InteriorGlueFrame #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The off-grid error is a cube error in the translated frame #
It is not new: CoarseGraining already proves it, unconditionally,
sorry-free, with oleans built —
Homogenization/CoarseGraining/Translation.lean carries the full covariance of
the coarse-graining apparatus under a real translation:
ResponseJ (w + U) p q a = ResponseJ U p q (a(· + w)) (:372)
BlockJ (w + U) P Q a = BlockJ U P Q (a(· + w)) (:303)
Mu (w + U) P a = Mu U P (a(· + w)) (:116)
σ⋆, σ⋆⁻¹, κ, σ, b coarse: the same, at :378--:439 .
𝓔_{t,∞,2}(w + P; g, a₀) = 𝓔_{t,∞,2}(P; g(·+w), a₀) .
What this unblocks (and what it does not) #
With this bridge, the child-frame composition can
feed InteriorGlueCap's cap at the root, provided the child-frame family is
built from the parent's flux-corrected field rather than the child's own
(the child-frame family uses the child's own
antisymmetric increment, which is a different — equally valid — shift of the same
equation). That re-basing, the analogous transport of the coarse-grained
ellipticity factors λ_{r,q}, Λ_{r,q}, and the energy-average transport are
the remaining assembly steps; none of them is assumed here.
References #
- CoarseGraining,
Homogenization/CoarseGraining/Translation.lean.
1. The adjoint commutes with the translation #
Transposition and translation of a coefficient field commute.
2. The set-level doubled response is translation covariant #
The doubled response of a translated set. Both halves move by
CoarseGraining's ResponseJ_translateSet_eq_translateCoeffField; the adjoint
half needs the commutation of §1.
3. The one-cube quantity #
The off-grid one-cube maximum is CoarseGraining's, in the translated frame.
4. The shells and the multiscale error #
The frame bridge.
The multiscale error of the off-grid cube w + P, taken with the ambient
field g, equals CoarseGraining's cube error of P taken with the
translated field g(· + w).