Coarse-graining support: Support.CoarseGraining.ThetaEllipticity #
Imported from the Apache-2.0 CoarseGraining development at commit
c7ddd76c08ade64fed1b8d2ca51be14dfee8deb4.
Ellipticity class and shared matrix infrastructure #
Formalization of the sharp-constant pointwise ellipticity vocabulary of
Proposition 2.1 of the high-moment paper (Armstrong–Kuusi–Loher, in
preparation), against the coarse-graining surface of this development. Items
A1–A3, together with a handful of shared MatLoewnerLE helpers and the key
nonsymmetric flux inequality (★) reused by the sharp block bounds.
All matrix work is on Vec d = Fin d → ℝ / Mat d; no EuclideanSpace.
Scalar-multiple-of-identity quadratic forms and MatLoewnerLE helpers #
A1 — the (1, Θ) ellipticity class #
A1. Membership in the uniform ellipticity class with constants (1, Θ):
ξ · A ξ ≥ |ξ|² and ξ · A⁻¹ ξ ≥ Θ⁻¹ |ξ|².
Equations
Instances For
A2 — the law-level ellipticity predicate #
A2. A carrier coefficient law is Θ-elliptic when almost every
realization lies, almost everywhere in space, in the (1, Θ) ellipticity class.
Following the carrier redesign (Packet P3, decision E-2), the entrywise
measurability conjunct of the paper's class Ω_Θ is now free by type: every
element of the honest-fields carrier RegCoeffField d carries a proof that each
of its scalar entries is Borel measurable (RegCoeffField.entry_measurable), so
the a.e.-modification bridge (CoarseBounds/AeBridge.lean) recovers the
pointwise-elliptic representative from a.entry_measurable rather than a bundled
conjunct. The statement is therefore the paper's clean Ω_Θ membership.
Equations
- HCPolySupport.ThetaEllipticLaw Θ P = ∀ᵐ (a : HCPolySupport.RegCoeffField d) ∂P, ∀ᵐ (x : HCPolySupport.Vec d), HCPolySupport.IsEllipticMatrix 1 Θ (a.toFun x)
Instances For
The key nonsymmetric flux inequality (★) #
For an elliptic matrix B, |B η|² ≤ Lam · (η · sᴮ η) where sᴮ = symmPart B.
This is the second ellipticity inequality read backwards, and is the workhorse
behind the sharp flux bounds A5 and the nonsymmetric coercivity A4.
The flux inequality (★): ‖B η‖² ≤ Lam · η · (symmPart B) η.
A3 — symmetric part Loewner bounds #
A3 (upper). s ≤ Θ • 1 in the Loewner order, s = symmPart A.
A3 (lower). 1 ≤ s in the Loewner order, s = symmPart A.