Radon-Nikodym derivative and Lebesgue decomposition for kernels #
Let γ be a countably generated measurable space and κ, η : kernel α γ be finite kernels.
Then there exists a function kernel.rnDeriv κ η : α → γ → ℝ≥0∞ jointly measurable on α × γ
and a kernel kernel.singularPart κ η : kernel α γ such that
κ = kernel.withDensity η (kernel.rnDeriv κ η) + kernel.singularPart κ η,- for all
a : α,kernel.singularPart κ η a ⟂ₘ η a, - for all
a : α,kernel.singularPart κ η a = 0 ↔ κ a ≪ η a, - for all
a : α,kernel.withDensity η (kernel.rnDeriv κ η) a = 0 ↔ κ a ⟂ₘ η a.
Furthermore, the sets {a | κ a ≪ η a} and {a | κ a ⟂ₘ η a} are measurable.
The construction of the derivative starts from kernel.density: for two finite kernels
κ' : kernel α (γ × β) and η' : kernel α γ with fst κ' ≤ η', the function
density κ' η' : α → γ → Set β → ℝ is jointly measurable in the first two arguments and satisfies
that for all a : α and all measurable sets s : Set β and A : Set γ,
∫ x in A, density κ' η' a x s ∂(η' a) = (κ' a (A ×ˢ s)).toReal.
We use that definition for β = Unit and κ' = map κ (fun a ↦ (a, ())). We can't choose η' = η
in general because we might not have κ ≤ η, but if we could, we would get a measurable function
f with the property κ = withDensity η f, which is the decomposition we want for κ ≤ η.
To circumvent that difficulty, we take η' = κ + η and thus define rnDerivAux κ η.
Finally, rnDeriv κ η a x is given by
ENNReal.ofReal (rnDerivAux κ (κ + η) a x) / ENNReal.ofReal (1 - rnDerivAux κ (κ + η) a x).
Up to some conversions between ℝ and ℝ≥0, the singular part is
withDensity (κ + η) (rnDerivAux κ (κ + η) - (1 - rnDerivAux κ (κ + η)) * rnDeriv κ η).
The countably generated measurable space assumption is not needed to have a decomposition for
measures, but the additional difficulty with kernels is to obtain joint measurability of the
derivative. This is why we can't simply define rnDeriv κ η by a ↦ (κ a).rnDeriv (ν a)
everywhere (although rnDeriv κ η has that value almost everywhere). See the construction of
kernel.density for details on how the countably generated hypothesis is used.
Main definitions #
ProbabilityTheory.kernel.rnDeriv: a functionα → γ → ℝ≥0∞jointly measurable onα × γProbabilityTheory.kernel.singularPart: akernel α γ
Main statements #
ProbabilityTheory.kernel.mutuallySingular_singularPart: for alla : α,kernel.singularPart κ η a ⟂ₘ η aProbabilityTheory.kernel.rnDeriv_add_singularPart:kernel.withDensity η (kernel.rnDeriv κ η) + kernel.singularPart κ η = κProbabilityTheory.kernel.measurableSet_absolutelyContinuous: the set{a | κ a ≪ η a}is MeasurableProbabilityTheory.kernel.measurableSet_mutuallySingular: the set{a | κ a ⟂ₘ η a}is Measurable
References #
Theorem 1.28 in [O. Kallenberg, Random Measures, Theory and Applications][kallenberg2017].
TODO #
- prove uniqueness results.
- link kernel Radon-Nikodym derivative and Radon-Nikodym derivative of measures, and similarly for singular parts.
Auxiliary function used to define ProbabilityTheory.kernel.rnDeriv and
ProbabilityTheory.kernel.singularPart.
This has the properties we want for a Radon-Nikodym derivative only if κ ≪ ν. The definition of
rnDeriv κ η will be built from rnDerivAux κ (κ + η).
Equations
- ProbabilityTheory.kernel.rnDerivAux κ η a x = ProbabilityTheory.kernel.density (ProbabilityTheory.kernel.map κ (fun (a : γ) => (a, ())) ⋯) η a x Set.univ
Instances For
A set of points in α × γ related to the absolute continuity / mutual singularity of
κ and η.
Equations
- ProbabilityTheory.kernel.mutuallySingularSet κ η = {p : α × γ | ProbabilityTheory.kernel.rnDerivAux κ (κ + η) p.1 p.2 = 1}
Instances For
A set of points in α × γ related to the absolute continuity / mutual singularity of
κ and η. That is,
withDensity η (rnDeriv κ η) a (mutuallySingularSetSlice κ η a) = 0,singularPart κ η a (mutuallySingularSetSlice κ η a)ᶜ = 0.
Equations
- ProbabilityTheory.kernel.mutuallySingularSetSlice κ η a = {x : γ | ProbabilityTheory.kernel.rnDerivAux κ (κ + η) a x = 1}
Instances For
Radon-Nikodym derivative of the kernel κ with respect to the kernel η.
Instances For
Singular part of the kernel κ with respect to the kernel η.
Instances For
The singular part of κ with respect to η is mutually singular with η.
Lebesgue decomposition of a finite kernel κ with respect to another one η.
κ is the sum of an abolutely continuous part withDensity η (rnDeriv κ η) and a singular part
singularPart κ η.
The set of points a : α such that κ a ≪ η a is measurable.
The set of points a : α such that κ a ⟂ₘ η a is measurable.