OneStepConditional #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
l.excess.decay.good.scales, conditionally on the harmonic-approximation anchor #
The one-step excess-decay contraction is assembled here from
- everything proved in
OneStepWindows/OneStepCompetitor/OneStepTriangle/OneStepAssembly/OneStepGoodScales, and - exactly one derived-result hypothesis,
hharm, which is the conclusion of the harmonic-approximation anchorAlgsuperdiff.Frozen.Section4.harmonic_approximation_good_scales, transcribed as aPropat the instance this proof needs.
The instance hharm is transcribed at #
The general clause is instantiated at
d := d , M := M , s := s , L := L , m := m , n := n - 2 ,
x := wellPlacedCentre x m (n-2) , z := z , u := u , h := h , g := g ,
v := v , w := u - v
i.e. at the window choice y := wellPlacedCentre x m (n-2) proved admissible
in OneStepWindows.image_add_wellPlacedCentre_subset_windowChoice. Every
index is therefore written here exactly as the anchor prints it after that
substitution — the good-event index is n - 2 + 3, not the arithmetically
equal n + 1, and the replacement window is (y + ·) '' □_{n-2}.
The right-hand side is carried as a single universally quantified B : ℝ≥0∞
with B ≠ ⊤, so that instantiating B at the anchor's own four-term
right-hand side turns hharm into that clause verbatim.
The honest-vs-printed delta (leg by leg) #
- Good-event index. Print gates at
𝒢(n, z; s/8, (s/8)δ^{1/2}); the anchor delivers at indexn - 2 + 3 = n + 1. Carried here at the anchor's index. The two events are incomparable (no monotonicity ofgoodEventAtin the scale index exists, and none is structurally available: the𝒢₀/𝒢₂weights themselves depend on the index). - Good-event
εslot. Print gates atε = (s/8)δ^{1/2}, the anchor atε = 1/2. Both appear here:hmemis at the printedε,hharmat the anchor's, andOneStepGoodScales.le_of_indicator_goodEventAt_lebridges them (goodEventAt_mono_ep). This is a bridge, not a deviation. - Replacement window. Print puts
‖u-v‖onU_2 = (x+□_{n-2}) ∩ □_m; the anchor puts it on the full cubey + □_{n-2} ⊇ U_2. Carried at the anchor's window, paid at the volume ratio3^{d}. - Contraction factor. The
3^{-k/2}leg is at the printed windowE(u, (x+□_n) ∩ □_m); theδ^{1/2}leg is insideB, i.e. inside the unexpanded anchor.
The one-step excess-decay contraction, conditional on the harmonic approximation anchor.
E(u, U_k) ≤ C_t Csch κ (3^{-k})^{1/2} E(u, U_0)
+ (81 C_t Csch + 9·3^k √((3^k)^d)) · 3^{-n} · 3^d · ‖RHS‖
+ C_t (3^{n-k})^{1/2} Kh
valid pathwise at every ω of the printed good event
𝒢(n-2+3, z; s/8, (s/8)δ^{1/2}).