Alphabeta Math
LemmaStatement: AI-adaptedProof: AI-generatedPipeline-generated
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.

Fixed-pivot projection has first-order bounded-Lipschitz kernel quadrature error

Statement

Let μ∈Mw(E) be positive and put m=M0(μ). With F the continuous vector field and FΔ the no-cutoff grid field, for PΔμ=∫PΔ(x)μ(dx) one has ∥FΔ(PΔμ)−PΔF(μ)∥BL≤Δ[3LK+K∗2m2+(Lβ(D+1)+β∗LB)m].

Facts & Assumptions

Given: A mesh with maximum cell width Δ≤1, bounded Lipschitz kernels, and a positive finite-number measure.

[F1]

Unbounded-grid fixed-pivot coagulation-fragmentation dynamics: FΔ projects every product and daughter to the grid by PΔ and preserves each event's first moment.

[F2]

Continuous-size coagulation-fragmentation weak model: F has the stated coagulation and fragmentation weak forms, with K Lipschitz and dBL(Bx,By)≤LB∣x−y∣.

[F3]

Bounded-Lipschitz discrepancy for finite measures: ∥σ∥BL is the supremum over tests of supremum norm and Lipschitz constant at most 1.

[F4]

Fixed-pivot weights are nonnegative and reproduce number and mass: PΔ(z) has total mass 1, expected displacement at most Δ/2, expected mass exactly z, and second-moment excess at most Δ2/4.

[F5]

Bounded coagulation is bilinear and bounded in weighted total variation: the continuous coagulation term maps Mw(E)2 to Mw(E).

[F6]

Mass-normalized fragmentation is bounded in weighted total variation: the continuous fragmentation term maps Mw(E) to Mw(E).

[F7]

Unbounded-grid fixed-pivot dynamics are globally well posed and stable: FΔ is well-defined on weighted grid measures.

Proof

1.1givenF3F4F5F6F7algebra

By [F5] and [F6], F(μ)∈Mw(E), and [F4] makes PΔF(μ) well-defined; [F7] gives FΔ(PΔμ)∈Mw(E). Fix a test φ admissible in [F3] and set φˉ(z)=∫φ(u)PΔ(z)(du). On each cell this is the linear interpolation of endpoint values; its slope has absolute value at most 1, so φˉ is also admissible. The displacement estimate [F4] gives ∫∣u−z∣PΔ(z)(du)≤Δ/2.

2.1F1F2step 1.1algebra

For the coagulation term, sample X∼PΔ(x) and Y∼PΔ(y) independently. The grid-field test integrand averaged over X,Y has gain Eφˉ(X+Y) and losses φˉ(x)+φˉ(y); the projected continuous-field integrand has gain φˉ(x+y) and the same losses. The gain difference is at most E(∣X−x∣+∣Y−y∣)≤Δ. Also E∣K(X,Y)−K(x,y)∣≤LKΔ, and the event bracket has absolute value at most 3. Thus the absolute difference of the two coagulation integrals is at most 12(3LK+K∗)Δm2.

2.2F2F3step 1.1algebra

For fragmentation, write G(x)=∫φˉ(z)Bx(dz). Then ∣G(x)∣≤D, ∣G(x)−φ(x)∣≤D+1, and ∣G(X)−G(x)∣≤LB∣X−x∣ by [F2] and [F3]. Since Eφ(X)=φˉ(x), the integrand difference equals E{β(X)[G(X)−φ(X)]}−β(x)[G(x)−φˉ(x)]=E[β(X)(G(X)−G(x))]+E[(β(X)−β(x))G(x)]+E[(β(x)−β(X))φ(X)]. The three terms are bounded by β∗LBE∣X−x∣, LβDE∣X−x∣, and LβE∣X−x∣, respectively. Using E∣X−x∣≤Δ proves the displayed bound after integrating over μ.

3.1F3step 2.1step 2.2∎

Adding the coagulation and fragmentation bounds holds for every admissible test in [F3]. Taking their supremum gives the asserted bounded-Lipschitz norm inequality.

Depends on

Used by

Dependency tree · two levels

10 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.

Sources