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:
ae_coarseBlockQuadratic_lower_of_thetaEllipticLaw— the a.s. lowerC1Loewner bound (mirroring the upper boundae_coarseBlockQuadratic_bounds_...).half_le_barSigmaAtScale—1/2 ≤ b.barSigmaStarAtScale_pos/barSigmaStarAtScale_le_two_mul_Theta—0 < candc ≤ 2Θ.
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.
0 < c.
c ≤ 2Θ.