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LeanPool.CarlsonFunctions.Dirichlet.IntegrationByParts

Integration by parts for regularized Dirichlet integrals #

The normalized positive power x₊ ^ (a - 1) / Gamma a has derivative x₊ ^ (a - 2) / Gamma (a - 1) when 2 < re a, including at zero. Products of these functions give the Dirichlet density in a free-coordinate chart, extended by zero outside the simplex. Mathlib's integration-by-parts theorem on the ambient coordinate space then gives regDirichletIntegral_tangent_ibp without a boundary term. This result uses only the native integral theory.

noncomputable def DirichletTransform.dirichletChartDensity {ι : Type u_1} [Fintype ι] (i : ι) (b : ι → ℂ) (x : { j : ι // j ≠ i } → ℝ) :

The regularized density in a free-coordinate chart, extended by zero.

Equations
Instances For
    theorem DirichletTransform.prod_positiveGammaPower_eq_regDirichletDensity {ι : Type u_1} [Fintype ι] (b : ι → ℂ) (u : ι → ℝ) (hu : ∑ j : ι, u j = 1) :
    theorem DirichletTransform.dirichletChartDensity_mul_eq_indicator {ι : Type u_1} [Fintype ι] (i : ι) (b : ι → ℂ) (f : (ι → ℝ) → ℂ) :
    theorem DirichletTransform.integral_dirichletChartDensity_mul {ι : Type u_1} [Fintype ι] (i : ι) (b : ι → ℂ) (f : (ι → ℝ) → ℂ) :
    theorem DirichletTransform.dirichletChartDensity_lower {ι : Type u_1} [Fintype ι] (i k : ι) (b : ι → ℂ) (x : { j : ι // j ≠ i } → ℝ) :
    theorem DirichletTransform.hasLineDerivAt_dirichletChartDensity {ι : Type u_1} [Fintype ι] (i : ι) (j : { j : ι // j ≠ i }) (b : ι → ℂ) (hb : ∀ (k : ι), 2 < (b k).re) (x : { j : ι // j ≠ i } → ℝ) :
    theorem DirichletTransform.regDirichletIntegral_tangent_ibp {ι : Type u_1} [Fintype ι] (i : ι) (j : { j : ι // j ≠ i }) (b : ι → ℂ) (hb : ∀ (k : ι), 2 < (b k).re) {f : (ι → ℝ) → ℂ} (hf : ∀ u ∈ Convexity.StdSimplex.coordinateSet ℝ ι, DifferentiableAt ℝ f u) (hdf : ContinuousOn (fun (u : ι → ℝ) => (fderiv ℝ f u) (Pi.single (↑j) 1 - Pi.single i 1)) (Convexity.StdSimplex.coordinateSet ℝ ι)) :

    Tangential integration by parts, initially with exponents that vanish differentiably at every boundary face. The Gamma normalization removes the usual exponent coefficients.