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D5 shrinking witness pairs: divided-difference m=2 bound - #125
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The fixed-eta factorial moment stays the outer boundary. Mutual separation may tend to zero inside the fixed remote region, and the ordered same-index expectation remains O(k r^3). Co-authored-by: Dylan Roy <d6g8k5htny@privaterelay.appleid.com>
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Review of #125 at head Read: the full three-dot diff (4 files, +312/−2), Mathematics. The §3 upper bound reads as sound at its stated scope: Jacobian δ^d, σ_min(H) ≤ ‖Hu‖ ⇒ |det H| ≤ ‖Hu‖‖H‖_F^{d−1}, H_x u = −(δ/2)D³f(x)[u,u,·]+O(δ²) under G₁=0, majorant C k r³ δ^{2−d}, and ∫s^{2−d}s^{d−1}ds = ∫s ds. Findings:
Engineering. Draft; conflicts in both shared files against current main ( Verdict: AMEND — ACCEPT-at-stated-scope for the §3 upper bound as an author-side note; amendments 1–4 plus rebase before this leaves draft. Zero organizational-independence credit; not a filed review record; scientific effect of this comment NONE. Generated by Claude Code |
…itness-bcee # Conflicts: # docs/NAVIGATION.json # docs/RESEARCH_INDEX.md Co-authored-by: Dylan Roy <d6g8k5htny@privaterelay.appleid.com>
- Display the uniform moment input as Lemma 1 with the complete compact parameter set (r, x, u, delta, t) and its regression/Sobolev/Fernique proof; §2 now cites the lemma instead of a one-sentence appeal to regression. - Reword §3, §5 and §6 so the note claims an upper bound only; the r^3 is named as an artifact of the discarded second height indicator and the true shrinking-pair order is stated as not established here. - Restore the original #76 route row in docs/RESEARCH_INDEX.md and add a separate shrinking-pair row; the index paragraph says upper bound only. - Rename the fifth axial derivative to omega (rho is the remote radius), make the Bargmann-Fock check rational, fix the delta_* wording, and state that the lock tests restate algebra and cannot detect an analytic error. - Resolve the NAVIGATION.json / RESEARCH_INDEX.md conflicts against main. Ran: python -B -m unittest discover -s tests (127 OK); tools/navigation_check.py (no problems). Scientific effect NONE. Co-authored-by: Dylan Roy <d6g8k5htny@privaterelay.appleid.com>
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Amendment for review comment 5850462018 landed on this branch at What changed, item by item:
Ran at Remains uncertain and untouched: the true order of the shrinking-pair count; the pinned contact kernel; everything in §6. Landing this merges an author-side note with an explicit AMEND record — it moves no STATUS row. |
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…itness-bcee Co-authored-by: Dylan Roy <d6g8k5htny@privaterelay.appleid.com>
Scope
Additive reconnaissance only. The closed fixed-ρ / fixed-η review and
Math-/frontiers/remote_window_20260924/PROOF.mdat191ea7d541a486736ba7bbddfd4eac25a6c4567b(SHA256a332bae9bdc0106ce17047f7e0409cc3d94eb610a0c7b74ba5ba2d01a1620cb7) are unchanged.The outer boundary is the accepted fixed-η factorial moment: for separation bounded below independently of
r, the ordered same-index pair expectation is(k r^3)^2times a joint contact integral, and the unordered-pair probability isO(r^6).Result
Both witnesses stay in the fixed remote region
D_ρ. Their separationη(r)may tend to zero. The divided-difference coordinateshave Jacobian
δ^dand a contact covariance(∇f(x), H_x u)that stays uniformly positive definite. Each witness determinant is thenO(δ)becauseσ_min(H) ≤ ||H u||, so the product isO(δ^2). One endpoint weight and the original endpoint normalizerZ_r ~ r^2are used once. The two heights are not independent: with both axial derivatives zero,f(y)-f(x) = -μ δ^3/12 + O(δ^4), so a shrinking pair shares one window of lengthk r^3.The separation integral is
∫ s ds, which stays bounded asη ↓ 0in every dimensiond ≥ 2. Thereforeuniformly in
η ∈ (0, δ_*], and the unordered-pair probability is at most half of that. The fixed-ηO(r^6)bound is not inherited onceηshrinks.Sending
η → 0inside the fixed-η kernel is blocked: the raw gradient covariance collapses, the Jacobianδ^{-d}was omitted from that kernel, and the leading axial curvatures have opposite signs, so same-index pairs need an extra transverse-curvature or third-derivative jet. That extra jet is not required for the upper bound.Pin neighborhoods, the intermediate annulus, elder pairing, and global RN / 24-jet closure stay open.
Checks
tests/test_d5_shrinking_witness.pylocks the Jacobian, the determinant comparison, the axial and height-gap coefficients, the radial integral, and the model-field residual variance6. It does not sample the periodized pinned field. Landing and navigation checks passed locally. A Bargmann–Fock sampling diagnostic is recorded in the note and is not an input to the bound.