OAI/Analysis/Mahler/ExactSphereFluxBridge.lean
3 declarations, 0 contain sorry, 0 declared as axioms
- theorem
OAI.Mahler.coordinateSphereDensity_fluxPullbackline 13Source documentation
The real coordinate cofactor sum is the actual complex sphereFlux density. The volume of the chosen frame is +1, so no orientation or normalization factor remains.
theorem coordinateSphereDensity_fluxPullback {k : ℕ} (B : ComplexEuclidean (k+1) → ComplexEuclidean (k+1) [⋀^Fin (2*k+1)]→L[ℝ] ℂ) (x : Fin ((2*k+1)+1) → ℝ) : MahlerStokes.coordinateSphereDensity 1 (fluxPullback B) x = (orientedDensity (sphereFrame k) (sphereVolume k) (B (fluxCoordinates k x)).toAlternatingMap (fluxCoordinates k x)).re := by …Mentions: OAI.Mahler.ComplexEuclidean, OAI.MahlerStokes.coordinateSphereDensity, OAI.Mahler.fluxPullback, OAI.Mahler.orientedDensity, OAI.Mahler.sphereFrame, OAI.Mahler.sphereVolume, OAI.Mahler.fluxCoordinates
- lemma
OAI.Mahler.continuousOn_fluxPullback_sphereline 36 - theorem
OAI.Mahler.sphereFlux_eq_coordinateFluxline 52Source documentation
The hemisphere-coordinate Stokes flux is exactly Mahler's real flux of a complex form. Only continuity on the sphere is required.
theorem sphereFlux_eq_coordinateFlux {k : ℕ} (B : ComplexEuclidean (k+1) → ComplexEuclidean (k+1) [⋀^Fin (2*k+1)]→L[ℝ] ℂ) (hB : ContinuousOn B (sphere 0 1)) : sphereFlux k (fun x => (B x).toAlternatingMap) = MahlerStokes.sphereFlux 1 (fluxPullback B) := by …Mentions: OAI.Mahler.ComplexEuclidean, OAI.Mahler.sphereFlux, OAI.MahlerStokes.sphereFlux, OAI.Mahler.fluxPullback