Documentation

LeanPool.Superdiffusion.Support.HighContrast.Corridor.PhaseComparison.Stability

Stability #

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

Per-phase stability of the corridor observable #

Statement of p.phase.comparison's stability estimate e.phase.comparison.stability in the discrete-grid setting. With U := cubeSet (originCube d m), S := corridorSet ℓ σ, and Z the minimizer for (a, P) (exists_cubeBlockMinimizer, which supplies Mu U P a = blockEnergyAverage U a Z):

The general B′3 assembly is abs_coarseObservable_sub_le_of_minimizer; abs_phaseObservable_sub_le_of_minimizer specializes it to the corridor field. abs_phaseObservable_sub_le (M2) is the existential wrapper. The Z-as-input form is what grid averaging needs, since one minimizer serves every phase σ.

Field-level ellipticity transport through the corridor #

theorem HCPolySupport.isEllipticFieldOn_corridorField {d : ℕ} {Θ : ℝ} {U : Set (Vec d)} (hU : MeasurableSet U) (hΘ : 1 ≤ Θ) {ℓ : ℝ} {σ : Vec d} {a : CoeffField d} (hEll : IsEllipticFieldOn 1 Θ U a) :

The corridor self-map preserves everywhere-(1, Θ)-ellipticity on U: the pointwise ellipticity is corridorField_isEllipticMatrix, and the entrywise measurability of the U-truncated modified field is the corridor-gated piecewise of the constant (1 : Mat d) and the original truncated field.

The Mu-quadratic as a normalized energy integral #

P·𝐀(U; a)P = (vol U)⁻¹ ∫_U Z·(blockCoeffField a)Z for any minimizer Z of (a, P) on the half-open triadic cube. This is Mu = ½ P·𝐀 P combined with Mu = blockEnergyAverage, the ½ cancelling the density's ½.

The general two-field coarse-stability lemma (B′3 core) #

theorem HCPolySupport.abs_coarseObservable_sub_le_of_minimizer {d : ℕ} [NeZero d] {Θ : ℝ} (hΘ : 1 ≤ Θ) {m : ℤ} {S : Set (Vec d)} (P : BlockVec d) {c c' : CoeffField d} (hEll : IsEllipticFieldOn 1 Θ (cubeSet (originCube d m)) c) (hEll' : IsEllipticFieldOn 1 Θ (cubeSet (originCube d m)) c') (hS : MeasurableSet S) (hSU : S ⊆ cubeSet (originCube d m)) (hagreeOff : Set.EqOn c c' (cubeSet (originCube d m) \ S)) {Z : BlockState d} (hZadm : IsBlockMuAdmissible (cubeSet (originCube d m)) P Z) (hZresp : BlockResponseSpace c (cubeSet (originCube d m)) Z) (hZeng : Mu (cubeSet (originCube d m)) P c = blockEnergyAverage (cubeSet (originCube d m)) c Z) :

General coarse stability. For two fields c, c' that are (1, Θ)-elliptic on U := cubeSet (originCube d m) and agree on U ∖ S, the coarse observable moves by at most 48 Θ (vol U)⁻¹ times the S-energy of any minimizer Z for c. This is the corridor-independent heart of abs_phaseObservable_sub_le_of_minimizer.

M2: corridor specialization #

M2 core. Given the minimizer Z for (a, P) (its admissibility, response-space membership and energy-realizing identity), the corridor-phase comparison bound holds with the corridor energy of that specific Z. This is a specialization of the general two-field bound; abs_phaseObservable_sub_le obtains Z and calls this.

M2 (per-phase stability). For a fixed grid phase σ and a coefficient a that is (1, Θ)-elliptic on U := cubeSet (originCube d m), the coarse observable moves by at most a normalized corridor energy of the minimizer Z for (a, P).