OAI/Analysis/Mahler/SourceFluxRegularity.lean
12 declarations, 0 contain sorry, 0 declared as axioms
- def
OAI.Mahler.sourceDCOperatorline 15Source documentation
Linear jet operator for the normalization -D(u)(iv)/4.
def sourceDCOperator : (E →L[ℝ] ℂ) →L[ℝ] E [⋀^Fin 1]→L[ℝ] ℂ := …
- lemma
OAI.Mahler.contDiffAt_sourceDCline 20 - lemma
OAI.Mahler.contDiffAt_sourceDDCline 25 - def
OAI.Mahler.continuousWedgePowerline 35Source documentation
The recursive shuffle power as a continuous form.
def continuousWedgePower (a : E [⋀^Fin 2]→L[ℝ] ℂ) : (k : ℕ) → E [⋀^WedgePowerSlots k]→L[ℝ] ℂ | 0 => ContinuousAlternatingMap.constOfIsEmpty ℝ E (Fin 0) 1 | k+1 => continuousWedge a (continuousWedgePower a k) omit [NormedSpace ℂ E] [IsScalarTower ℝ ℂ E] [FiniteDimensional ℝ E] inMentions: OAI.Mahler.WedgePowerSlots, OAI.Mahler.continuousWedge
- lemma
OAI.Mahler.continuousWedgePower_toAlternatingMapline 41 - lemma
OAI.Mahler.contDiffAt_continuousWedgePowerline 48 - def
OAI.Mahler.continuousSourceBoundaryFormline 56 - lemma
OAI.Mahler.continuousSourceBoundaryForm_eqline 61 - lemma
OAI.Mahler.continuousSourceBoundaryForm_applyline 68 - theorem
OAI.Mahler.contDiffAt_sourceBoundaryFormline 74Source documentation
C1 regularity of the whole actual flux form uses C3 of its potential.
theorem contDiffAt_sourceBoundaryForm {u : E → ℂ} {x : E} (hu : ContDiffAt ℝ 3 u x) (k : ℕ) : ContDiffAt ℝ 1 (continuousSourceBoundaryForm u k) x := by …Mentions: OAI.Mahler.continuousSourceBoundaryForm
- theorem
OAI.Mahler.MassHypotheses.contDiffOn_energyBoundaryFormline 85 - theorem
OAI.Mahler.MassHypotheses.contDiffOn_logBoundaryFormline 90