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Lecture notes. Written from the material of Berkeley Stat 210A, licensed CC BY 4.0. These are notes, not a transcript: the material has been reorganised and rewritten. This adaptation carries the same licence, and the original is linked above.

10. The Factorization Theorem

What this covers

This chapter proves the factorization theorem: a statistic \(T\) is sufficient for \(\theta\) exactly when the density of the data splits into a piece that depends on \(\theta\) only through \(T\), and a piece that does not involve \(\theta\) at all. It assumes the definition of sufficiency — that the conditional distribution of \(X\) given \(T(X)\) does not depend on \(\theta\) — and the basic apparatus of dominated families: a \(\sigma\)-finite dominating measure \(\mu\) and the Radon–Nikodym derivative \(p_\theta = dP_\theta/d\mu\).

Setting and statement

Let \((\mathcal{X}, \mathcal{A})\) be a measurable space and \(\mathcal{P} = \{P_\theta : \theta \in \Theta\}\) a family of probability measures on it. Suppose the whole family is dominated by a single \(\sigma\)-finite measure \(\mu\) — every \(P_\theta\) is absolutely continuous with respect to \(\mu\) — and write \(p_\theta = dP_\theta/d\mu\) for the resulting densities. Dominance is what makes a single function \(p_\theta(x)\) available to factor in the first place; without a common dominating measure there is no shared density to split.

Theorem (Factorization Theorem). A statistic \(T : \mathcal{X} \to \mathcal{Y}\) is sufficient for \(\theta\) if and only if there exist measurable functions $$ u : \mathcal{Y} \times \Theta \to [0,\infty), \qquad v : \mathcal{X} \to [0,\infty) $$ such that, for every \(x \in \mathcal{X}\) and every \(\theta \in \Theta\), $$ p_\theta(x) = u(T(x), \theta)\, v(x). $$

Read the two factors separately. \(u\) is where all the \(\theta\)-dependence is allowed to live, and it may see \(x\) only through \(T(x)\). \(v\) may depend on \(x\) in any way at all, but never on \(\theta\). So the theorem trades sufficiency — a statement about conditional distributions — for a purely algebraic property of the density that is normally far easier to check by inspection: try to peel \(\theta\) out of \(p_\theta(x)\) into a factor that sees \(x\) only through \(T(x)\), leaving a \(\theta\)-free remainder.

Sufficiency implies factorization

Suppose \(T\) is sufficient for \(\theta\). By definition, the conditional distribution of \(X\) given \(T(X) = t\) does not depend on \(\theta\): writing \(k(x \mid t)\) for this common conditional density, it is the same function whether computed under \(P_\theta\) or under any other member of the family.

Let \(f_{T,\theta}(t)\) denote the marginal density of \(T(X)\) under \(P_\theta\). The joint density of \(X\) decomposes as (marginal density of \(T\)) times (conditional density of \(X\) given \(T\)), and the conditional factor does not involve \(\theta\): $$ p_\theta(x) = f_{T,\theta}(t)\, k(x \mid t), \qquad t = T(x). $$ Set \(v(x) = k(x \mid T(x))\) — a function of \(x\) alone, since \(\theta\) never entered it — and \(u(t,\theta) = f_{T,\theta}(t)\). Then \(p_\theta(x) = u(T(x),\theta)\,v(x)\), which is the required factorization.

(The source's own proof pauses at exactly this point to flag a subtlety: the naive discrete computation \(p_\theta(x) = P_\theta(X = x \mid T(X) = t)\, P_\theta(T(X) = t)\) does not literally make sense once \(x\) ranges over a continuum, since \(P_\theta(X = x) = 0\) there. The fix is the passage to densities carried out above, which the proof states rather than re-derives from first principles.)

Factorization implies sufficiency

Now suppose \(p_\theta(x) = u(T(x), \theta)\, v(x)\) for measurable \(u, v\). Fix a measurable set \(B \in \mathcal{A}\) and a value \(t\), and write the conditional probability of \(X \in B\) given \(T(X) = t\) under \(P_\theta\) as a ratio of integrals over the fiber \(T^{-1}(t)\): $$ P_\theta(X \in B \mid T(X) = t) = \frac{\displaystyle\int_{B \cap T^{-1}(t)} p_\theta(x)\, d\mu(x)} {\displaystyle\int_{T^{-1}(t)} p_\theta(x)\, d\mu(x)}. $$ Substitute the factorization. On the fiber \(T^{-1}(t)\) every point \(x\) satisfies \(T(x) = t\), so \(u(T(x),\theta) = u(t,\theta)\) is literally constant over the domain of both integrals and can be pulled outside each: $$ P_\theta(X \in B \mid T(X) = t) = \frac{u(t,\theta)\displaystyle\int_{B \cap T^{-1}(t)} v(x)\, d\mu(x)} {u(t,\theta)\displaystyle\int_{T^{-1}(t)} v(x)\, d\mu(x)} = \frac{\displaystyle\int_{B \cap T^{-1}(t)} v(x)\, d\mu(x)}{\displaystyle\int_{T^{-1}(t)} v(x)\, d\mu(x)}. $$ The \(u(t,\theta)\) factors cancel exactly, top and bottom, leaving an expression built only from \(v\) and the sets \(B \cap T^{-1}(t)\) and \(T^{-1}(t)\) — nothing that depends on \(\theta\). So the conditional distribution of \(X\) given \(T(X) = t\) is the same for every \(\theta\), which is precisely the definition of \(T\) being sufficient for \(\theta\). \(\blacksquare\)

What the two directions are really doing

The two halves of the proof are mirror images of each other. The forward direction takes the definition of sufficiency apart into a marginal-times-conditional decomposition and reads \(u\) and \(v\) straight off the two pieces. The reverse direction runs that decomposition backwards: given any factorization, the factor \(u(T(x),\theta)\) is forced to be constant on each fiber \(T^{-1}(t)\), because it can only see \(x\) through \(T(x)\) — so it always cancels out of the conditional-probability ratio, whatever it actually is, and the only thing left in the ratio is \(v\), which was \(\theta\)-free from the start. That cancellation is the entire mechanism of the theorem: it is why isolating the \(\theta\)-dependence into a single factor depending on \(x\) only through \(T(x)\) is not merely a sufficient condition for sufficiency, but an equivalent one.

Sources

  • Statement and complete proof of the factorization theorem (both directions): factorizationtheorem.md, UC Berkeley STAT 210A, Fall 2024 course reader, licensed CC BY 4.0, converted from factorizationtheorem.tex. No slides, transcript, or exercises were supplied for this chapter, and no other version of this material (from another year's offering of the course) was provided as input.

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