Why Boundary Limits Recover Marginals
A joint CDF records probabilities involving two coordinate restrictions at once. A marginal CDF asks about just one coordinate. The connection is simple to state but important to interpret: to retain the restriction on \(X\) while removing the restriction on \(Y\), let the upper bound on \(Y\) grow without limit. Eventually every possible finite value of \(Y\) is included. The remaining probability is exactly the probability that \(X\) is below its specified bound.
This operation does not require independence, a density, or a particular form of dependence. It follows from the definition of a joint CDF and a basic continuity property of probability.
In the first limit, \(b\) increases while \(x\) stays fixed. In the second, \(a\) increases while \(y\) stays fixed. The coordinate being sent to infinity is the restriction being removed; the coordinate held fixed is the one whose marginal distribution remains.
Why the Limits Hold
We prove the first identity; the proof of the second is the same with the roles of \(X\) and \(Y\) exchanged. Fix \(x\), and for each positive integer \(m\) define the event \(A_m=\{X\leq x,\;Y\leq m\}\). These events are increasing: \(A_m\subseteq A_{m+1}\). Their union is \(\{X\leq x\}\), because whenever \(X\leq x\), the real-valued random variable \(Y\) has some finite realized value and therefore \(Y\leq m\) for some sufficiently large integer \(m\).
For completeness, countable additivity implies continuity of probability for increasing events. Set \(D_1=A_1\) and \(D_m=A_m\setminus A_{m-1}\) for \(m\geq2\). The events \(D_m\) are disjoint, \(A_k=\bigcup_{m=1}^kD_m\), and \(\bigcup_{m=1}^{\infty}A_m=\bigcup_{m=1}^{\infty}D_m\). Thus \(P(A_k)=\sum_{m=1}^kP(D_m)\), and countable additivity gives \(\lim_{k\to\infty}P(A_k)=\sum_{m=1}^{\infty}P(D_m)=P(\bigcup_m A_m)\). It follows that \(\lim_{k\to\infty}F(x,k)=P(X\leq x)=F_X(x)\).
Finally, \(F(x,b)\) is nondecreasing in \(b\), since increasing \(b\) enlarges the event in its definition. Its limit as a real \(b\) tends to infinity therefore agrees with its limit along positive integers: for any \(b\) between consecutive integers, the value is bounded by the values at those integers. This proves the first identity for the stated real-variable limit. The same reasoning proves the second. \(\square\)
Worked Examples
Worked Example: Independent Exponential and Uniform Variables
Suppose \(X\sim\operatorname{Exp}(2)\) and \(Y\sim\operatorname{Uniform}(0,3)\) are independent. Here the exponential parameter is the rate. For \(x\geq0\), the CDF of \(X\) is \(1-e^{-2x}\); for \(0\leq y\leq3\), the CDF of \(Y\) is \(y/3\). The joint CDF, using independence, is
Hold \(x\) fixed and let \(y\) increase. If \(x<0\), the joint CDF remains zero. If \(x\geq0\), then for all \(y>3\), it equals \(1-e^{-2x}\). Consequently \(F_X(x)=0\) for \(x<0\) and \(F_X(x)=1-e^{-2x}\) for \(x\geq0\).
To obtain \(F_Y\), hold \(y\) fixed and let \(x\) increase. For \(0\leq y\leq3\), the limit of \((1-e^{-2x})y/3\) as \(x\to\infty\) is \(y/3\), since \(e^{-2x}\to0\). The limit is zero for \(y<0\), and it is one for \(y>3\). Thus the marginal CDFs agree with the stated exponential and uniform distributions.
For a numerical check, take \(x=(\log 2)/2\) and \(y=1.5\). Then \(e^{-2x}=1/2\), so \(F(x,y)=(1/2)(1.5/3)=1/4\). Sending \(y\) above 3 gives \(F_X(x)=1/2\), while sending \(x\) to infinity gives \(F_Y(1.5)=1.5/3=1/2\). The joint value at these finite bounds is not either marginal value.
Worked Example: Marginals in a Dependent Mixture
Let a component be selected with probability \(1/2\). In component 1, \(X\) and \(Y\) are independent exponentials with rates 1 and 2; in component 2, they are independent exponentials with rates 3 and 1. The component selection is shared by both coordinates, so this construction can produce dependence. For nonnegative \(x,y\), its joint CDF is
If \(x<0\) or \(y<0\), the joint CDF is zero. For fixed \(x\geq0\), let \(y\to\infty\). Both exponential terms involving \(y\) tend to zero, so
and \(F_X(x)=0\) for \(x<0\). In the other direction, for fixed \(y\geq0\), let \(x\to\infty\). This gives
with \(F_Y(y)=0\) for \(y<0\). Each marginal is a mixture of exponential distributions; neither marginal requires identifying the component from the observed value of the other coordinate.
The joint value at \(x=y=\log 2\) illustrates the distinction between joint and marginal probabilities. Since \(e^{-x}=1/2\), \(e^{-2y}=1/4\), and \(e^{-3x}=1/8\),
The marginal values are \(F_X(\log2)=\tfrac12(\tfrac12)+\tfrac12(\tfrac78)=\tfrac{11}{16}\) and \(F_Y(\log2)=\tfrac12(\tfrac34)+\tfrac12(\tfrac12)=\tfrac58\). Their product is \(55/128\), which differs from the joint value \(13/32=52/128\). In particular, the joint CDF is not generally the product of its marginal CDFs.
Worked Example: Marginals of a Correlated Normal Pair
Let \(Z_1,Z_2\) be independent standard normal random variables, and set \(X=Z_1\) and \(Y=\rho Z_1+\sqrt{1-\rho^2}Z_2\), where \(-1<\rho<1\). This is a standard construction of a bivariate normal pair. Its joint CDF is \(F(x,y)=P(X\leq x,Y\leq y)\); a closed-form expression for this joint probability is not needed to recover the marginals.
By the boundary-limit theorem, \(F_X(x)=\lim_{y\to\infty}F(x,y)\). Since \(X=Z_1\), this marginal CDF is the standard normal CDF \(\Phi(x)\). Also \(Y\) is a linear combination of independent standard normals with mean zero and variance \(\rho^2+(1-\rho^2)=1\), so \(Y\) is standard normal and \(F_Y(y)=\Phi(y)\). For example, if \(\rho=0.6\), the joint CDF at \((0,0)\) is a probability involving both restrictions; the two marginal CDF values are each \(\Phi(0)=1/2\), regardless of \(\rho\). This shows how the boundary limits identify the coordinate distributions without requiring a formula for the interior of the joint CDF.
Boundary Checks and a Common Pitfall
For any real-valued pair, a joint CDF also has useful zero-boundary limits. For fixed \(x\), as \(y\to-\infty\), the events \(\{X\leq x,Y\leq y\}\) decrease to the empty event: no finite realized value of \(Y\) can be below every real bound. Continuity of probability for decreasing events gives \(\lim_{y\to-\infty}F(x,y)=0\). The decreasing-event property follows from countable additivity by applying continuity for increasing events to complements. Likewise, \(\lim_{x\to-\infty}F(x,y)=0\) for fixed \(y\). At the positive boundaries, the limits are the marginals, not necessarily 1, because the other coordinate's bound remains fixed.
A common mistake is to try to obtain \(F_X(x)\) by evaluating \(F(x,0)\), or by setting the two arguments equal and using \(F(x,x)\). Neither operation removes the condition on \(Y\). For example, in the independent exponential-uniform example, \(F(x,0)=0\), while \(F_X(x)=1-e^{-2x}\) for \(x\geq0\). The correction is to take a limit in the other coordinate: \(F_X(x)=\lim_{y\to\infty}F(x,y)\). Similarly, recover \(F_Y(y)\) by taking \(x\to\infty\), not by choosing an arbitrary finite \(x\).
Check Your Understanding
Use the boundary-limit identities and distinguish each marginal event from a joint event.
- Write \(F_Y(y)\) as a limit of the joint CDF, specifying which argument is held fixed.
- Why does \(\bigcup_{m=1}^{\infty}\{X\leq x,Y\leq m\}=\{X\leq x\}\) hold for real-valued \(Y\)?
- In the independent exponential-uniform example, what is \(F_X(x)\) for \(x\geq0\), and why does taking \(y=1.5\) not remove the restriction on \(Y\)?
- In the mixture example, give the expression for \(F_Y(y)\) when \(y\geq0\).
- For fixed \(x\), what is \(\lim_{y\to-\infty}F(x,y)\), and what event interpretation explains the answer?