Current task: —

Updated 08-18-2026

G-001 — Multiple-zero density bounds as extra chain constraint ("Idea C")

Date: 2026-08-17 | Session: 001 | Track: A | Tag: [FAILED-ATTEMPT(obstruction below)] Opened: D-009 §4 (Idea C), thread T5. Killed: same day, before literature investment — the obstruction is unconditional on any s₂ bound.

Attempt

Feed an unconditional upper bound on on-line multiple zeros (s₂ ≤ κN, Levinson/CGG-style input) into the chain as an extra constraint, hoping to beat 2 − R(ψ). Rationale at opening: the 0.682 ceiling theorem constrains only 2-moment certificates; multiplicity bounds are a different data class.

Obstruction (the s₂/p substitution symmetry)

On-line doubles and off-line pairs play IDENTICAL roles in the chain: both cost 2 in N(I′), both occupy the Q′ positive-index budget at the flat charge 4 (D-005). Replace each on-line double at ordinate γ by an off-line pair {½+δ+iγ, ½−δ+iγ}. In every bandwidth-one two-moment datum: e^{2πij(γ+iδ)/N} + e^{2πij(γ−iδ)/N} = 2e^{2πijγ/N} + O(δ) (δ→0), which equals the double's contribution m=2. Hence the adversary moves all multiple mass into depth→0 off-line pairs leaving every usable measurement unchanged; any s₂-bound is vacuous against this configuration.

Lesson

The binding wall is not moments, windows, or multiplicities — it is that OFF-LINE-PAIR MASS at shallow depth is invisible to every unconditional data class in the method. Any certificate improvement must either (1) see depth directly (needs prime-pair/support>1 data — walls S1/S2, D-006 §6), or (2) constrain p by new unconditional input — and p-bounds are essentially RH-strength (the D–H/Epstein gate). Multiplicity-side inputs (s₂) are provably useless within this framework.

Salvage