BoundaryTransports #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The boundary lane's data transports onto the anchor window #
The boundary Caccioppoli's data legs — the force [g] and the boundary
gradient [∇h] — are Gagliardo seminorms, not L² norms, and this module
supplies the same move for them:
[f]_{H^s(c+□_{n+2})} ≤ 3^d · [f]_{H^s(W')} ,
together with the composition that the boundary Caccioppoli's right-hand side actually reads: CoarseGraining's cube Besov seminorm of the transported force, in the covering cube's own frame, priced by the anchor's own window seminorm.
References #
- ABK26,
l.harmonic.approximation.good.scales, Step 2.
1. The Gagliardo window move #
Gagliardo transport assuming containment of the covering cube in the window.
The Gagliardo seminorm transport onto the anchor's window.
Real-valued Gagliardo transport under the same containment and finiteness hypotheses.
The Gagliardo window move, in the real-valued form the boundary assembly consumes. The finiteness hypothesis is the anchor's own clause (iv), read on the anchor's window.
2. The force leg of the boundary Caccioppoli, onto the anchor's window #
The transported force Besov budget under covering-cube containment.
The transported force's cube Besov seminorm, priced on the anchor's window.
BoundaryOuterAssembly reads its force leg as CoarseGraining's cube Besov
seminorm of y ↦ −g(y + c) on the covering cube □_{n+2} in that cube's own
frame. This is the composition of BesovBridge's Besov--Gagliardo comparison
at the covering cube with the window move of section 1: the whole leg is priced
by the anchor's own [g]_{H^s(W')} at the scale weight 3^{s(n+2)} and the
coefficient-free constant besovGagliardoConstant d · 3^d.
3. The covering cube's own clause-(iv) data #
The anchor's L² datum, restricted to the boundary covering cube.
The anchor's Gagliardo datum, restricted to the boundary covering cube.