OAI/Analysis/CoulombTransport/CoulombSupportExistence.lean
6 declarations, 0 contain sorry, 0 declared as axioms
- theorem
OAI.Problem356.CoulombSupportExistence.stationary_eqline 17Source documentation
The two explicit conventions for the stationary field coincide.
theorem stationary_eq (a : E3) : StationaryMap.stationary a = stationaryEquation 20 a := by …Mentions: OAI.Problem356.E3, OAI.Problem356.StationaryMap.stationary
- def
OAI.Problem356.CoulombSupportExistence.Dline 28 - def
OAI.Problem356.CoulombSupportExistence.Hline 31 - theorem
OAI.Problem356.CoulombSupportExistence.D_eqline 37 - theorem
OAI.Problem356.CoulombSupportExistence.nonempty_coulombLocalSupportingChartsline 45Source documentation
The actual Coulomb stationary charts admit a local supporting potential with exact equality precisely on the stationary branch.
theorem nonempty_coulombLocalSupportingCharts (k : Fin 3) : Nonempty (LocalSupportingCharts (StationaryMap.jointPotential (axisVector k)) (stationaryEquation 20 (axisVector k)) (axisVector k) (0, -axisVector k)) := by … - theorem
OAI.Problem356.CoulombSupportExistence.nonempty_coulombLocalSupportingCharts_stationaryline 102Source documentation
The supporting charts in the scalar-potential stationary convention.
theorem nonempty_coulombLocalSupportingCharts_stationary (k : Fin 3) : Nonempty (LocalSupportingCharts (StationaryMap.jointPotential (axisVector k)) (StationaryMap.stationary (axisVector k)) (axisVector k) (0, -axisVector k)) := by …Mentions: OAI.Problem356.StationaryMap.jointPotential, OAI.Problem356.StationaryMap.stationary