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EM does not decrease the observed log likelihood

Statement

Assume the Axiom of Choice. Let p(θ,x,z) be a jointly measurable normalized complete-data density as in Latent-variable joint and observed-data factorization, and fix observed data x. Put mθ(x)=∫p(θ,x,z) μ(dz). Let θt and θ satisfy 0<mθt(x),mθ(x)<∞. Define qt(z)=p(θt,x,z)/mθt(x) and qθx(z)=p(θ,x,z)/mθ(x). Assume qtμ≪qθxμ,∫qt(z)(∣log⁡p(θt,x,z)∣+∣log⁡p(θ,x,z)∣) μ(dz)<∞, and D(qtμ∥qθxμ)<∞. Use log⁡0=−∞ and set qt∣log⁡p∣=0 wherever qt=0. Then, with Q(θ∣θt)=∫qt(z)log⁡p(θ,x,z) μ(dz), ℓx(θ)−ℓx(θt)=Q(θ∣θt)−Q(θt∣θt)+D(qtμ∥qθxμ). Consequently, any admissible update with Q(θ∣θt)≥Q(θt∣θt) does not decrease ℓx. An exact M-step has this property when its maximum is attained over an admissible candidate set containing θt. No equality-of-parameter conclusion is asserted when the KL divergence is zero.

Facts & Assumptions

Given: Assume AC, the supplied measurable spaces and density, a fixed observation x, current and candidate parameters with positive finite observed marginals, the stated absolute integrability and support conditions, and finite directional KL divergence.

[A1]

The Axiom of Choice: AC is assumed by the finite-valued Radon–Nikodym representative in the KL definition, the nonnegativity theorem, and uniqueness of Radon–Nikodym densities.

[F1]

Latent-variable joint and observed-data factorization: p is one jointly measurable nonnegative function normalized on every parameter fiber; mθ(x)=∫p(θ,x,z) μ(dz) and qθx=p/mθ(x) is defined only on a positive finite fiber.

[F2]

The observed density is the latent marginal under Tonelli: qt and qθx are probability densities on the positive finite fibers in the statement.

[F3]

The measure with density f relative to μ: q μ is the measure A↦∫Aq dμ.

[F4]

Kullback–Leibler divergence: under AC and P≪Q, the divergence is ∫log⁡r dP for a finite-valued Radon–Nikodym representative r=dP/dQ.

[F5]

Integrating against a density agrees with integrating the product: for nonnegative measurable f,g, ∫g d(fμ)=∫gf dμ.

[F6]

Kullback–Leibler divergence is nonnegative: under AC and the stated directional convention, D(P∥Q)≥0.

[F7]

Expectation-maximization: generalized mode requires nondecreasing Q, and exact mode selects an attained maximizer over an admissible set containing the current iterate.

[F8]

Monotonicity and nonnegative homogeneity of the nonnegative integral: pointwise order and multiplication by a positive finite scalar pass to nonnegative integrals.

[F9]

Every complete ordered field is Archimedean: the positive integers are unbounded in R.

[F10]

A nonnegative integral over a null set vanishes: a nonnegative measurable function integrates to zero over a measurable null set.

[F11]

A sigma-finite signed measure that is absolutely continuous with respect to a sigma-finite positive measure has a unique almost-everywhere density: under AC, a finite absolutely continuous measure has a density unique up to almost-everywhere equality when the positive reference measure is sigma-finite.

Proof

1.1givenF2F3F8F9F10

By [F2] and [F3], P:=qtμ and Q:=qθxμ are probability measures. For u=qt and u=qθx, n1{u=∞}≤u and ∫u dμ=1, so [F8] gives nμ{u=∞}≤1 for every positive integer n; [F9] forces both infinite-value sets to be μ-null. Let N be their union. By [F10], P(N)=Q(N)=0. Also P{qθx=0}=0, since Q{qθx=0}=0 and P≪Q. Finally P{qt=0}=0 by the definition of P. Thus qt and qθx are finite and strictly positive on a P-full set.

2.1givenA1F1F2F4F5F10F11algebra

By [A1] and [F4], choose a finite-valued Radon–Nikodym derivative r=dP/dQ. Define r~=rqθx off N and r~=0 on N, and define q~t=qt off N and q~t=0 on N. These are finite-valued measurable functions. For every measurable A, [F5] and [F10] give ∫Ar~ dμ=∫Arqθx dμ=∫Ar dQ=P(A)=∫Aqt dμ=∫Aq~t dμ. Since μ is sigma-finite and P is finite, a sigma-finite exhaustion for μ is also finite for P. Uniqueness [F11] therefore gives r~=q~t μ-almost everywhere. On the P-full set from step 1.1, r=qt/qθx and log⁡r=log⁡p(θt,x,z)−log⁡mθt(x)−log⁡p(θ,x,z)+log⁡mθ(x). The stated absolute-integrability conditions make these log terms integrable. Integrating this equality with respect to P=qtμ and using [F4] yields D(P∥Q)=Q(θt∣θt)−Q(θ∣θt)+ℓx(θ)−ℓx(θt), which rearranges to the claimed identity.

3.1givenF6F7step 2.1algebra∎

By [F6], the KL term in the identity is nonnegative, so the observed log-likelihood difference is at least the Q difference. A generalized admissible update has nonnegative Q difference by [F7]. An attained exact maximizer over a set containing θt has the same property. Hence either update does not decrease the observed log likelihood.

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