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[P2] C4 self-matching site triangulation parity control #44

Description

@LightChainr

Goal

Build the closest exact control for the proposed matching-parity projector: a site-percolation, C4-symmetric, self-matching periodic triangulation.

See notes/c4-self-matching-triangulation-control.md.

Lattice

Take the square lattice and add one diagonal to every square, alternating / and \ by checkerboard face parity (equivalently connect the even-parity corners). Every face is triangular, so the graph is its own site matching graph.

The degree pattern is 8/4 on the two vertex parities and the diagonal pattern is C4 invariant up to translation/rotation.

For periodic amenable site percolation the self-matching relation gives exact p_c=1/2.

Why this control is decisive

At the finite-size critical center, with the same quotient and wrapping convention,

M(1/2)=R_G(1/2)-R_G(1/2)=0

should be an algebraic/runtime invariant.

But the individual wrapping probability can still carry a C4 spin-4 anisotropy. Therefore this model separates:

  • matching-even square anisotropy (x=4 candidate);
  • matching-odd central residual (x=21/4 candidate), which must vanish in the self-matching control.

This is more directly comparable to the square-site target than square-bond duality, while avoiding the C6 spin-4 suppression of the ordinary triangular lattice.

Compatible Gaussian sizes

Checkerboard parity descends when both period components are odd. Start with

  • N=130: (11,3) vs (9,7);
  • N=170: (13,1) vs (11,7).

If needed, confirm with N=290: (17,1) vs (13,11).

The existing cyclic label j=ax+by mod N satisfies j mod 2 = x+y mod 2 for odd (a,b), so the checkerboard sublattice is cheap to implement in the current same-N engine.

Exact correctness gate

Before stochastic runs:

  1. verify all quotient faces are triangles;
  2. verify the site matching generator adds no connectivity beyond the graph itself;
  3. exhaustively verify central M=0 on the smallest compatible quotients;
  4. verify C4 invariance up to quotient automorphism;
  5. verify degree/local-face multisets across the two orientation representations.

Production observables

At p=1/2, retain individual either/cross wrapping probabilities for both orientations. Form

P4[R]=(R(theta1)-R(theta2))/DeltaCos4.

The matching difference should be asserted zero rather than estimated as a noisy target.

Compare, in this order:

  • fixed P4[R] = A N^-1;
  • zero anisotropy;
  • only after fixed scoring, free exponent/log alternatives.

The control amplitude need not equal the target square/matching-pair amplitude.

Acceptance

The two-spin4 parity model is strongly supported if this C4 self-matching site lattice has a reproducible ordinary N^-1 cos4theta anisotropy while the central matching-odd sector remains exactly zero.

A failure of the finite self-matching identity is an implementation error until proven otherwise; a failure of the N^-1 ordinary anisotropy is a scientific negative result.

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priority:P2Deferred research or on-demand support; no default new compute allocation.

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