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LeanPool.Superdiffusion.Support.HighContrast.Variance.ScalarBounds

ScalarBounds #

Ported from scottnarmstrong/CoarseGraining at c7ddd76c08ade64fed1b8d2ca51be14dfee8deb4. Module imports, support namespace and local option directives adapted for Lean Pool.

Scalar normalization bounds for the fluctuation bridge #

The fluctuation observable normalizes the centered coarse block matrix by the diagonal D = diag(scalarFullBlockInvSqrtDiag b c), where b = barSigmaAtScale and c = barSigmaStarAtScale are the structural-law scalars.

Here we pin down the two-sided bounds on b and c that make the diagonal normalization uniformly bounded:

The b and c values are read off the isotropic annealed block matrix (annealedBlockMatrixAtScale_eq_scalarAnnealedBlockMatrixAtScale), whose diagonal basis pairings equal b and c⁻¹, integrated against the a.s. C1′ sandwich (mean_zero_coarse_blockQuadratic).

C1 (lower, a.s.). Under the amended ThetaEllipticLaw Θ L, the coarse block observable a.s. dominates the lower diagonal quadratic form ½|p|² + (2Θ)⁻¹|q|². Proved by routing each realization through the C2 truncation bridge to an everywhere-(1,Θ)-elliptic representative and applying the deterministic lower Loewner sandwich, exactly as ae_coarseBlockQuadratic_bounds_of_thetaEllipticLaw does for the upper bound.

Integrability of the coarse block quadratic form for a fixed probe vector, under any ThetaEllipticLaw on a probability law.

1/2 ≤ b. The structural-law scalar \bar\sigma_m is at least 1/2: it is the annealed diagonal upper-left entry, which the integrated lower C1 sandwich bounds below by 1/2.