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Centered filtering Feynman–Kac operators contract terminal tests

Statement

Let X be a nonempty standard-Borel space with a sigma-finite reference measure λ, and let η0 be a probability on it. For s≥1, supply jointly measurable, strictly positive finite densities gs(z∣x) of probability transition kernels relative to λ, and measurable likelihood factors fs with 0<a≤fs(z)≤b<∞. These specified versions satisfy, for one C≥1 and every s,x,x′,z, gs(z∣x)≤Cgs(z∣x′). Define cs=ηs−1(gsfs), ηs(h)=ηs−1(gs(fsh))/cs, and Esh(x)=gs(fsh)(x)/cs. They are the operators of Finite-horizon SMC CLT classes and variance recursions restricted to last-state tests in the corresponding filtering model. Put ρ=1−C−2. For every bounded measurable real terminal test ψ and 0≤k<t, ∥Ek+1:t(ψ−ηtψ)∥∞≤Cρt−kosc⁡(ψ). For k=t the identity image is bounded by osc⁡(ψ); use ρn=0 for n≥1 when C=1. This is a closed last-state-test assertion, not a contraction of arbitrary functions of the full stored path. Positivity, finiteness and the ratio bounds refer to the supplied pointwise density versions, not to unspecified unrelated null-set versions.

Facts & Assumptions

Given: The specified positive finite density versions, probability transitions, initial probability, uniform row ratio and likelihood bounds, and bounded terminal test in the Statement.

[F1]

Measurability of integration against a kernel: a nonnegative measurable function integrated against a probability kernel has a measurable section integral.

[F2]

Tonelli's theorem for nonnegative measurable functions on a sigma-finite product: nonnegative measurable product integrals equal their iterated integrals.

[F3]

Uniform density ratios bound the Dobrushin coefficient: normalized probability-kernel density rows with ratio at most R have Dobrushin coefficient at most 1−R−1.

[F4]

Dobrushin contraction coefficient for a probability kernel: the coefficient is the supremum event-supremum total-variation distance between two output laws.

[F5]

Layer-cake formulas for random variables: for a nonnegative bounded random variable U≤1, EU=∫01P(U>r)dr.

Proof

1.1F1givenconstructalgebra

Fix k<t. Define Qj,th(x) by iterating the kernels gj+1,…,gt, multiplying by fj+1,…,ft, and evaluating h at the final state. Put Hj,t=Qj,t1 and Ht,t=1. Measurability follows from [F1], while probability normalization and the bounds on fs give at−j≤Hj,t≤bt−j. Comparing the first transition row gives Hj,t(x)≤CHj,t(x′) for j<t. Consequently rk,t:=Hk,t/ηk(Hk,t) is positive, at most C, and has ηk-mean one.

2.1F1F2F3step 1.1constructalgebra

For j=k+1,…,t, set Lj,t(x,dz)=gj(z∣x)fj(z)Hj,t(z)λ(dz)/Hj−1,t(x). The recursion for H shows that these are probability kernels, with strictly positive finite denominators. The ratio of two of their density rows is [gj(z∣x)/gj(z∣x′)][Hj−1,t(x′)/Hj−1,t(x)]≤C2 by step 1.1. Thus [F3] gives δ(Lj,t)≤1−C−2=ρ. Telescoping the H factors in the product kernel Pk,t=Lk+1,t⋯Lt,t gives Pk,th=Qk,th/Hk,t.

3.1F4F5step 2.1constructalgebra

For any probability kernel K and bounded real h of positive oscillation, put u=(h−inf⁡h)/osc⁡(h). Then 0≤u≤1, and [F5] under each output law gives Ku(x)−Ku(x′)=∫01[K(x,{u>r})−K(x′,{u>r})]dr. By [F4], its absolute value is at most δ(K). If the oscillation is zero, K preserves the constant and the same oscillation bound is immediate. Hence osc⁡(Kh)≤δ(K)osc⁡(h). Iterating this inequality along the kernels in step 2.1 gives osc⁡(Pk,th)≤ρt−kosc⁡(h).

4.1F2step 1.1step 2.1step 3.1givenalgebra∎

The filtering recursion and iterated integration [F2] yield ηth=ηk(Qk,th)/ηk(Hk,t) and ∏j=k+1tcj=ηk(Hk,t). Thus Ek+1:th=rk,tPk,th. Take h=ψ−ηtψ. Then ηk(rk,tPk,th)=0, and rk,tηk is a probability by step 1.1. Therefore the global infimum of Pk,th is at most zero and its supremum is at least zero, so its sup norm is at most its oscillation. Step 3.1 bounds this by ρt−kosc⁡(ψ); multiplying by rk,t≤C proves the claim. For k=t, the mean ηtψ lies between inf⁡ψ and sup⁡ψ, giving the identity-case bound.

Source notes

The local proof supplies the normalized future-kernel argument explicitly. The density-ratio hypothesis alone does not compare a target transition to its proposal; the separate variance theorem imposes that additional domination and an initial weight bound. No finite-particle or arbitrary-path time-uniform claim is imported from the source.

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