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Ordinary importance sampling is unbiased

Statement

Let (X,X,μ) be a measure space, let p~≥0 and q≥0 be measurable densities with Zp=∫p~ dμ∈(0,∞) and ∫q dμ=1, and set π(dx)=p~(x)μ(dx)/Zp and Q(dx)=q(x)μ(dx). Let f:X→R be measurable with ∫∣f∣p~ dμ<∞. Suppose q>0 μ-almost everywhere on {fp~≠0} and X1,…,Xn are IID with law Q. For the ordinary importance sampling estimator in Ordinary importance sampling, EQ[μ^IS]=∫f dπ.

Facts & Assumptions

Given: The densities, integrability, support, and IID sampling hypotheses in the Statement.

[F1]

Ordinary importance sampling: With Yi=f(Xi)p~(Xi)/(Zpq(Xi)) when q(Xi)>0 and Yi=0 otherwise, the estimator is μ^IS=n−1∑i=1nYi.

[F2]

Change of variables for expectation: For a random element X with law Q, a nonnegative measurable g satisfies E[g(X)]=∫g dQ, possibly with value +∞; if g(X) is integrable, the same identity holds as a finite integral.

[F3]

The Lebesgue integral is linear on L1(μ): The Lebesgue integral is linear on integrable functions; in particular, the expectation of a finite average of integrable random variables is the average of their expectations.

[F4]

Expectation of a nonnegative or integrable random variable: The expectation of an integrable real random variable is its finite Lebesgue integral.

[F5]

Integrating against a density agrees with integrating the product: for a nonnegative measurable density r and nonnegative measurable h, ∫h d(r dμ)=∫hr dμ, including infinite values. Integrable real and complex functions, and their integrals: an absolutely integrable real function has integral equal to the finite difference of the integrals of its positive and negative parts.

Proof

Given: Use the target expectation θ:=∫f dπ and the estimator specified in Ordinary importance sampling.

1.1givenF1F2F4algebraF5

Use [F5] with density r=q for integration against Q and with r=p~/Zp for integration against π. For every i, apply the nonnegative case of [F2] to ∣Yi∣. Since Xi has law Q, EQ∣Yi∣=∫{q>0}∣f(x)∣p~(x)Zpq(x)q(x) dμ(x)=1Zp∫{q>0}∣f∣p~ dμ≤1Zp∫X∣f∣p~ dμ<∞. Thus Yi is Q-integrable. For any real measurable h whose absolute integral is finite against r dμ, apply [F5] separately to h+=max⁡(h,0) and h−=max⁡(−h,0): both product integrals are finite because h±≤∣h∣. Subtracting their finite identities yields ∫h d(r dμ)=∫hr dμ, since (hr)±=h±r for r≥0 (with the density convention 0⋅∞=0). The integrable case of [F2] therefore gives EQ[Yi]=∫{q>0}f(x)p~(x)Zpq(x)q(x) dμ(x)=1Zp∫{q>0}fp~ dμ. The support condition makes fp~=0 μ-almost everywhere on {q=0}; hence this last integral equals Zp−1∫Xfp~ dμ=∫f dπ=θ.

2.1F1F3F4step 1.1algebra∎

By [F1], μ^IS=n−1∑i=1nYi. Apply [F3] and step 1.1 to obtain EQ[μ^IS]=n−1∑i=1nEQ[Yi]=θ.

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