OAI/NumberTheory/DukePrimeDegree/Entropy/CountableFutureMap.lean
8 declarations, 0 contain sorry, 0 declared as axioms
The entire future as a measurable sequence
This representation makes future-measurable events constant on each complete future fiber. It is used to restrict local disintegrations to saturated events when gluing them.
- def
OAI.DukePrimeDegree.entireFutureObservationline 20 - lemma
OAI.DukePrimeDegree.entireFutureObservation_measurableline 23 - lemma
OAI.DukePrimeDegree.countableFutureSigma_eq_comapline 28 - lemma
OAI.DukePrimeDegree.transverseCountableFutureSigma_eq_comapline 35 - lemma
OAI.DukePrimeDegree.countableFutureFiber_eq_of_memline 50 - theorem
OAI.DukePrimeDegree.mem_future_event_iffline 63Source documentation
Every event in the complete transverse-future sigma algebra is constant along its future fibers, with no exceptional set needed.
theorem mem_future_event_iff {S V Y : Type*} [MeasurableSpace S] [MeasurableSpace V] (T : Y → Y) (Q : Y → ℕ) (F : S × V → Y) {E : Set (S × V)} (hE : MeasurableSet[⨆ m, transverseLabelSigma (fun z => countableFutureCode T Q m (F z))] E) (z : S × V) {u : V} (hu : u ∈ countableFutureFiber T Q F z) : (z.1,u) ∈ E ↔ z ∈ E := by …Mentions: OAI.DukePrimeDegree.transverseLabelSigma, OAI.DukePrimeDegree.countableFutureCode, OAI.DukePrimeDegree.countableFutureFiber
- theorem
OAI.DukePrimeDegree.measurable_countableFuture_massline 82Source documentation
Fiber masses of a kernel depending only on the transverse coordinate are measurable in the transverse-future sigma algebra itself. Thus mass conditions used to select boxes really are future events.
theorem measurable_countableFuture_mass {S V Y : Type*} [MeasurableSpace S] [MeasurableSpace V] [MeasurableSpace Y] (κ : Kernel S V) [IsSFiniteKernel κ] {T : Y → Y} (hT : Measurable T) {Q : Y → ℕ} (hQ : Measurable Q) {F : S × V → Y} (hF : Measurable F) (A : Set (S × V)) (hA : MeasurableSet A) : Measurable[⨆ m, transverseLabelSigma (fun z => countableFutureCode T Q m (F z))] (fun z => κ z.1 ({t | (z.1,t) ∈ A} ∩ countableFutureFiber T Q F z)) := by …Mentions: OAI.DukePrimeDegree.transverseLabelSigma, OAI.DukePrimeDegree.countableFutureCode, OAI.DukePrimeDegree.countableFutureFiber
- theorem
OAI.DukePrimeDegree.measurableSet_future_mass_containedline 115Source documentation
The event that a complete future fiber has no mass outside a fixed time domain is measurable using only the transverse coordinate and the future name.
theorem measurableSet_future_mass_contained {S V Y : Type*} [MeasurableSpace S] [MeasurableSpace V] [MeasurableSpace Y] (κ : Kernel S V) [IsSFiniteKernel κ] {T : Y → Y} (hT : Measurable T) {Q : Y → ℕ} (hQ : Measurable Q) {F : S × V → Y} (hF : Measurable F) (B : Set V) (hB : MeasurableSet B) : MeasurableSet[⨆ m, transverseLabelSigma (fun z => countableFutureCode T Q m (F z))] {z | κ z.1 (countableFutureFiber T Q F z \ B) = 0} := by …Mentions: OAI.DukePrimeDegree.transverseLabelSigma, OAI.DukePrimeDegree.countableFutureCode, OAI.DukePrimeDegree.countableFutureFiber