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LeanPool.AnomalousDiffusion.AVenhance.Infra.Construction.MaterialAuxiliaryInduction

All-order material jets with a separate auxiliary spatial/word budget.

structure AVenhance.Infra.Construction.MaterialAuxJetLevels {β : ℝ} (I : Ingredients β) (Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ) (N : ℕ) (K : ℝ) (cut : ℕ) :

Source material/spatial jets through cut, using auxiliary budget N. The material range remains finite because time-cutoff data are only used through Nstar; spatial orders can exceed that cutoff.

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    theorem AVenhance.Infra.Construction.material_aux_velocity_nonempty_spatial_abs_le_of_A3 {β C : ℝ} (I : Ingredients β) {Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ} (hΦ : IsStreamSeq I Φ) (hreg : StreamRegularityBounds C I Φ) {m : ℕ} (hm : 1 ≤ m) (α : List (Fin 2)) (hne : α ≠ []) {N : ℕ} (hbudget : α.length + 1 ≤ N) (i : Fin 2) (z : Section4.AmnrSpace) :
    |Section4.amnrWord (fun (y : Section4.AmnrSpace) => streamVel (Φ m) y.1 y.2) (List.map some α) (fun (y : Section4.AmnrSpace) => streamVel (Φ m) y.1 y.2 i) z| ≤ Section4.amnrSpatialVelocityConstant N * epsilon β I.Λ m ^ (β - 1) * (epsilon β I.Λ m)⁻¹ ^ α.length

    Spatial velocity jets at arbitrary finite auxiliary order follow from the all-order spatial displays of the stream-regularity estimates, with no bound on the velocity value.

    theorem AVenhance.Infra.Construction.material_aux_jet_levels_spatial {β C : ℝ} (I : Ingredients β) {Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ} (hΦ : IsStreamSeq I Φ) (hreg : StreamRegularityBounds C I Φ) {N : ℕ} :
    ∃ (K : ℝ), 1 ≤ K ∧ MaterialAuxJetLevels I Φ N K 0

    The zero material level is precisely the source spatial stream-regularity estimate.

    theorem AVenhance.Infra.Construction.material_aux_fastVelocity_mixed_abs_le_of_lower_gradient_bounds {β C : ℝ} (I : Ingredients β) {Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ} (hΦ : IsStreamSeq I Φ) (hreg : StreamRegularityBounds C I Φ) {K : ℝ} {Nspace cut : ℕ} (hlevels : MaterialAuxJetLevels I Φ Nspace K cut) (hK : 0 ≤ K) {m : ℕ} (hm : 1 ≤ m) (α : List (Fin 2)) (n : ℕ) (hn : n ≤ cut + 1) (hcutN : cut + 1 ≤ Nstar β) (hbudget : α.length + 1 + 2 * n ≤ Nspace) (i : Fin 2) (z : Section4.AmnrSpace) :
    |Section4.amnrWord (fun (y : Section4.AmnrSpace) => streamVel (Φ (m - 1)) y.1 y.2) (Section4.amnrMixedWord α n) (fun (y : Section4.AmnrSpace) => streamVel (Φ m) y.1 y.2 i - streamVel (Φ (m - 1)) y.1 y.2 i) z| ≤ (1 + 2 ^ (Nspace + 1) * K) ^ n * materialAuxStreamMixedCurrentConstant I Nspace * epsilon β I.Λ m ^ (β - 1) * (epsilon β I.Λ m)⁻¹ ^ α.length * a β I.Λ m ^ n

    Fast velocity mixed jets use the differentiated recursion and lower material-gradient jets, with the source material order kept at Nstar.

    Uniform fast-velocity constant for the auxiliary material word budget.

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      Scale-step constant for changing the velocity in a material word.

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      • One or more equations did not get rendered due to their size.
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        theorem AVenhance.Infra.Construction.material_aux_velocity_higher_source_step {β C : ℝ} (I : Ingredients β) {Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ} (hΦ : IsStreamSeq I Φ) (hreg : StreamRegularityBounds C I Φ) {Nspace n m : ℕ} {K : ℝ} (hn : 1 ≤ n) (hnN : n ≤ Nstar β) (hlevels : MaterialAuxJetLevels I Φ Nspace K (n - 1)) (hK : 1 ≤ K) (α : List (Fin 2)) (hbudget : α.length + 2 * n + 1 ≤ Nspace) (hm : 1 ≤ m) (i : Fin 2) (z : Section4.AmnrSpace) :
        |Section4.amnrWord (fun (y : Section4.AmnrSpace) => streamVel (Φ (m - 1)) y.1 y.2) (List.map some α) ((Section4.amnrWord (fun (y : Section4.AmnrSpace) => streamVel (Φ m) y.1 y.2) (List.replicate n none) fun (y : Section4.AmnrSpace) => streamVel (Φ m) y.1 y.2 i) - Section4.amnrWord (fun (y : Section4.AmnrSpace) => streamVel (Φ (m - 1)) y.1 y.2) (List.replicate n none) fun (y : Section4.AmnrSpace) => streamVel (Φ (m - 1)) y.1 y.2 i) z| ≤ materialAuxHigherVelocityStepConstant I K Nspace n α.length * epsilon β I.Λ m ^ (β - 1) * (epsilon β I.Λ m)⁻¹ ^ α.length * a β I.Λ m ^ n

        One higher source material order follows from strictly lower velocity and gradient levels plus the all-order transported fast increment.

        theorem AVenhance.Infra.Construction.material_aux_velocity_higher_material_abs_le_of_source_lower_levels {β C : ℝ} (I : Ingredients β) {Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ} (hΦ : IsStreamSeq I Φ) (hreg : StreamRegularityBounds C I Φ) {Nspace n : ℕ} {K : ℝ} (hn : 1 ≤ n) (hnN : n ≤ Nstar β) (hlevels : MaterialAuxJetLevels I Φ Nspace K (n - 1)) (hK : 1 ≤ K) (m : ℕ) (α : List (Fin 2)) (hbudget : α.length + 2 * n + 1 ≤ Nspace) (i : Fin 2) (z : Section4.AmnrSpace) :
        |Section4.amnrWord (fun (y : Section4.AmnrSpace) => streamVel (Φ m) y.1 y.2) (Section4.amnrMixedWord α n) (fun (y : Section4.AmnrSpace) => streamVel (Φ m) y.1 y.2 i) z| ≤ 2 * materialAuxHigherVelocityStepConstant I K Nspace n α.length * epsilon β I.Λ m ^ (β - 1) * (epsilon β I.Λ m)⁻¹ ^ α.length * a β I.Λ m ^ n

        The higher material velocity jets telescope over scales. Their exponent is uniformly negative, so the new constant is independent of the scale.

        The source constant after one auxiliary material induction level.

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          theorem AVenhance.Infra.Construction.material_aux_velocity_advance {β C : ℝ} (I : Ingredients β) {Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ} (hΦ : IsStreamSeq I Φ) (hreg : StreamRegularityBounds C I Φ) {N cut : ℕ} {K : ℝ} (hlevels : MaterialAuxJetLevels I Φ N K cut) (hK : 1 ≤ K) (hcutN : cut + 1 ≤ Nstar β) (m : ℕ) (α : List (Fin 2)) (r : ℕ) (hr : r ≤ cut + 1) (hne : Section4.amnrMixedWord α r ≠ []) (hbudget : α.length + 2 * r + 1 ≤ N) (i : Fin 2) (z : Section4.AmnrSpace) :
          |Section4.amnrWord (fun (y : Section4.AmnrSpace) => streamVel (Φ m) y.1 y.2) (Section4.amnrMixedWord α r) (fun (y : Section4.AmnrSpace) => streamVel (Φ m) y.1 y.2 i) z| ≤ materialAuxVelocityAdvanceConstant I K N cut * epsilon β I.Λ m ^ (β - 1) * (epsilon β I.Λ m)⁻¹ ^ α.length * a β I.Λ m ^ r

          Extend the velocity part of the source invariant through its next material order, summing the actual scale increments.

          noncomputable def AVenhance.Infra.Construction.materialAuxJetAdvanceConstant {β : ℝ} (I : Ingredients β) (K : ℝ) (N cut : ℕ) :

          Advancing one material level closes the gradient estimates from the velocity estimates at that same level and the previous gradient level.

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            theorem AVenhance.Infra.Construction.material_aux_jet_levels_advance {β C : ℝ} (I : Ingredients β) {Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ} (hΦ : IsStreamSeq I Φ) (hreg : StreamRegularityBounds C I Φ) {N cut : ℕ} {K : ℝ} (hlevels : MaterialAuxJetLevels I Φ N K cut) (hK : 1 ≤ K) (hcutN : cut + 1 ≤ Nstar β) :
            ∃ (Knew : ℝ), 1 ≤ Knew ∧ MaterialAuxJetLevels I Φ N Knew (cut + 1)
            theorem AVenhance.Infra.Construction.material_aux_jet_levels_all_orders_of_A3 {β C : ℝ} (I : Ingredients β) {Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ} (hΦ : IsStreamSeq I Φ) (hreg : StreamRegularityBounds C I Φ) :
            ∃ (K : ℝ), 1 ≤ K ∧ MaterialAuxJetLevels I Φ (2 * Nstar β + 1) K (Nstar β)

            The differentiated recursion and the actual stream-regularity spatial estimates give all source word bounds through the paper's material cutoff. The auxiliary word budget is 2*Nstar+1; time derivatives of recursion cutoffs never exceed the literal Nstar.