Finite-coordinate simplex integrals #
The last barycentric coordinate is reconstructed from the other coordinates. Separating the last free coordinate gives the one-dimensional slices used by the simplex FTC.
theorem
MeasureTheory.integral_stdSimplex_fin
{n : ℕ}
{E : Type u_1}
[NormedAddCommGroup E]
[NormedSpace ℝ E]
(g : (Fin (n + 1) → ℝ) → E)
:
∫ (u : Fin (n + 1) → ℝ) in Convexity.StdSimplex.coordinateSet ℝ (Fin (n + 1)), g u ∂Measure.stdSimplexMeasure = ∫ (v : Fin n → ℝ) in posSimplexFin n 1, g (finSimplexPoint v)
The standard-simplex integral in the chart omitting its last coordinate.
theorem
MeasureTheory.integral_posSimplexFin_snoc
{n : ℕ}
{E : Type u_1}
[NormedAddCommGroup E]
[NormedSpace ℝ E]
(g : (Fin (n + 1) → ℝ) → E)
(hg : IntegrableOn g (posSimplexFin (n + 1) 1) volume)
:
Fubini with the last free coordinate integrated first.
theorem
MeasureTheory.integral_posSimplexFin_snoc_outer
{n : ℕ}
{E : Type u_1}
[NormedAddCommGroup E]
[NormedSpace ℝ E]
(g : (Fin (n + 1) → ℝ) → E)
(hg : IntegrableOn g (posSimplexFin (n + 1) 1) volume)
:
The same Fubini decomposition, with the separated coordinate integrated last.