Documentation

LeanPool.NavierStokesAndEuler.Euler.EnergyWordCoordinates

Exact concatenated coordinates connecting energy regularization to the actual external/base Gevrey forcing.

theorem EulerEnergyWordCoordinates.wordAtLevel_word (period : ℝ) [Fact (0 < period)] {s : ℕ} (q n : ℕ) (w : Fin n → Fin 4) (h : n + q ≤ s) (u : ↥(EulerCylinderSobolevSpace.SobolevSpace period s)) {m : ℕ} (hm : m ≤ q) (v : Fin m → Fin 4) :

A derivative of a genuine word-at-level block is the literal concatenated strong derivative.

theorem EulerEnergyWordCoordinates.boundedWordBlock_eq_wordAtLevel (period : ℝ) [Fact (0 < period)] {s : ℕ} (q n : ℕ) (h : q + n ≤ s) (w : Fin n → Fin 4) :

Bounded word blocks and the spatial-estimate word-at-level operator are the same genuine map.

theorem EulerEnergyWordCoordinates.wordAtLevel_comp (period : ℝ) [Fact (0 < period)] {s p q n m : ℕ} (w : Fin n → Fin 4) (v : Fin m → Fin 4) (h : n + q ≤ s) (h' : m + p ≤ q) (u : ↥(EulerCylinderSobolevSpace.SobolevSpace period s)) :

Two actual Sobolev word blocks compose by literal word concatenation.

The total derivative length in one external/base energy component.

Equations
Instances For

    The literal base-then-external concatenated derivative word of an energy component.

    Equations
    Instances For

      Every total energy word stays below the advertised external-plus-base cutoff.

      The actual external/base metric-energy coordinate is exactly its concatenated strong derivative.

      theorem EulerEnergyWordCoordinates.energyValueFamily_eq (period : ℝ) [Fact (0 < period)] {s : ℕ} (q N : ℕ) (hN : N + q ≤ s + 1) (T : ℝ) (u : C(↑(Set.Icc 0 T), ↥(EulerCylinderSobolevSpace.SobolevSpace period (s + 1)))) (I : EulerGevreyMetricComparison.ExternalWord N) (t : ↑(Set.Icc 0 T)) :

      The actual continuous energy family used by regularization is exactly the spatial Gevrey energy family.

      The H¹ concatenated word is exactly the twice-blocked derivative used by the actual top transport.