From Events to Test Functions
Conditional expectation is defined by testing against events in the conditioning sigma-algebra. This event-by-event definition is precise, but it can be cumbersome: in applications, the quantity being tested is often a bounded measurable random variable rather than an indicator.
The key fact is that the event identity already contains all the bounded tests. Indicators give the identity for simple functions by finite linearity, and bounded measurable functions can be uniformly approximated by simple functions. Integrability makes the resulting passage to the limit valid.
The Defining Identity
Let \((\Omega,\mathcal F,\mathbb P)\) be a probability space, let \(\mathcal G\subseteq\mathcal F\) be a sigma-algebra, and let \(X\) be an integrable real-valued random variable. A conditional expectation of \(X\) given \(\mathcal G\) is an integrable, \(\mathcal G\)-measurable random variable \(Y\) such that
Here \(\mathbf 1_A\) denotes the indicator of \(A\). The event identity is meaningful because both \(X\) and \(Y\) are integrable. We will show that it implies an identity for every bounded, real-valued, \(\mathcal G\)-measurable test random variable \(Z\).
If \(S\) is such a simple test, the event identity immediately gives
All terms are finite: \(S\) is bounded, and \(X,Y\) are integrable. The important step is extending this calculation beyond simple tests.
The Bounded-Test Theorem
The proof uses two separate facts. Simple tests reduce the claim to a finite sum of event identities. Uniform approximation then controls the error by an integrable quantity, namely \(|X|\) or \(|Y|\). No exchange of an uncontrolled limit with expectation is needed.
Continuity in the Test Function
The same estimates give a useful quantitative statement. For a bounded test \(Z\), each of the maps \(Z\mapsto\mathbb E[XZ]\) and \(Z\mapsto\mathbb E[YZ]\) changes continuously when the test changes in uniform size.
where \(\|Z-W\|_\infty\) may be taken as any bound for \(|Z-W|\) outside a null set.
The proof applies with \(Y\) in place of \(X\) as well. This continuity estimate explains why a uniform approximation is especially convenient: the approximation error is multiplied only by a finite first absolute moment.
Worked Example: Symmetry and Conditioning on Absolute Value
Worked Example: Symmetry and Conditioning on Absolute Value
Let \(\Omega=[-1,1]\) with the uniform probability distribution, let \(X(x)=x\), and let \(\mathcal G=\sigma(|X|)\). We claim that \(Y=0\) is a version of \(\mathbb E[X\mid\mathcal G]\).
Every set \(A\in\mathcal G\) is symmetric about zero: membership in \(A\) depends only on \(|x|\), so \(x\in A\) if and only if \(-x\in A\). The density is \(1/2\), and a change of variable \(x\mapsto -x\) gives
Thus \(\mathbb E[X\mathbf 1_A]=0=\mathbb E[Y\mathbf 1_A]\) for every \(A\in\mathcal G\). The candidate \(Y=0\) is integrable and \(\mathcal G\)-measurable, so it is a conditional expectation. The theorem now gives \(\mathbb E[XZ]=0\) for every bounded \(\mathcal G\)-measurable test \(Z\). For instance, \(Z=1+|X|\) is such a test, and direct symmetry also yields
Worked Example: A Test Depending on One Coordinate
Worked Example: A Test Depending on One Coordinate
Let \(U\) and \(V\) be the coordinate functions on the unit square \([0,1]^2\) with uniform probability measure. Set \(X=U+V\), and let \(\mathcal G=\sigma(U)\). We check that \(Y=U+\tfrac12\) is a conditional expectation.
For any \(A\in\mathcal G\), there is a Borel set \(B\subseteq[0,1]\) such that \(A=\{U\in B\}\). Fubini's theorem gives
The candidate \(Y\) is \(\mathcal G\)-measurable and integrable, so the event identity verifies the claim. To see the bounded-test version explicitly, choose \(Z=U^2\). Then
while
The theorem gives the same equality for every bounded measurable function of \(U\), not only for this particular choice \(U^2\).
Worked Example: An Independent Integrable Factor
Worked Example: An Independent Integrable Factor
Let \(U\) be uniform on \([0,1]\), let \(V\) be an independent exponential random variable with density \(e^{-v}\) for \(v\ge0\), and set \(X=UV\). Let \(\mathcal G=\sigma(U)\). Since \(V\) is nonnegative and has mean
the random variable \(X\) is integrable. We claim that \(Y=U\) is a conditional expectation of \(X\) given \(\mathcal G\).
For \(A=\{U\in B\}\in\mathcal G\), independence gives
Now take the bounded \(\mathcal G\)-measurable test \(Z=1/(1+U)\). Since \(u/(1+u)=1-1/(1+u)\), direct integration gives
For the candidate \(Y\), the same calculation yields
This illustrates how the test identity can be used with a non-indicator function that directly matches the quantity in an application.
Why Boundedness Matters Here
Boundedness ensures that \(XZ\) and \(YZ\) are integrable whenever \(X\) and \(Y\) are integrable. It also provides the error estimates that make the simple-function approximation argument work. For example, if \(|Z|\le C\), then \(|XZ|\le C|X|\), whose expectation is finite.
For an unbounded \(\mathcal G\)-measurable test, the products \(XZ\) and \(YZ\) need not be integrable. Even when they are, uniform approximation by bounded simple functions is no longer available in the same form. Thus the theorem makes a specific claim about bounded tests; extending it to an unbounded test requires additional integrability conditions and a separate justification.
The practical lesson is to choose the test class deliberately. When the test is bounded and measurable with respect to the conditioning sigma-algebra, the event definition supplies the desired identity automatically. The proof is not an extra assumption about conditional expectation; it is a consequence of the defining event identities and integrability.
Check Your Understanding
Use the event identity and the approximation argument to answer these questions.
- Why does the defining identity hold for every simple \(\mathcal G\)-measurable test once it holds for indicators of events in \(\mathcal G\)?
- How does the quantized approximation \(S_n=2^{-n}\lfloor 2^nZ\rfloor\) control the error in \(\mathbb E[XZ]\)?
- Which hypotheses ensure that both \(\mathbb E[XZ]\) and \(\mathbb E[YZ]\) are finite for a bounded test \(Z\)?
- How does choosing \(Z=\mathbf 1_A\) prove the converse direction of the bounded-test theorem?
- Why does the proof not automatically establish the same identity for every unbounded \(\mathcal G\)-measurable test?