OneStepBoundaryEndpoint #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The boundary-branch excess-decay endpoint #
OneStepSchauderChain.excessDecay_oneStep_interior_of_harmonicApprox closed the
four Schauder slots of
OneStepConditional.excessDecay_oneStep_of_harmonicApprox on the interior
branch, at K_h = 0. This module does the same on the boundary branch,
through the boundary branch's split Schauder bound:
Csch = boundarySchauderConst d = 48 · 3^{3/2} · schauderConst d · √((24(d+1))^d) ,
K_h = boundarySchauderConst d · (3^{-n})^{1/2} · (3^{-(n-2)} · boundaryDatumLeg …) .
The competitor enters through classical harmonicity on the doubled window
reflectedWindow x m (n-2) — which is what
OneStepSchauderComposeBoundary.exists_classicalCompetitor_reflectedWindow
produces from a variationally harmonic odd extension — together with its
square-integrability there. Nothing here restricts the met set: the geometry
of OneStepBoundaryGeometry is uniform in it.
What is still open, precisely #
- The
_of_weaklyHarmoniclevel.OneStepSchauderComposeInterior.excessDecay_oneStep_interior_of_weaklyHarmonicremoves the classical-harmonicity slot by applying Weyl's lemma on the anchor's moved replacement cubey + □_{n-2}, which is exactly where the anchor'shharmlives. On the boundary branch the Schauder competitor lives onreflectedWindow x m (n-2), and the moved replacement cube is not contained in it (in a met coordinate the clamped cube protrudes on the window side:windowLo ≥ y_i − ½·3^{n-2}), so the two representatives must be identified onU_2— where both are continuous and both agree a.e. with the competitor — beforehharmcan be transported. That identification, plus theEqOntransfer ofgradFieldand ofaffineExcess, is the remaining assembly; it is bookkeeping, not analysis.