Densities, masses, and parameter measurability of exponentially tilted measures #
Mathlib's MeasureTheory.Measure.tilted sends a measure μ and a potential f to the normalized
measure (∫ exp f ∂μ)⁻¹ • exp f • μ. This file adds the facts used to identify tilted
members of concrete families of distributions.
MeasureTheory.Measure.map_tiltedtransports a tilt by a statistic on the target through a measurable pushforward.TauCeti.tilted_withDensity: tilting a measure with densitygmultipliesgby the normalized weight, so a tilted law with a density again has an explicit density.TauCeti.tilted_singleton: the mass of a singleton under a tilted measure, which identifies tilted laws on countable spaces;TauCeti.tilted_diracrecords that point masses are fixed.TauCeti.measurable_tiltedandTauCeti.measurable_tilted_mul: a jointly measurable family of potentials tilts an s-finite kernel into a measurable family of measures. For any measureμ(s-finite or not),t ↦ μ.tilted (t * X ·)is measurable for the Giry measurable structure.
Tilting a measure with density g multiplies the density by the normalized exponential
weight.
The mass of a singleton under an exponentially tilted measure.
A point mass is unchanged by every tilt.
Parameter measurability of tilting. Tilting the members of an s-finite kernel by a jointly measurable family of potentials gives a measurable family of measures.
The exponential tilts μ.tilted (t * X ·) of a measure along a measurable statistic form a
measurable family in the tilting parameter t. If μ is not s-finite, then no exp (t * X ·) is
integrable (a positive integrable density would make μ s-finite), so every tilt vanishes.
Pushing an exponential tilt forward commutes with tilting by a statistic on the target.