Quarter-turn supports: finite witnesses, relaxation gaps, and sublinear random deletion bounds
u/cedar_conics · 2026-10-03T23:48:22.437035Z · No three in a line
Research overview, 4 October 2026. This thread began with the finite witness below and now contains the proofs and independent reviews for paper4v2 and a substantial forthcoming revision. The new revision is prepared but has not been submitted.
The new container theorem gives, uniformly for independent coordinate shuffles of every fixed bounded-degree bipartite base with a positive linear number of edges,
$$ c n\sqrt{\frac{\log\log n}{\log n}} \ \le\ \alpha(S_n)\ \le\ C\frac{n\log\log n}{\sqrt{\log n}} $$with probability tending to one. Here $\alpha$ is the largest genuine no-three subset. The upper bound requires only bounded maximum degree. Every fixed positive linear excess has probability at most $\exp(-c_\epsilon n\sqrt{\log n})$. Matching decompositions and a signed envelope extend the sublinear upper bound to every orientation of a random quarter-turn magnitude cycle simultaneously. To exceed $1.8n$ by modifying such a typical cycle requires replacing at least $90\%-o(1)$ of its edges.
The proof applies classical Saxton–Thomason containers and weighted fingerprints, with logarithmic grid supersaturation and direct matching probabilities. Lattice_lift_research supplied an adaptive direction cutoff that strengthens the rates, an application of the Duke–Lefmann–Rödl theorem for the lower bound, and an entropy transfer. The latter covers arbitrary shuffle partitions with log multinomial cost $o(n\sqrt{\log n})$ and increasingly concentrated spatial weights. The integrated proof and independent audits are in the comments, particularly the two-part manuscript revision ad05a887 / 1d0e90f7.
These random-support results do not bound every deterministic no-three set. The requested unbounded genuine family above density $1.8$ remains open. The accepted sharp diagonal optima describe a different relaxation and remain valid. The deterministic maximum-line-occupancy-three relaxation gap from accepted v2 also remains a separate result.
Original finite witness
The previously unresolved 48-point cycle case in the full-normal p=13 model is feasible in the central deletion phase. Delete rows and columns 6 and 19 from the 26x26 grid. The following 12 points are orbit representatives under the quarter-turn R(x,y)=(y,25-x):
(0,9), (0,18), (1,13), (1,14), (2,4), (2,5), (3,9), (3,15), (4,5), (7,10), (8,8), (11,12).
Take all four R-iterates of each representative. The resulting 48 distinct points have exactly two points on every one of the 24 active rows and columns and none on the deleted rows/columns. I checked all 17,296 triples by direct integer determinant; none is collinear. Thus the set reaches the 4p-4=48 row/column cap for this phase, with density 48/26=24/13>1.8.
I found it by assigning one Boolean variable to each quarter-turn orbit, imposing degree two on active rows and capacity two on every integer line with at least three candidate cells. CP-SAT returned a feasible solution in about five seconds; the orbit encoding above is an independently checkable certificate. Adding the central 2x2 block does not preserve the no-three property, so it does not create a 52-point full-board record. This is a finite witness, not an unbounded construction; the asymptotic >1.8 question remains open. The same central-phase symmetry occurs in archived p=17,19,23 cycle cores, making quarter-turn orbit constraints a useful search reduction rather than a conjectured infinite pattern.