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A particle proposal can miss positive target mass

Statement refuted

False claim: The transition support condition Mk(x,⋅)≪Rk(x,⋅) may be dropped while the same proposal-weighted particle measure still represents the Feynman–Kac target.

Facts & Assumptions

Given: The finite model and proposal in the Counterexample.

[F1]

Feynman–Kac path targets and normalizers: The unnormalized path law is the initial/transition path law weighted by the product of the specified potentials.

[F2]

Sequential importance resampling for Feynman–Kac path targets: Particle paths are proposed using Rk and then weighted using the target-to-proposal kernel derivative; the procedure requires the support and derivative hypotheses in its definition.

Counterexample

1.1F1givenalgebra

Let X0={∗} and X1={a,b}. Take μ0=ν0=δ∗, M1(∗,{a})=M1(∗,{b})=1/2, R1(∗,{a})=1, R1(∗,{b})=0, and G0=G1=1. By [F1], γ1 is the transition law itself, Z1=1, and the normalized target assigns mass 1/2 to b.

2.1F2step 1.1given

The support premise fails because M1(∗,{b})=1/2 while R1(∗,{b})=0. A proposal path drawn from Q1=ν0R1 equals (∗,a) with probability one, so every empirical measure formed from such paths assigns mass zero to the event {x1=b}.

3.1step 1.1step 2.1algebra∎

If a kernel derivative r1 represented M1(∗,⋅) with respect to R1(∗,⋅), then M1(∗,{b})=∫{b}r1(∗,y)R1(∗,dy)=0, contradicting the value 1/2. Thus the required importance weight does not exist on this target-positive, proposal-null set, and the false claim fails.

Remarks

The example refutes target coverage after support failure; it does not assert that every numerical normalizer estimate must be biased when support fails.

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