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Atlas.TheoryOfProbability.code.StrongMarkovBM

def BrownianMotion.stoppedShiftedProcess {Ω : Type u_1} (B : NNRealΩ) (T : ΩENNReal) :
NNRealΩ

The process obtained from B by shifting time by the stopping time T and recentering at B(T): t ↦ B(T + t) - B(T).

Instances For
    theorem strong_markov_property_bm {Ω : Type u_1} {m : MeasurableSpace Ω} {B : NNRealΩ} { : MeasureTheory.Filtration NNReal m} {μ : MeasureTheory.Measure Ω} [MeasureTheory.IsProbabilityMeasure μ] (hB_zero : ∀ᵐ (ω : Ω) μ, B 0 ω = 0) (hB_indep : ∀ (s t : NNReal), s tProbabilityTheory.Indep ( s) (MeasurableSpace.comap (fun (ω : Ω) => B t ω - B s ω) inferInstance) μ) (hB_cont : ∀ᵐ (ω : Ω) μ, Continuous fun (t : NNReal) => B t ω) (T : ΩENNReal) (hT_stop : IsStoppingTimeContinuous T) (hT_fin : ∀ᵐ (ω : Ω) μ, T ω < ) :

    Strong Markov property for Brownian motion (Lecture 39). Given a real-valued Brownian motion B adapted to with B 0 = 0, independent Gaussian increments and continuous paths, and an almost-surely finite stopping time T, the shifted/recentered process t ↦ B(T + t) - B(T) is independent of ℱ_T, starts at 0, has the same Gaussian increment distribution as B, and has continuous paths almost surely.