional ball. Two reductions: restrict to a perturbation family (a lower bound, exact for the family); and, under monotonicity, locate each threshold by bisection in O(log 1/δ) evaluations. R = (|𝓘|, |𝓑|) costs three bisections plus one — measured, 180 evaluations and 20 ms at the reference point.

6.1 Sufficient conditions for computing a restricted modulus

ω_D(ε) is a supremum over an infinite-dimensional set, and §6 so far has only produced ω_{D,Θ}, a lower bound. This subsection gives conditions under which the gap closes and the computation is certified.

Let the admissible perturbations be parameterised as u_{d,w} with direction d ∈ S and amplitude w ≥ 0, u_{d,0} = u.

Theorem 6.1 (attainment and conditional effective computation). Assume

  • (C1) Coverage. Every u′ ∈ D_ε equals u_{d,w} for some (d,w)∈S×[0,∞).
  • (C2) Ray regularity. For each fixed d, the error, aggregate, and detection statistics are non-decreasing in w, and the error is continuous.
  • (C3) Directional regularity. S is compact and d↦ω_D^{(d)}(ε) is continuous.

Then the full restricted modulus is attained:

ω_D(ε)=max_{d∈S}ω_D^{(d)}(ε).

Compactness and continuity prove existence, not by themselves an effective finite algorithm. For certified computation to a requested tolerance, additionally assume:

  • (C4) Effective directional control. A finite δ-net of S can be constructed and a known modulus of continuity μ satisfies |ω_D^{(d)}-ω_D^{(g)}|≤μ(dist(d,g)).

Then for any δ-net G⊂S,

max_{g∈G}ω_D^{(g)}(ε) ≤ ω_D(ε) ≤ max_{g∈G}ω_D^{(g)}(ε)+μ(δ).

In the Lipschitz special case μ(r)=Λr, this recovers the implemented Λδ bound. If ray thresholds are computable by certified bisection to error δ′, the total cost is |G|·O(log(1/δ′)) ray evaluations.

Proof. (C1) permits decomposition of the supremum by directions. (C2) reduces each ray value to a threshold search. (C3) gives attainment of the outer supremum by the extreme-value theorem. Under (C4), choose for each d∈S a g∈G with dist(d,g)≤δ; then ω_D^{(d)}≤ω_D^{(g)}+μ(δ)≤max_G+μ(δ). The grid lower bound is immediate. The complexity statement follows from the certified ray solver. ∎

Corollary 6.1 (coverage is the remaining structural obstruction). Under (C2)–(C4), everything except (C1) is a finite computation with a certified error bound. Coverage is the remaining structural obstruction once ray regularity, effective compactness, and a certified continuity modulus have been supplied; none of those computational hypotheses is free. What distinguishes coverage is that no computation can verify it: it is a claim that the chosen family exhausts what the certification procedure will accept. Absent a proof of (C1), every reported value is a lower bound on ω_D — which is why the quantities in this document are written ω_{D,Θ}.

Λ is likewise not free: estimating it from the largest slope between adjacent grid nodes is plausible but not certified, and a certified upper bound requires an a priori smoothness bound on the family. transfermod.modulus.certified_grid_max returns (lower, upper, Λ) and documents which of these is which.

In the reference application. Directions are indexed by ρ, and ω_D^{(ρ)}(5e-3) is Lipschitz with estimated Λ ≈ 0.149:

grid spacing δ nodes lower upper = lower + Λδ
0.200 5 0.023538 0.053310
0.100 10 0.023538 0.038424
0.050 19 0.023538 0.030981
0.010 95 0.023538 0.025027

Every bracket contains the fine-grid value, and the interval tightens as Λδ. One caveat visible here: ω_D^{(ρ)} increases as ρ ↓ 0 and saturates — 0.023407 at ρ=0.2, 0.023553 at 0.02, 0.023561 at 0.002 — so the direction set (0,1) is not compact and the supremum is attained only in the limit. (C3) holds on the compactification [0,1], where the limit exists; the reported 0.0235 is the value there. That is a concrete instance of why compactness is a hypothesis and not a formality.

7. Reference application: numerically diagonalised finite-cutoff compact U(1) spectral inference

7.1 Setup

X = spectral decompositions of a two-point response; ‖·‖_A = signal-normalised correlator residual with equal-time moments; Q = extremal decay rate (a mass gap). The target is the reference application throughout — 2+1D compact U(1) Kogut–Susskind gauge theory on a small periodic lattice with a hard-wall-truncated electric basis, solved by full floating-point diagonalisation of the selected Gauss-law basis block. Thus Q is a finite-matrix eigenvalue difference with no Monte Carlo sampling error, but it remains sector-, volume-, cutoff-, and channel-dependent. Correlators follow from C(t) = Σ_n |⟨0|O_c|n⟩|² e^{−(E_n−E_0)t}. Reference diagnostics check the all-sector strong-coupling gap (→g² on the 2×2 torus), the zero-winding plaquette-sector gap (→2g²), gauge invariance, Hermiticity, winding-block preservation, full-versus-sector channel agreement, and cutoff-boundary occupation.

w_corrupt(τ) is the least fabricated amplitude shifting the estimated Q by more than τ.

7.2 The perturbation family

(formerly "Confound construction" — unchanged, now realising §4's u_w)

The family fabricates a single faint slow mode at rate ρ·Δ (ρ < 1) carrying a fraction w of the operator variance, renormalising the true weights so C(0) is preserved exactly. Being slowest it dominates the long-time tail and biases the effective-mass plateau downward, while its contribution stays below the aggregate error floor over the measured window. Physically: a fabricated long-range correlation — a spurious near-zero eigenvalue in a reduced operator, or a slow autocorrelation mode in a sampler.

The alternative direction is structurally constrained: a surrogate matching the reference on the window to precision ε cannot bias the leading rate upward freely, since window data bound the slowest rate from below. Upward bias requires a genuine light state with small operator overlap — the unsmeared-operator regime — supplied as a secondary mechanism.

Proposition 7.1 (constructibility of faint slow modes). (Realisation-specific: an existence statement about one perturbation family, not a structural result.) Let the reference have spectral representation C(t) = Σ_n w_n e^{−Δ_n t} with w_n > 0, total weight W ∈ (0,∞) and slowest rate Δ. Fix a bounded window [0, t_max], an aggregate tolerance ε > 0 and 0 < ρ < 1. Adding a mode at rate ρΔ with weight wW and rescaling the original weights by (1 − w) — so C_w(0) = C(0) exactly — there exists w > 0 with ‖C_w − C‖_A ≤ ε while the asymptotic rate of C_w equals ρΔ.

Proof. The asymptotic rate is ρΔ for every w > 0, the added mode being strictly slowest with positive weight. And C_w − C = w(W e^{−ρΔ·} − C) is linear in w on the bounded window, so ‖C_w − C‖_A = w‖W e^{−ρΔ·} − C‖_A → 0; take w ≤ ε/‖W e^{−ρΔ·} − C‖_A. ∎

The window bound is load-bearing: over [0,∞) the aggregate discrepancy no longer vanishes with w uniformly, which is the same fact as ω growing with t_max.

7.2.1 Adversarial interpretation

Proposition 7.1 can be written as an adversarial optimization problem. For an admissible family

$$D_\varepsilon(u)=\{u' : \|u'-u\|_A\le\varepsilon\},$$

the constructed slow mode seeks a member of (D_\varepsilon(u)) that maximizes the declared downstream discrepancy. This is mathematically parallel to the robust-optimization view of adversarial examples: a perturbation remains small in the validation geometry while producing a large change after the downstream map. The scientific distinction is that the perturbation is a surrogate model or spectral measure and the target is a derived physical conclusion.

The connection supplies useful language and algorithms—inner maximization, attack families, certified radii, and robust training—but does not identify the two problems. Scientific admissibility is set by a validation contract, and the quantity of interest may be asymptotic, operator-valued, or physically constrained in ways absent from standard input-space attacks.

7.3 Where the pair sits

Finite-window Q is ‖·‖_A-continuous (row 2 of the trichotomy, by the w → 0 table), so Theorem 3.1 gives certifiability at some tolerance. The modulus says at which:

ε 5e-3 1e-4 1e-6 1e-8
ω(ε) 0.950 0.928 0.497 0.030

At the acceptance floor Q is essentially unconstrained; (ε₀, 3%)-certifiability needs ε₀ ~ 1e-8, five orders tighter. Gating restores control, flat in ε as Theorem 5.2 predicts: ω_D = 0.0235 at every ε above, matching the independently computed family threshold τ* = 2.36% below which silent risk becomes positive. Taking Q as the true t → ∞ rate instead puts the same system and seminorm in row 3: Q(u_w) = ρQ(u) for every w > 0, discontinuous, and ω_D = 0.950 — uncertifiable by Corollary 3.2 and unrescued by Corollary 5.1.

7.4 The certified set, and results

(formerly "Benchmark design", "Gate", "Pilot result", "Robustness")

D is defined by a preregistered gate with conventional tests (equal-time expectation and variance; signal-normalised aggregate RMSE) and spectral tests (channel-gap error; effective-mass plateau; relative tail-decay error; leading-overlap alignment), thresholds frozen before interpretation. D was fixed before ω was defined, which is why the agreement in §7.3 between ω_D and τ* is evidence rather than construction.

The gate evaluates outputs, not architectures: the contract is correlator(ts), variance(), metadata(), with optional provenance() and training_info(); models with an explicit spectral decomposition supply spectral() and inherit the rest. Four families are implemented, one representative each, because each fails for a different structural reason: (I) numerical — exact diagonalisation and Krylov/Lanczos, the trust anchor, required to agree with the reference to machine precision (gap 8.9e-16, correlator 1.4e-15); (II) reduced — POD/Galerkin and reduced transfer operators, where subspace truncation and Rayleigh–Ritz bias the extremal spectrum; (III) learned — a VMC-trained neural quantum state and a fitted multi-exponential model, where aggregate loss is blind to low-signal modes; (IV) constructed — the positive control, without which sensitivity would be untested. Confidence originates in Class I and transfers downward.

Pilot. The honest reduced-transfer surrogate and an echo control are certified (no false positive). The constructed control passes every conventional test — identical equal-time variance, aggregate RMSE 2.6e-3 below a 5e-3 floor — and fails the spectral tests, reporting Q ~40% below truth. Stable across a coupling and truncation sweep.

Reachable from ordinary practice. A POD/Krylov–Galerkin reduction exhibits the failure with no adversarial design. Krylov moment matching reproduces equal-time and short-time data essentially exactly, so conventional checks cannot fail; Rayleigh–Ritz converges from above, so an under-resolved reduction over-estimates systematically and single-signed. Ranks 2–5 are confounds (gap error 3–33%, C(0) error ≲ 2e-15); rank ≥ 6 is certified. At ranks 4–5 the gap error is inside tolerance and the tail test alone drives the verdict — long-time fidelity is the leading indicator.

Cross-estimator robustness. Effective-mass plateau, single- and multi-exponential fits, Prony/linear-prediction reconstruction, and AIC model averaging all recover the reference Q on clean data and are biased identically by the constructed perturbation, because each reads the same corrupted tail. These are distinct functionals of a shared correlator information basis: their agreement shows that the failure is not estimator-specific, but it is not independent corroboration. A variational operator basis catches single-channel confounds as cross-channel inconsistency, but not those applied consistently across channels, which still require the reference.

Information bases of gates. A gate result can be labelled by the measured information on which it depends. Formally, let G be the set of gate tests and let b : G → 𝓘 map each test to an information-basis label. Then gate diversity |{g₁,…,gₘ}| and information-basis diversity |{b(g₁),…,b(gₘ)}| are distinct quantities. The map b is metadata for interpreting a certification report; it does not enter the restricted-modulus theorems and does not assert statistical independence. In the implementation the labels distinguish equal-time observables, an aggregate correlator window, a long-distance correlator tail, and an explicit spectral decomposition.

Stability. R converges under truncation refinement as Q does (Λ = 1,2,3,4 → |𝓘| = 3.18, 2.92, 2.92, 2.92) and moves with the physics, so it characterises the inference problem rather than the discretisation.

7.5 A non-physics instance: graph sparsification

The transfer construction is not specific to spectral physics. The executable graph instance in scripts/run_graph_instance.py takes:

  • (X): weighted graphs on a fixed vertex set;
  • (|\cdot|_A): relative Frobenius error of the graph Laplacian;
  • (Q): algebraic connectivity, the Fiedler value (\lambda_2).

A perturbation weakens inter-cluster bridge edges while conserving total edge weight. Aggregate Laplacian error remains small, yet (\lambda_2)—and therefore conclusions about mixing, robustness, and clustering—can change substantially. The instance reproduces the same logical pattern as the spectral example:

small aggregate approximation error
        does not imply
small error in a structurally sensitive derived quantity.

This second domain is intentionally compact rather than a full graph-theoretic case study. Its role is to demonstrate that the fidelity-modulus construction depends on an admissible set, a quantity of interest, and a discrepancy geometry—not on the physics of correlator tails.

Coverage tiers and one-sided interpretation

A computed family-restricted value has one of three epistemic statuses:

  1. Proven exact: (C1) is proved and (\omega_{D,\Theta}=\omega_D).
  2. Certified adversarial floor: the family supremum is valid but coverage is unproved, so (\omega_{D,\Theta}\le\omega_D).
  3. Exploratory sample: even the family supremum has not been established.

The one-sided interpretation is essential:

Large floors condemn; small floors do not acquit.

A large certified floor proves substantial exposure. A small floor cannot rule out an unsearched confound and therefore must not be described as a negative result or a safety certificate.

Agreement among several perturbation families is useful robustness evidence, but it does not prove (C1); distinct families may share the same blind spot.

Exact coverage in structured families

The coverage condition (C1) is generally substantive, but it can be proved in important structured settings.

Theorem — continuous linear functional over a Hilbert ball

Let (H) be a real Hilbert space, let (D_\varepsilon(u)={u+h:|h|_H\le\varepsilon}), and let (Q) be continuous and linear with Riesz representer (q). Then

$$\sup_{\|h\|_H\le\varepsilon}|Q(u+h)-Q(u)| = \varepsilon\|q\|_H,$$

attained by (h=\pm\varepsilon q/|q|_H) when (q\neq0).

For a nonlinear (Q), the representer of (DQ(u)) gives only a local first-order adversarial direction unless stronger global assumptions are proved.

Theorem — ellipsoidal linear coverage and seminorm kernels

Let (M\succeq0), let (D_\varepsilon={h:h^\top Mh\le\varepsilon^2}), and let (Q(h)=q^\top h). If (q) has a nonzero component in (\ker M), then the modulus is infinite. Otherwise,

$$\omega(\varepsilon) = \varepsilon\sqrt{q^\top M^\dagger q}.$$

This theorem makes the seminorm-kernel warning exact: an uncontrolled quantity direction is not merely numerically unstable; it is unbounded under the stated validation contract.

Corollary — sketch-nullspace coverage

Under (Ph=0) and (|h|_2\le\varepsilon),

$$\sup |\langle q,h\rangle| = \varepsilon\|\Pi_{\ker P}q\|_2.$$

The projected query direction is the exact extremizer.

Theorem — leading eigenvalue under Frobenius perturbations

For symmetric (A) and unrestricted symmetric (\Delta) satisfying (|\Delta|_F\le\varepsilon),

$$\sup_\Delta \left[ \lambda_{\max}(A+\Delta)-\lambda_{\max}(A) \right] = \varepsilon.$$

A rank-one perturbation (\Delta=\varepsilon vv^\top), with (v) a leading eigenvector, attains the bound. This statement does not automatically extend to spectral gaps, Fiedler values, trace-constrained density matrices, or physically constrained Laplacian perturbations.

Known tensions

Four limitations are structural rather than incidental. They are stated here together because each qualifies a headline number elsewhere in the document.

1. Coverage is unproved, so the spectral-family values are ω_{D,Θ} lower bounds. Corollary 6.1 is exact about this: without a proof that the single-mode family exhausts the certified set, what is computed is ω_{D,Θ}. The quantitative claims — the 40× gating reduction, ω_{D,Θ} = 0.0235, the |𝓑| = 0 certification below τ* = 2.36% — are therefore family-dependent. A richer family could only raise ω_D, never lower it, so the direction of the error is known; its size is not.

2. The linear regime is narrow enough that first-order analysis is useless where the theory operates. κ_rel ≈ 4 × 10⁶ and the linearisation holds only for ε ≲ 2 × 10⁻⁷, against a 5 × 10⁻³ acceptance floor — four orders of magnitude out. This is the case for computing the modulus rather than quoting a condition number, but it also means the interesting regime is exactly the one where classical first-order reasoning has already stopped applying. Row 2 is not an edge case of the classical theory; it is outside it.

3. The composition slack is bounded but still too large for a stage-wise error budget. The slack is now controlled a priori by the openness constant of the upstream map (slack ≤ 1/c in the homogeneous case), but c must be estimated, and the measured 3.6–4.5× gap between ω̂₂ ∘ ω̂₁ and the true composite means stage-wise gating bounds a pipeline but does not yet budget one: a four-stage chain could inherit two orders of magnitude of slack. Estimating c without solving the composite problem (open question 4) is the highest-leverage theoretical follow-up here. A natural refinement is to characterize intermediate maps that are contractive in the relevant validation and decision geometries. If one stage strictly contracts admissible perturbations, the composite bound should inherit less slack than the general openness estimate; the exact improvement depends on how contraction interacts with the declared discrepancies at the two stages.

4. The verdict depends on how the quantity of interest is read. The same system is row 2 for a finite-window estimator and row 3 for the true t → ∞ rate, so the practical claim is sensitive to the choice of estimator. The cross-estimator robustness checks (plateau, exponential fits, Prony, AIC averaging, all biased identically) mitigate this but do not remove it: they show that several extraction algorithms applied to the same correlator tail agree, not that the tail supplies independent evidence or that a finite window is the right reading.

8. Scope

Demonstrated on a finite-volume, finite-cutoff system with numerically diagonalised reference matrices; this establishes a detectable failure mode and a non-false-positive gate, not any continuum or Yang–Mills statement. ω is computed over a single-mode family, hence a lower bound on the modulus over all perturbations. Certification is a threshold test, not a validated bound.

9. Open questions

A finite-ε refinement of Theorem 3.1 (the row-1/row-2 boundary); estimating ω without a reference of known Q; the cost of estimating ω_D in general; tightness of Proposition 2.2(7) beyond the openness bound of the slack proposition — estimating c without solving the composite problem, and the non-homogeneous case; whether contractive intermediate maps yield a strictly sharper composition calculus than the current openness bound; whether the tensor-product subadditivity of log(1 + ω) reflects a deeper information-geometric or resource-additive structure, or is only the algebraic linearization of a multiplicative error bound; what replaces Corollary 3.1 for order-type discrepancies; making ω_D a construction objective, stage-wise per Proposition 2.2(7); and whether sketching or sparsification supplies a practically interesting row-2 pair.

The operator viewpoint. Proposition 2.2 is really a theorem about the transfer operator T : Q ↦ ω_Q rather than about any single modulus. Identifying the class of maps T preserves, and whether T is determined by its behaviour on a generating family of quantities, would make the theory more compact than it is here — where T appears as an organising device rather than an object of study. That is the direction in which the structural layer would next be strengthened, and it generates its own questions: which transformations preserve T, which contract it, what the complexity of evaluating T is on different classes of quantities, and whether T admits an axiomatic characterisation (below).

An axiomatization theorem? With 𝒢 given by Definition 2.1, the question is trivial: Proposition 2.1 says T(Q) is the least element of 𝒢(Q), which is unique, so T is already determined. The interesting version drops 𝒢. Start instead from an abstract assignment T : Q ↦ g_Q into non-decreasing functions, required only to satisfy the structural axioms — a decomposition property, the calculus of Proposition 2.2, an adjunction with restriction, and naturality under reparameterisation — with no reference to the defining supremum. Is T then unique? An affirmative answer would be an axiomatization theorem: it would characterise the fidelity modulus by its behaviour rather than by its construction, so that any operator satisfying the least-guarantee property, the basic calculus, restriction–saturation relation and reparameterisation behavior is necessarily T. A negative answer would exhibit a second, inequivalent transfer calculus, which would be at least as interesting.

Empirical extensions required for external validation

The mathematical results above do not by themselves establish that the framework is effective across contemporary surrogate-model pipelines. Three classes of experiments remain especially important.

Learned operators and trained neural surrogates

Constructed confounds establish possibility and, in some settings, exact worst cases. Learned-operator experiments address a different empirical question: whether aggregate and decision error actually decouple in trained surrogates that were not designed to exhibit the phenomenon.

The first trained-model audit in this repository is negative. A random-feature diffusion operator passes its ordinary smooth-distribution validation, but every member of the frozen localized challenge family has relative global L2 error far above the declared aggregate threshold. The largest decision error rises with conspicuous aggregate error; no point enters the predeclared small-aggregate/large-decision region. The instance therefore demonstrates proportionate out-of-distribution degradation, not a failure hidden from aggregate validation.

This distinction is substantive. Passing an in-distribution validation set does not make a later out-of-distribution error “silent” when the same aggregate metric detects that error on the challenged input. The empirical object is the joint aggregate–decision profile, not the fact that the model once passed a different sample.

External validation must therefore test discovery rather than constructibility. The confirmatory protocol in LEARNED_OPERATOR_PROTOCOL.md freezes external checkpoints, metrics, quantities, thresholds, families, budgets, and reporting rules before evaluation. Coupled and null profiles are first-class outcomes; a negative result must not be replaced post hoc by a newly designed successful family.

Computational scaling in higher-dimensional PDEs

The finite-grid procedure of Theorem 6.1 is transparent, but its cost grows with the dimension and resolution of the perturbation parameterization. Large-scale two- and three-dimensional PDE instances should therefore report complexity empirically: objective evaluations, admissibility evaluations, convergence of the supremum estimate, and benefits from adaptive search or adjoint-informed directions.

This is a question about the practical attainability of the restricted supremum, not the validity of the theorem.

Posterior-measure Silent Risk

The measure-qualified definition permits a posterior measure (\Pi(\mathrm d u\mid Y)). In that case Silent Risk is the posterior mass of admissible alternatives whose decision discrepancy exceeds a declared tolerance:

$$\mathrm{SR}_{\Pi,\tau} = \Pi\!\left( \ell(Q(u),Q_0)>\tau \mid Y \right).$$

A Bayesian instance should keep three objects distinct:

  1. the posterior law constructing or weighting the admissible family;
  2. the decision discrepancy (\ell);
  3. the transfer functional (Q).

The experiment should be compared against posterior summaries that can conceal decision instability, including plug-in estimates and parameter-level credible intervals.

Version 1.2.2 includes compact executable validations for each track (numerical results: VALIDATION_REPORT.md). Their outcomes are mixed: the learned-operator instance is negative for decoupling, the PDE study addresses only compact-grid feasibility, and the Bayesian study validates software separation of probabilistic and decision-level quantities. None replaces an external pretrained-operator, solver-coupled 3D, or non-conjugate Bayesian study.

Spectral-gap API migration

exact_gap is deprecated and will be removed in TransferMod 2.0. It is a warning-emitting compatibility alias for sector_gap, not a separate global quantity. New code should use:

Legacy name Canonical replacement
exact_gap sector_gap
global_physical_gap when the full all-sector basis is available
spectrum_scope and basis_mode to state interpretation

References

Becker, R., and Rannacher, R. (2001). “An Optimal Control Approach to A Posteriori Error Estimation in Finite Element Methods.” Acta Numerica 10:1–102. doi:10.1017/S0962492901000010.

Bertsimas, D., and Sim, M. (2004). “The Price of Robustness.” Operations Research 52(1):35–53.

Goodfellow, I. J., Shlens, J., and Szegedy, C. (2014). “Explaining and Harnessing Adversarial Examples.” arXiv:1412.6572.

Higham, N. J. (2002). Accuracy and Stability of Numerical Algorithms, 2nd ed. SIAM.

Madry, A., Makelov, A., Schmidt, L., Tsipras, D., and Vladu, A. (2017). “Towards Deep Learning Models Resistant to Adversarial Attacks.” arXiv:1706.06083.

Oden, J. T., and Prudhomme, S. (2001). “Goal-Oriented Error Estimation and Adaptivity for the Finite Element Method.” Computers & Mathematics with Applications 41(5–6):735–756. doi:10.1016/S0898-1221(00)00317-5.

Oden, J. T., and Prudhomme, S. (2002). “Estimation of Modeling Error in Computational Mechanics.” Journal of Computational Physics 182(2):496–515. doi:10.1006/jcph.2002.7183.

Owhadi, H., Scovel, C., Sullivan, T. J., McKerns, M., and Ortiz, M. (2013). “Optimal Uncertainty Quantification.” SIAM Review 55(2):271–345. doi:10.1137/10080782X.

Patera, A. T., and Rozza, G. (2007). Reduced Basis Approximation and A Posteriori Error Estimation for Parametrized Partial Differential Equations. MIT Pappalardo Graduate Monographs in Mechanical Engineering.

Prudhomme, S., and Oden, J. T. (1999). “On Goal-Oriented Error Estimation for Elliptic Problems: Application to the Control of Pointwise Errors.” Computer Methods in Applied Mechanics and Engineering 176:313–331. doi:10.1016/S0045-7825(98)00343-0.

Rozza, G., Huynh, D. B. P., and Patera, A. T. (2008). “Reduced Basis Approximation and A Posteriori Error Estimation for Affinely Parametrized Elliptic Coercive Partial Differential Equations.” Archives of Computational Methods in Engineering 15(3):229–275. doi:10.1007/s11831-008-9019-9.

Smith, R. C. (2013). Uncertainty Quantification: Theory, Implementation, and Applications. SIAM.

Appendix A. Extensions

A.0 Why a minimum exists

The ambient poset [0,∞]^{(0,∞)} under the pointwise order is a complete lattice, [0,∞] being one and products of complete lattices being complete. 𝒢 is upward closed (weakening a valid guarantee keeps it valid) and closed under arbitrary pointwise infima (an infimum of upper bounds of S(ε) is an upper bound of S(ε)), hence is a principal up-set generated by its own infimum. Existence is therefore structural rather than incidental; uniqueness is trivial; the content of Proposition 2.1 is that this abstractly guaranteed infimum is ω, and is attained — so 𝒢 has a least element, not merely a greatest lower bound.

A.1 Further extensions

Arbitrary discrepancies on Q (spectral, order-type, Hausdorff — covering operator-valued Q) and arbitrary divergences on X (Bregman, KL, quantile): Definitions 1–2, Proposition 2.1, Theorem 6.1 hold verbatim; Theorem 3.1 needs d(u,u) = 0 and a convergence notion. Locality and uniform classes; vector-valued and Banach-valued codomains; multi-parameter families by ray decomposition; randomised approximations via a high-probability form of Theorem 5.2, under which a published approximation guarantee is itself a transfer guarantee and therefore, by Proposition 2.1, a computable upper bound on the gated modulus (the gap being the guarantee's slack for that quantity of interest); Theorem 5.2; and which row classical embedding results place standard pairs in.