OAI/MathematicalPhysics/NavierStokes/ForcedComputation/Scalar/PlaneHeatLaplacian.lean

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5 declarations, 0 contain sorry, 0 declared as axioms

Cartesian integration by parts for the Euclidean Gaussian.

  1. theorem OAI.ForcedComputation.PlaneHeat.integral_cartesian line 14
  2. theorem OAI.ForcedComputation.PlaneHeat.integral_cartesian_symm line 23
  3. theorem OAI.ForcedComputation.PlaneHeat.product_data_integrable line 32
  4. theorem OAI.ForcedComputation.PlaneHeat.integral_second_one line 40

    Source documentation

    Integration by parts in the second Cartesian coordinate; hypotheses refer to the actual one-variable slices of the data.

    theorem integral_second_one {t : ℝ} (ht : 0 < t) {f f' f'' : Plane → F}
        (hf : Continuous f) (hf'' : Continuous f'')
        (hd : ∀ r s, HasDerivAt (fun y => f ![r,y]) (f' ![r,s]) s)
        (hdd : ∀ r s, HasDerivAt (fun y => f' ![r,y]) (f'' ![r,s]) s)
        (C D E : ℝ) (hC : ∀ x, ‖f x‖ ≤ C) (hD : ∀ x, ‖f' x‖ ≤ D)
        (hE : ∀ x, ‖f'' x‖ ≤ E) :
        (∫ x : Plane, (oneDim t (x 0) * oneDimSecond t (x 1)) • f x) =
          ∫ x : Plane, kernel t x • f'' x := by
    …

    Mentions: OAI.ForcedComputation.PlaneHeat.oneDim, OAI.ForcedComputation.PlaneHeat.oneDimSecond, OAI.ForcedComputation.PlaneHeat.kernel

  5. theorem OAI.ForcedComputation.PlaneHeat.integral_second_zero line 64