OAI/MeasureTheory/DyadicAvoidance/ExposureMoments.lean
3 declarations, 0 contain sorry, 0 declared as axioms
- theorem
OAI.Problem310.ExposureMoments.map_restrict_eq_smul_of_fibersline 13Source documentation
Joint masses of complete finite/countable patterns determine the law after restriction to an exposure event. No division by the mass of the event is needed.
theorem map_restrict_eq_smul_of_fibers {A : Type u_A} {V : Type u_V} [MeasurableSpace A] [MeasurableSpace V] [Countable V] [MeasurableSingletonClass V] (μ : Measure A) (ν : Measure V) (E : Set A) (f : A → V) (hf : Measurable f) (hjoint : ∀ v, μ (E ∩ {a | f a = v}) = μ E * ν {v}) : Measure.map f (μ.restrict E) = μ E • ν := by … - theorem
OAI.Problem310.ExposureMoments.lintegral_restrict_comp_of_fibersline 30Source documentation
The exposure factorization extends from pattern events to every nonnegative function of the fresh pattern, including the active-test generating function.
theorem lintegral_restrict_comp_of_fibers {A : Type u_A} {V : Type u_V} [MeasurableSpace A] [MeasurableSpace V] [Countable V] [MeasurableSingletonClass V] (μ : Measure A) (ν : Measure V) (E : Set A) (f : A → V) (hf : Measurable f) (hjoint : ∀ v, μ (E ∩ {a | f a = v}) = μ E * ν {v}) (g : V → ENNReal) (hg : Measurable g) : (∫⁻ a in E, g (f a) ∂μ) = μ E * ∫⁻ v, g v ∂ν := by … - theorem
OAI.Problem310.ExposureMoments.lintegral_restrict_comp_eq_of_fibersline 44Source documentation
A supplied fresh-pattern moment can be used unchanged after center exposure.
theorem lintegral_restrict_comp_eq_of_fibers {A : Type u_A} {V : Type u_V} [MeasurableSpace A] [MeasurableSpace V] [Countable V] [MeasurableSingletonClass V] (μ : Measure A) (ν : Measure V) (E : Set A) (f : A → V) (hf : Measurable f) (hjoint : ∀ v, μ (E ∩ {a | f a = v}) = μ E * ν {v}) (g : V → ENNReal) (hg : Measurable g) (q : ENNReal) (hmoment : (∫⁻ v, g v ∂ν) = q) : (∫⁻ a in E, g (f a) ∂μ) = μ E * q := by …