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LeanPool.AnomalousDiffusion.AVenhance.Infra.Parabolic.FourierGalerkin.TimeDependentCutoffProduct

Product-space identities for time-dependent Fourier cutoffs #

The modewise weak identities are first regrouped as product-space integrals. This keeps the bounded drift and the vector gradient in their natural Hilbert spaces before the physical-cell representatives are substituted.

@[instance_reducible]

Use normalized Haar measure on the unit circle for periodic integrals.

Equations
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Instances For
    theorem AVenhance.Infra.Parabolic.FourierGalerkin.FrozenDriftProblem.synchronized_limit_spacetimeFourierCutoff_product_identity (P : FrozenDriftProblem) (Uprod : ↥ScalarProductTimeL2) (Gprod : ↥GradientProductTimeL2) {φ : ℝ → Homogenization.Vec 2 → ℝ} (hφ : ContDiff ℝ ↑⊤ fun (p : ℝ × Homogenization.Vec 2) => φ p.1 p.2) (N : ℕ) (hidentity : -∑ j : Fin (RealFourierDimension N), inner ℝ Uprod (scalarProductTestLp (deriv (spacetimeRealFourierCoefficient φ N j)) (realFourierModeL2 N j) ⋯) + ∑ j : Fin (RealFourierDimension N), inner ℝ Gprod (P.weightedDriftProductTestLp (spacetimeRealFourierCoefficient φ N j) N (realFourierUnitCoefficient N j) ⋯) + P.κ * ∑ j : Fin (RealFourierDimension N), inner ℝ Gprod (gradientProductTestLp (spacetimeRealFourierCoefficient φ N j) (realFourierModeGradL2 N j) ⋯) = ∑ j : Fin (RealFourierDimension N), spacetimeRealFourierCoefficient φ N j 0 * inner ℝ P.initialTorusL2 (realFourierModeL2 N j)) :

    The three finite sums in the time-dependent mode identity are the product-space pairings against the value, drift-weighted value, and gradient of one finite Fourier cutoff.