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LeanPool.Superdiffusion.Algsuperdiff.Section4.Provider.ExcessDecay.InteriorWindowMove

InteriorWindowMove #

Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.

The Gagliardo window move: the child window into the anchor's parent window #

InteriorGlueWindow restricts the anchor's clause-(iv) data from □_m to a sub-window — a membership transport, no constant. This module supplies the opposite, quantitative move on the seminorm itself, which the assembly needs on the correction and forcing legs:

  [g]_{H^s(x+□_n)}  ≤  3^{d} · [g]_{H^s(W)} ,      W = (z+□_{n+2}) ∩ □_m ,

whenever the anchor's geometry binder holds. The mechanism is the volume normalization alone: the Gagliardo measure of a window A is |A|^{-1}(vol⊗vol)|_{A×A}, so passing from W to the smaller x+□_n costs exactly the volume ratio |W|/|x+□_n| ≤ 3^{2d} inside an L², i.e. 3^{d}.

The ratio is the two-scale one because the anchor's own geometry binder puts the child x+□_n inside z+□_{n+1}, hence inside z+□_{n+2}, which carries W; the crude bound |W| ≤ |□_{n+2}| = 3^{2d}|□_n| is used, so the constant is 3^{d} and not the 3^{2d} a two-step application would give.

References #

1. The volume of an origin cube #

2. The seminorm under a window shrink #

The Gagliardo seminorm on a sub-window, at the volume ratio.

If B ⊆ A and |A| ≤ K |B| then [f]_{H^s(B)} ≤ K^{1/2} [f]_{H^s(A)}. Both sides are ℝ≥0∞, so no finiteness is required.

3. The anchor's child-to-parent window move #

The d-only constant of the window move: 3^d, the square root of the two-scale volume ratio.

Equations
Instances For

    The window move.

    Under the anchor's geometry binder, the Gagliardo seminorm on the child window x + □_n is bounded by 3^d times the seminorm on the anchor's own right-hand-side window W = (z+□_{n+2}) ∩ □_m.