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How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Mean-field training and feature learning — Examples

1 · Prerequisites

2 · Logical flowchart

3 · Definitions, theorems and proofs

None yet.

4 · Examples, counterexamples and false statements

ExampleConstruction: AI-generatedVerification: AI-generatedjudge pass (gpt-6-luna)Open item page →

A single particle does not separate two spheres

Example

Let d≥2 and 0<ra<rb. The one-particle initialization μ0 that assigns unit mass to the origin has compact support {0}⊂B(0,rb), but its support does not separate raSd−1 from rbSd−1: a path from the inner to the outer sphere can avoid the origin.

Facts & Assumptions

Given: d,ra,rb, and the support in the Example.

Verification

Given: Standard basis vectors e1,e2∈Rd.

1.1givenconstruct

The path consisting of the radius-ra circular arc from rae1 to rae2, the radial segment from rae2 to rbe2, and the radius-rb circular arc from rbe2 to rbe1 is continuous after linear reparameterization of its three pieces. Its endpoints lie on the required spheres and every point on it has norm at least ra>0.

2.1givenstep 1.1∎

The path therefore avoids spt⁡μ0={0} while joining the two spheres. By the definition of separation, this support does not separate them.

ExampleConstruction: AI-generatedVerification: AI-generatedOpen item page →

Moving features can represent a target missed by a fixed feature

Example

Let H=R2, y=(1,0), R(z)=12∥z−y∥2, Θ=[0,2π], φ(θ)=(cos⁡θ,sin⁡θ), and V=0. The one-particle measure assigning unit mass to (a,θ) represents aφ(θ) and can attain zero risk at (a,θ)=(1,0). If the feature is fixed at θ=π/2 and only a varies, the minimum risk is 1/2. This finite-dimensional feature-energy example shows a representational distinction only; it makes no convergence claim about either training dynamics.

Facts & Assumptions

Given: The finite-dimensional model and risk in the Example.

[F1]

A one-particle measure at (a,θ) has feature moment aφ(θ) and objective R(aφ(θ)). Feature-measure energy and its regularity assumptions

Verification

Given: R, y, φ, and [F1] as in the Example.

1.1F1givenalgebra

At (a,θ)=(1,0), φ(0)=(1,0)=y, so [F1] gives risk R(y)=0. Since R is a squared norm divided by two, no objective value is negative; hence the moving model has minimum risk zero.

2.1F1givenalgebra∎

With the feature fixed at π/2, φ(π/2)=(0,1) and ∥aφ(π/2)−y∥2=a2+1. Therefore R(aφ(π/2))=(a2+1)/2≥1/2, with equality at a=0. This gives the claimed fixed-feature minimum.

CounterexampleConstruction: AI-adaptedVerification: AI-adaptedjudge pass (gpt-6-luna)Open item page →

The signed-square ReLU differential need not be locally Lipschitz

Statement refuted

Refuted claim: the differential of the signed-square ReLU feature map is locally Lipschitz near the parameter (1,1).

For input law with density p(x)=(2π)−1/2e−x2/2 on R, define Φ(w,b)(x)=max⁡{w∣w∣x+b∣b∣,0} as an element of L2(p(x)dx). This feature map is Fréchet differentiable near (1,1), but its differential is not locally Lipschitz there.

Facts & Assumptions

Given: The signed-square feature and Gaussian density in the Statement.

[F1]

The Gaussian density is continuous, positive on every real interval, and has finite second moment, so the feature belongs to L2 and the kink hyperplane has measure zero. Signed-square ReLU feature parameterization

[F2]

For w,b>0, the preactivation is rw,b(x)=w2x+b2 and its unique zero is c(w,b)=−b2/w2. Signed-square ReLU feature parameterization

Counterexample

Given: Φ, p, and [F1]–[F2] in the Statement.

1.1F1F2givenalgebra

On a small neighborhood of (1,1) with w,b>0, the root c(w,b) is a smooth function of parameters. For an increment h=(h1,h2), r(w,b)+h(x)−rw,b(x)=2wh1x+2bh2+h12x+h22. The candidate differential is DΦ(w,b)h=1x>c(w,b)(2wh1x+2bh2). Outside the interval between c(w,b) and c((w,b)+h), the two preactivations have the same sign; there the ReLU remainder is either zero or h12x+h22, whose L2(pdx) norm is O(∣h∣2) by the finite second moment in [F1]. The interval between the two roots has length O(∣h∣) and lies in a fixed bounded neighborhood of −1; on it the pointwise remainder is O(∣h∣), so its L2(pdx) norm is O(∣h∣3/2). Thus the full remainder is o(∣h∣), proving Fréchet differentiability and the displayed differential.

2.1F1step 1.1algebra∎

At (1,1) the derivative in direction ew=(1,0) is 2x1x>−1. At (1,1+δ) it is 2x1x>−(1+δ)2. For 0<δ≤1/4, their squared L2 distance is 4∫−(1+δ)2−1x2p(x) dx≥8p(2)δ, because the interval lies in [−2,−1], where x2≥1 and p(x)≥p(2), and has length 2δ+δ2≥2δ. The operator norm difference of the two differentials is at least their difference on the unit vector ew. Dividing by the parameter distance δ gives a quotient at least 8p(2)/δ, which diverges as δ↓0. Therefore the differential is not locally Lipschitz at (1,1).

Source note

Chizat and Bach's Lemma D.5 establishes differentiability under a finite-second-moment density assumption. The proposition's application does not establish local Lipschitzness of this differential, which is a separate feature-energy hypothesis.

Sources