Measurability of the marked excursion measure #
Rational physical times enumerate all passage-jump labels through local time. Keeping the first occurrence of each label yields a measurable sum of Dirac masses.
(J. Bertoin, Lévy Processes, Cambridge University Press, 1996, Chapter IV, Sections 2–4; K. Itô, Poisson point processes attached to Markov processes, Proc. Sixth Berkeley Symp. Math. Statist. Probab. 3 (1972), 225–239.)
Random-measure measurability: the map f ↦ excursionPointMeasure f is AEMeasurable
(into Measure (ℝ≥0 × Excursion) with its Giry/evaluation σ-algebra).
Measurable modification (the measurable field of IsTimeSimpleLevy): there is a
measurable map ξ : DLoc → Measure (ℝ≥0 × Excursion) a.s. equal to excursionPointMeasure.
Box counts are AE-measurable (all measurable boxes/sets).
Past labels are F_{T_a}-measurable (up to a null set): the restriction of μ to labels
≤ a agrees a.s. with an F_{T_a}-measurable random measure
(all those excursions end by T_a).