OAI/Analysis/FiniteFactor/Sampling/SecondMoment.lean
9 declarations, 0 contain sorry, 0 declared as axioms
- theorem
OAI.FiniteFactor.samplingTransportDensity_boundsline 11 - theorem
OAI.FiniteFactor.samplingTransportDensity_integralline 34 - def
OAI.FiniteFactor.samplingVelocityMeasureline 54 - theorem
OAI.FiniteFactor.samplingVelocity_probabilityline 56 - def
OAI.FiniteFactor.samplingIdealSecondline 62Source documentation
Actual averaged density of the uncut diagonal transport.
def samplingIdealSecond (h s : ℝ) : ℝ := …
- theorem
OAI.FiniteFactor.samplingIdealSecond_boundsline 65 - theorem
OAI.FiniteFactor.samplingIdealSecond_measurableline 96 - theorem
OAI.FiniteFactor.samplingIdealSecond_integralline 101Source documentation
Fubini gives the exact mass identity for the averaged transport density.
theorem samplingIdealSecond_integral (h : ℝ) (hh : 0 < h) (hh1 : h < 1) : (∫ s, samplingIdealSecond h s ∂unitIntervalMeasure) = 1 := by …Mentions: OAI.FiniteFactor.samplingIdealSecond, OAI.FiniteFactor.unitIntervalMeasure
- theorem
OAI.FiniteFactor.samplingIdealSecond_squareline 124Source documentation
The source's quadratic cancellation for the actual averaged uncut transport density. The exact mass-one identity eliminates the linear term.
theorem samplingIdealSecond_square (h : ℝ) (hh : 0 < h) (hh1 : h < 1) : (∫ s, samplingIdealSecond h s^2 ∂unitIntervalMeasure) = 1+(∫ s, (samplingIdealSecond h s-1)^2 ∂unitIntervalMeasure) ∧ (∫ s, samplingIdealSecond h s^2 ∂unitIntervalMeasure) ≤ 1+h^2/(1-h)^2 := by …Mentions: OAI.FiniteFactor.samplingIdealSecond, OAI.FiniteFactor.unitIntervalMeasure