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LeanPool.Superdiffusion.Algsuperdiff.Section4.Provider.BoundsEaL.ShellSlotBounds

ShellSlotBounds #

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

The two gauge slots, resolved into a head block and an L-carrying tail #

Nothing here imports that file, and nothing here claims the anchor.

The shell-sum route #

MajorantSlots.lean isolates the whole L-dependence of Step 3's display in the two gauges of the recentered shell h = k_L − k_{j−2} − (k_L − k_m)_{□_m}. This module resolves both gauges into

(an L-FREE head block over the layers k ∈ (j−2, m])  +  (a tail over k ∈ (m, L]) ,

using only proved material:

Both tails are values of ONE functional of the shell stream, the (m, L]-layer gauge sum

tailLayerSum k v ω L = Σ_{i ∈ (m, L]} ‖∇ j_i‖_{W^{1,∞}(3^k v + □_k)} ,

which is nondecreasing in L. An L-free bound for it is therefore the ONLY L-uniformity input the whole majorant needs; it is a parameter here (hT), disclosed below.

The disclosed obligation hT, and why it is not discharged here #

hT asks for a real T k v ω dominating the tail sums for every L ≥ m, i.e. for the convergence of the upper shell series with an explicit bound. This is a genuine mathematical input about the stream, not a source premise and not a proof step in disguise:

References #

The layer gauge sums #

The head block of the layer expansion at the cube 3^k v + □_k: the layers i ∈ (k−2, m], which is the block the Step-3 display resums. L-free.

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    noncomputable def Algsuperdiff.Section4.Provider.BoundsEaL.tailLayerSum {d : ℕ} (m k : ℤ) (v : Fin d → ℤ) (omega : Section3.Cutoff.CutoffSample d) (L : ℤ) :

    The tail block of the layer expansion at the cube 3^k v + □_k: the layers i ∈ (m, L], i.e. the k > m block. This is the ONLY carrier of L in the whole majorant.

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      noncomputable def Algsuperdiff.Section4.Provider.BoundsEaL.tailLayerTerm {d : ℕ} (m k : ℤ) (v : Fin d → ℤ) (omega : Section3.Cutoff.CutoffSample d) (i : ℤ) :

      The layer gauge extended by zero below the recentering scale: the canonical ℤ-indexed summand of the upper shell series.

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        The canonical tail gauge: the value of the upper shell series.

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          theorem Algsuperdiff.Section4.Provider.BoundsEaL.tailLayerSum_le_tailSeriesGauge {d : ℕ} (m k : ℤ) (v : Fin d → ℤ) (omega : Section3.Cutoff.CutoffSample d) (hsum : Summable (tailLayerTerm m k v omega)) (L : ℤ) :
          tailLayerSum m k v omega L ≤ tailSeriesGauge m k v omega

          The obligation hT, reduced to summability.

          If the upper shell series converges at ω, its value is an L-uniform bound for every tail block. This is the exact bridge from a probabilistic summability statement to the L-freeness input used below: no other property of the stream is needed.

          The gradient slot #

          The gradient gauge of the recentered shell, split at m.

          The cube-scale normalization of Annular.GradNormalization followed by the layer expansion of Support.shellW1InfGradNorm_translate_shellIncrement_split. The head block is L-free; the tail block is the k > m layer sum.

          The L-free gradient slot, at a caller-supplied tail gauge T.

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            theorem Algsuperdiff.Section4.Provider.BoundsEaL.gradientW1Infinity_step3Shell_le_lFreeGradSlot {d : ℕ} (M : Section3.ABKModel d) {m : ℤ} (R : HCPolySupport.TriadicCube d) (h2m : R.scale - 2 ≤ m) (T : ℤ → (Fin d → ℤ) → Section3.Cutoff.CutoffSample d → ℝ) (omega : Section3.Cutoff.CutoffSample d) (hT : ∀ (L : ℤ), m ≤ L → tailLayerSum m R.scale R.index omega L ≤ T R.scale R.index omega) (L : ℤ) (hle : R.scale - 2 ≤ L) (hmL : m ≤ L) :
            (step3Shell M L m R hle omega).gradientW1Infinity ≤ lFreeGradSlot m T R omega

            The gradient slot bound, L-free. Every L ≥ m obeys the same bound once the tail gauge is L-uniform.

            The value slot #

            The mean-value tail of the value slot, expanded into layers.

            3^{2m} ‖∇(k_L − k_m)‖_{W^{1,∞}(□_m)} is at most the (m, L] layer sum at the origin cube of scale m, by the same triangle inequality.

            The L² gauge of the recentered shell, split at m.

            Annular.valueL2_centeredShellUnitCube_le at the manuscript's own centering constant (k_L − k_m)_{□_m}, with the mean-value tail expanded into layers. The first summand is L-free.

            The L-free value slot, at a caller-supplied tail gauge T.

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              theorem Algsuperdiff.Section4.Provider.BoundsEaL.valueL2_step3Shell_le_lFreeValueSlot {d : ℕ} (M : Section3.ABKModel d) {m : ℤ} (R : HCPolySupport.TriadicCube d) (hnm : R.scale ≤ m) (hv : R.index ∈ Support.latticeCubeSet d R.scale m) (T : ℤ → (Fin d → ℤ) → Section3.Cutoff.CutoffSample d → ℝ) (omega : Section3.Cutoff.CutoffSample d) (hT : ∀ (L : ℤ), m ≤ L → tailLayerSum m m 0 omega L ≤ T m 0 omega) (L : ℤ) (hle : R.scale - 2 ≤ L) (hmL : m ≤ L) :
              (step3Shell M L m R hle omega).valueL2 ≤ lFreeValueSlot m T R omega

              The value slot bound, L-free.