Documentation

LeanPool.NavierStokesAndEuler.Euler.PacketPhysicalFrequencyBounds

A fixed polynomial frequency loss for every actual physical spatial derivative of a reconstructed lifted field.

Physical radius cost, given by sourceInverseRadius C R*(9*C^2*(R + (‖coordinateEquiv.symm.toContinuousLinearMap‖*(1+‖D.m₀‖))*S)+2).

Equations
  • One or more equations did not get rendered due to their size.
Instances For

    Physical fixed cost, given by 3*C*(physicalRadiusCost D R C S)^n*(n.factorial : ℝ)^2.

    Equations
    Instances For
      theorem EulerPacketPhysicalGevrey.physicalReconstruction_power_bound {U : Type u_1} [NormedAddCommGroup U] [InnerProductSpace ℝ U] (D : EulerTransversePacketProvider.Data U) (P κ k : ℝ) (e : ↑(Set.Icc 0 D.T) → EulerLiftedGradientSpace.LiftDomain P → EulerSmoothLimit.Space) (he : ∀ (t : ↑(Set.Icc 0 D.T)) (x : EulerLiftedGradientSpace.LiftDomain P), ContDiff ℝ (↑⊤) (EulerMetricTransport.localFieldLift P (e t) x)) (R C A S : ℝ) (hR : 0 ≤ R) (hC : 0 ≤ C) (hA : 0 ≤ A) (hS : 0 ≤ S) (hF : ∀ (n : ℕ) (t : ↑(Set.Icc 0 D.T)) (x : EulerSmoothLimit.Space), ‖iteratedFDeriv ℝ n (⇑(D.F.field t)) x‖ ≤ C * EulerGevrey.majorant R 0 n) (hb : ∀ (n : ℕ) (t : ↑(Set.Icc 0 D.T)) (x : EulerLiftedGradientSpace.LiftDomain P), ∑ w : Fin n → Fin 4, ‖EulerCylinderSobolev.iteratedFieldDerivative P w (e t) x‖ ≤ A * S ^ n * ↑n.factorial ^ 2) (X Y : ↑(Set.Icc 0 D.T) → EulerSmoothLimit.Space → EulerSmoothLimit.Space) (hX : ∀ (t : ↑(Set.Icc 0 D.T)) (x : EulerSmoothLimit.Space), HasFDerivAt (X t) ((D.F.field t) x) x) (hY : ∀ (t : ↑(Set.Icc 0 D.T)), Differentiable ℝ (Y t)) (hXY : ∀ (t : ↑(Set.Icc 0 D.T)) (x : EulerSmoothLimit.Space), X t (Y t x) = x) (hdet : ∀ (t : ↑(Set.Icc 0 D.T)) (x : EulerSmoothLimit.Space), Matrix.det (EulerPacketPiola.operatorMatrix ((D.F.field t) x)) = 1) (hk : 1 ≤ k) (hκ : |κ| ≤ 1) (n : ℕ) (t : ↑(Set.Icc 0 D.T)) (x : EulerSmoothLimit.Space) :