OAI/Analysis/FiniteFactor/Matrix/Integrals.lean
8 declarations, 0 contain sorry, 0 declared as axioms
- theorem
OAI.FiniteFactor.source_fiber_restrictline 10 - theorem
OAI.FiniteFactor.source_fiber_integralline 17 - theorem
OAI.FiniteFactor.source_fiber_integrableline 25 - theorem
OAI.FiniteFactor.sourceMatrixEntry_measurableline 33 - theorem
OAI.FiniteFactor.sourceMatrixEntry_integrableline 39 - theorem
OAI.FiniteFactor.sourceMatrixEntry_setIntegralline 44 - theorem
OAI.FiniteFactor.sourceVacuumFunctional_matrixIntegralline 53Source documentation
The displayed trace integral is the actual previously proved normal state.
theorem sourceVacuumFunctional_matrixIntegral (H : SourceHilbert SourceCoordinate →L[ℂ] SourceHilbert SourceCoordinate) : sourceVacuumFunctional H = ∫ x, sourceMatrixEntry H 0 0 x ∂sourceBaseMeasure := by …Mentions: OAI.FiniteFactor.SourceHilbert, OAI.FiniteFactor.SourceCoordinate, OAI.FiniteFactor.sourceVacuumFunctional, OAI.FiniteFactor.sourceMatrixEntry, OAI.FiniteFactor.sourceBaseMeasure
- theorem
OAI.FiniteFactor.sourceMatrixEntry_starline 60Source documentation
Adjoint matrix coefficients agree almost everywhere, on the actual source base.
theorem sourceMatrixEntry_star (θ : SourceCoordinate → ℝ) {H : SourceHilbert SourceCoordinate →L[ℂ] SourceHilbert SourceCoordinate} (hH : H ∈ sourceAlgebra θ) (k n : ℤ) : sourceMatrixEntry (star H) k n =ᵐ[sourceBaseMeasure] fun x => star (sourceMatrixEntry H n k x) := by …Mentions: OAI.FiniteFactor.SourceCoordinate, OAI.FiniteFactor.SourceHilbert, OAI.FiniteFactor.sourceAlgebra, OAI.FiniteFactor.sourceMatrixEntry, OAI.FiniteFactor.sourceBaseMeasure