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LeanPool.NavierStokesAndEuler.Euler.TimeLpGramGevrey

Uniform factorial estimates for the actual time Gram inverse #

The lower frame bound and actual coefficient derivatives give the estimates for the inverse appearing in the strong acceleration equation. No derivative bounds on a pre-existing inverse are assumed.

noncomputable def EulerTimeLpGramGevrey.gramCost (c C D : ) :

A polynomial top constant for coefficient amplitude 3 C² and forcing amplitude D.

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Instances For
    theorem EulerTimeLpGramGevrey.gramSolution_contDiff {P : Type u_1} {U : Type u_2} {E : Type u_3} [NormedAddCommGroup P] [NormedSpace P] [NormedAddCommGroup U] [InnerProductSpace U] [CompleteSpace U] [NormedAddCommGroup E] [InnerProductSpace E] [CompleteSpace E] (T : ) (hT : 0 T) (Q : PC((Set.Icc 0 T), U →L[] E)) (c : ) (hc : 0 < c) (hLower : ∀ (x : P) (t : (Set.Icc 0 T)) (v : U), c * v ^ 2 ((Q x) t) v ^ 2) (f : P(EulerTimeLp.TimeLp T U)) {n : WithTop ℕ∞} (hQ : ContDiff n Q) (hf : ContDiff n f) :
    ContDiff n fun (x : P) => (EulerTimeLpGramInverse.gramSolver T hT (Q x) c hc ) (f x)

    The Gram solve is the actual smoothly parameterized coercive solution.

    theorem EulerTimeLpGramGevrey.gramSolution_gevrey {P : Type u_1} {U : Type u_2} {E : Type u_3} [NormedAddCommGroup P] [NormedSpace P] [NormedAddCommGroup U] [InnerProductSpace U] [CompleteSpace U] [NormedAddCommGroup E] [InnerProductSpace E] [CompleteSpace E] (T : ) (hT : 0 T) (Q : PC((Set.Icc 0 T), U →L[] E)) (c : ) (hc : 0 < c) (hLower : ∀ (x : P) (t : (Set.Icc 0 T)) (v : U), c * v ^ 2 ((Q x) t) v ^ 2) (hQ : ContDiff (↑) Q) (Rc C : ) (hRc : 0 Rc) (hC : 0 C) (hbQ : ∀ (n : ) (x : P), iteratedFDeriv n Q x C * EulerGevrey.majorant Rc 0 n) (f : P(EulerTimeLp.TimeLp T U)) (hf : ContDiff (↑) f) (D R : ) (hD : 0 D) (hR : 2 * gramCost c C D * (Rc + 1) R) (d : ) (hbf : ∀ (n : ) (x : P), iteratedFDeriv n f x D * EulerGevrey.majorant R d n) (n : ) (x : P) :
    iteratedFDeriv n (fun (y : P) => (EulerTimeLpGramInverse.gramSolver T hT (Q y) c hc ) (f y)) x EulerGevrey.majorant R (d + 1) n

    One factorial shift for the genuine Gram inverse, with an explicit polynomial radius condition.

    theorem EulerTimeLpGramGevrey.inverseGramMultiplier_gevrey {P : Type u_1} {U : Type u_2} {E : Type u_3} [NormedAddCommGroup P] [NormedSpace P] [NormedAddCommGroup U] [InnerProductSpace U] [CompleteSpace U] [NormedAddCommGroup E] [InnerProductSpace E] [CompleteSpace E] (T : ) (hT : 0 T) (Q : PC((Set.Icc 0 T), U →L[] E)) (c : ) (hc : 0 < c) (hLower : ∀ (x : P) (t : (Set.Icc 0 T)) (v : U), c * v ^ 2 ((Q x) t) v ^ 2) (hQ : ContDiff (↑) Q) (Rc C : ) (hRc : 0 Rc) (hC : 0 C) (hbQ : ∀ (n : ) (x : P), iteratedFDeriv n Q x C * EulerGevrey.majorant Rc 0 n) (f : P(EulerTimeLp.TimeLp T U)) (hf : ContDiff (↑) f) (D R : ) (hD : 0 D) (hR : 2 * gramCost c C D * (Rc + 1) R) (d : ) (hbf : ∀ (n : ) (x : P), iteratedFDeriv n f x D * EulerGevrey.majorant R d n) (n : ) (x : P) :

    The same estimate applies to the explicit inverse-Gram multiplier in the strong equation.