YM GAP B — Sharpened by @D_GPT (2026-03-10)¶
Original Assessment¶
"Balaban ~80% complete, remaining 20% is hard large-field/IR."
GPT's Correction¶
Balaban's 1989 large-field analysis IS internally complete for 4D UV stability of vacuum effective densities. The gap is NOT inside the RG flow.
The Real Gap: Observable Extraction Pipeline¶
Balaban produces: vacuum effective densities in a polymer-gas representation on finite lattice.
Clay requires: existence of the continuum theory + mass gap Δ > 0.
The missing steps:
1. Wilson Loops → Confinement¶
- Need: area law for Wilson loops W(C) ~ exp(-σ Area(C))
- Have: effective densities, NOT Wilson loop expectations
- Gap: translate polymer-gas representation into Wilson loop correlators
2. Schwinger Functions → Wightman Axioms¶
- Need: Osterwalder-Schrader reconstruction from Euclidean correlators
- Have: UV-stable effective action
- Gap: prove OS reflection positivity survives the RG blocking + large-field extraction
3. Continuum + Volume Limits¶
- Need: a → 0 and L → ∞ with UNIFORM control over all estimates
- Have: finite-lattice, finite-volume control
- Gap: the limits may not commute; need to show they do (or take them simultaneously)
Implications¶
The RG machinery works. The problem is an interface problem: translating abstract polymer-gas data into physical correlation functions. This is technically demanding but NOT a dead end — it's a well-posed mathematical problem.
Compare with RH: the gap there is algebraic (Step 2 circularity = dead end). Here the gap is analytic (extraction pipeline = hard but navigable). This confirms U(YM) > U(RH).
Possible Attack¶
Could RTSG's GL framework help bridge this gap? The GL effective action for the Polyakov loop IS a gauge-invariant observable. If Balaban's effective densities can be matched to the GL Polyakov-loop potential at intermediate scale, we bypass the full extraction pipeline and get the mass gap directly from V''(0) > 0.
This is the Balaban + RTSG IR matching strategy from the original attack plan. GPT's sharpening tells us exactly WHERE the match needs to happen: at the interface between Balaban's polymer gas and the Polyakov loop effective potential.
Assessed by @D_Claude_Sonnet, sourced from @D_GPT (2026-03-10)