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Push-Forward Measures and Distribution Functions · Tutorial 227 of 798

Monotonicity, Right Continuity, and Limits of Cumulative Functions

Learn to prove the basic order, continuity, and tail-limit properties of cumulative functions, and to identify why finiteness matters.

Advanced 10 min read

What You'll Learn

  • Define the cumulative function of a finite Borel measure and of a push-forward measure.
  • Prove monotonicity directly from inclusion of half-lines.
  • Derive right continuity using continuity from above for finite measures.
  • Establish the limits at minus and plus infinity, including the zero-mass case.
  • Compute cumulative functions for discrete, continuous, and mixed measures.
  • Recognize how right continuity can fail when the measure is not finite.

What the Cumulative Function Records

A cumulative function records how much measure lies to the left of a moving threshold. Its defining sets are nested as the threshold moves, which gives monotonicity. Right continuity and the limits at the two ends of the real line follow from continuity properties of measures; the finiteness assumption is essential for the right-continuity argument.

Let \(\nu\) be a finite measure on \((\mathbb{R},\mathcal{B}_{\mathbb{R}})\), where finite means \(\nu(\mathbb{R})<\infty\). Write \(M=\nu(\mathbb{R})\), allowing \(M=0\). Define \(F:\mathbb{R}\to[0,M]\) by the measure of the closed half-line ending at \(t\). If \(\nu\) comes from a measurable map \(T:(X,\mathcal{M})\to(\mathbb{R},\mathcal{B}_{\mathbb{R}})\) and a finite measure \(\mu\) on \((X,\mathcal{M})\), its push-forward is \(\nu(B)=\mu(T^{-1}(B))\) for \(B\in\mathcal{B}_{\mathbb{R}}\). In that case the same cumulative function can be computed from the preimage of the half-line.

$$ F(t)=\nu((-\infty,t])=\mu(\{x\in X:T(x)\le t\}),\qquad M=\nu(\mathbb{R})=\mu(X). $$

The equality involving \(T\) is pointwise in \(t\); it follows from the definition of push-forward and the Borel measurability of \((-\infty,t]\). No probability normalization is assumed: \(M\) need not be \(1\). In the results below, statements about a general finite Borel measure \(\nu\) also apply to such a push-forward.

The Measure Continuity Used in the Proof

We will use continuity from below and continuity from above. These are consequences of countable additivity. In the second statement, the finiteness of the first set's measure is required.

Measure continuity: If \((A_n)\) is an increasing sequence of measurable sets in a measure space \((Y,\mathcal{A},\lambda)\), then \(\lambda(\bigcup_n A_n)=\lim_n\lambda(A_n)\), with infinity allowed. If \((A_n)\) is decreasing and \(\lambda(A_1)<\infty\), then \(\lambda(\bigcap_n A_n)=\lim_n\lambda(A_n)\).

Proof. For the increasing sequence, set \(D_1=A_1\) and \(D_n=A_n\setminus A_{n-1}\) for \(n\ge2\). The \(D_n\) are disjoint, \(\bigcup_nD_n=\bigcup_nA_n\), and \(A_N=\bigcup_{n=1}^N D_n\). Countable additivity gives \(\lambda(\bigcup_n A_n)=\sum_{n=1}^{\infty}\lambda(D_n)\), while finite additivity gives \(\lambda(A_N)=\sum_{n=1}^N\lambda(D_n)\). The partial sums increase to the series, proving continuity from below. For the decreasing sequence, the sets \(B_n=A_1\setminus A_n\) increase to \(B=A_1\setminus\bigcap_n A_n\). Since \(\lambda(A_1)<\infty\), subtraction is valid and \(\lambda(A_n)=\lambda(A_1)-\lambda(B_n)\). Continuity from below gives \(\lambda(B_n)\to\lambda(B)\); subtracting from \(\lambda(A_1)\) yields \(\lambda(A_n)\to\lambda(\bigcap_nA_n)\). \(\square\)

Monotonicity, Right Continuity, and Tail Limits

Theorem: Let \(\nu\) be a finite measure on \((\mathbb{R},\mathcal{B}_{\mathbb{R}})\), with \(M=\nu(\mathbb{R})\), and define \(F(t)=\nu((-\infty,t])\) for every real \(t\). Then:
  • \(F\) is nondecreasing: if \(s\le t\), then \(F(s)\le F(t)\).
  • \(F\) is right-continuous at every \(t\in\mathbb{R}\).
  • \(\lim_{t\to-\infty}F(t)=0\) and \(\lim_{t\to+\infty}F(t)=M\).
All these statements concern the defined values of \(F\) at every real number, not just almost everywhere.

Proof. If \(s\le t\), then \((-\infty,s]\subseteq(-\infty,t]\). Monotonicity of the measure therefore gives \(F(s)\le F(t)\).

Fix \(t\in\mathbb{R}\), and let \(t_n=t+1/n\). The sets \((-\infty,t_n]\) decrease, and their intersection is \((-\infty,t]\): a real number \(x\) belongs to every one of them exactly when \(x\le t\). Since \(\nu((-\infty,t_1])\le M<\infty\), continuity from above gives \(F(t_n)\to F(t)\). To verify right continuity for arbitrary thresholds, let \(\varepsilon>0\). Choose \(N\) such that \(F(t+1/N)<F(t)+\varepsilon\), using this sequence limit. Whenever \(t<s<t+1/N\), monotonicity gives \(F(t)\le F(s)\le F(t+1/N)<F(t)+\varepsilon\). Thus \(F(s)\to F(t)\) as \(s\) approaches \(t\) from the right.

For the limit at minus infinity, the sets \((-\infty,-n]\) decrease to the empty set as \(n\to\infty\). Their first member has finite measure, so continuity from above gives \(F(-n)\to\nu(\varnothing)=0\). Given \(\varepsilon>0\), choose \(N\) with \(F(-N)<\varepsilon\). For every \(t\le -N\), monotonicity gives \(0\le F(t)\le F(-N)<\varepsilon\), proving the limit as \(t\to-\infty\).

For the limit at plus infinity, the sets \((-\infty,n]\) increase to \(\mathbb{R}\). Continuity from below gives \(F(n)\to\nu(\mathbb{R})=M\). Given \(\varepsilon>0\), choose \(N\) with \(M-F(N)<\varepsilon\). If \(t\ge N\), then \(F(N)\le F(t)\le M\), so \(0\le M-F(t)\le M-F(N)<\varepsilon\). This proves the limit as \(t\to+\infty\). If \(M=0\), monotonicity and \(0\le F(t)\le M\) give \(F(t)=0\) for every \(t\), and the conclusions hold as well. \(\square\)

Computing the Cumulative Function

Worked Example: A Finite Discrete Measure

Let \(X=\{a,b,c\}\), let \(\mathcal{M}\) be all subsets of \(X\), and assign masses \(\mu(\{a\})=2\), \(\mu(\{b\})=1\), and \(\mu(\{c\})=3\). Define \(T(a)=-1\), \(T(b)=0\), and \(T(c)=2\). Compute the cumulative function of \(\nu=T_{\#}\mu\), where \(T_{\#}\mu(B)=\mu(T^{-1}(B))\).

The total mass is \(\mu(X)=2+1+3=6\). For \(t<-1\), none of the three image points satisfies \(T(x)\le t\), so \(F(t)=0\). For \(-1\le t<0\), only \(a\) is counted, giving \(F(t)=2\). For \(0\le t<2\), both \(a\) and \(b\) are counted, giving \(F(t)=2+1=3\). For \(t\ge2\), all three are counted, giving \(F(t)=2+1+3=6\). Therefore

$$ F(t)= \begin{cases} 0,&t<-1,\\ 2,&-1\le t<0,\\ 3,&0\le t<2,\\ 6,&t\ge2. \end{cases} $$

Check: the values at \(-1,0,2\) are respectively \(2,3,6\), matching the sums of masses with image at most each threshold. The formula is nondecreasing, and at each breakpoint its value agrees with the values immediately to its right. It is \(0\) for all \(t<-1\) and \(6\) for all \(t\ge2\), so its two tail limits are \(0\) and \(6=\mu(X)\).

Worked Example: The Push-Forward of Lebesgue Measure by a Square

Take \((X,\mathcal{M},\mu)=([0,1],\mathcal{L}|_{[0,1]},m)\), the Lebesgue measure restricted to \([0,1]\), and let \(T(x)=x^2\). The measure is finite, with \(\mu(X)=1\). Find \(F(t)=\mu(\{x\in[0,1]:x^2\le t\})\).

If \(t<0\), the inequality \(x^2\le t\) has no solution, so \(F(t)=0\). If \(0\le t\le1\), then \(x\in[0,1]\) and \(x^2\le t\) exactly when \(x\le\sqrt{t}\). The preimage is \([0,\sqrt{t}]\), whose Lebesgue measure is \(\sqrt{t}\). If \(t>1\), every \(x\in[0,1]\) satisfies \(x^2\le t\), so \(F(t)=1\). Thus

$$ F(t)= \begin{cases} 0,&t<0,\\ \sqrt{t},&0\le t\le1,\\ 1,&t>1. \end{cases} $$

Check: at \(t=0\), the preimage is \(\{0\}\), of Lebesgue measure \(0=\sqrt{0}\); at \(t=1\), it is all of \([0,1]\), of measure \(1=\sqrt{1}\). The formula is nondecreasing. As \(t\) decreases to \(0\) from above, \(\sqrt{t}\) tends to \(0=F(0)\); as \(t\) increases to \(1\) from above, \(F(t)=1=F(1)\). Its limits at minus and plus infinity are \(0\) and \(1=\mu(X)\).

Worked Example: A Measure with Both a Point Mass and a Density

On \((\mathbb{R},\mathcal{B}_{\mathbb{R}})\), define \(\nu=2\delta_{-1}+3m|_{[0,1]}\). Here \(\delta_{-1}\) assigns mass \(1\) to a Borel set containing \(-1\) and mass \(0\) otherwise; \(m|_{[0,1]}\) is Lebesgue measure restricted to \([0,1]\). The total mass is \(2+3\cdot1=5\). Compute \(F\).

For \(t<-1\), neither the point mass nor any part of \([0,1]\) is included, so \(F(t)=0\). For \(-1\le t<0\), the point mass contributes \(2\), while the interval contributes \(0\), so \(F(t)=2\). For \(0\le t\le1\), the point mass contributes \(2\), and the interval \([0,t]\) has length \(t\), contributing \(3t\); hence \(F(t)=2+3t\). For \(t>1\), the full point mass and the full interval contribute \(2+3\cdot1=5\). Therefore

$$ F(t)= \begin{cases} 0,&t<-1,\\ 2,&-1\le t<0,\\ 2+3t,&0\le t\le1,\\ 5,&t>1. \end{cases} $$

Check: \(F(-1)=2\), since \(-1\) is included by the condition \(x\le t\); \(F(0)=2+3\cdot0=2\); \(F(1)=2+3\cdot1=5\). The formulas on the right of \(-1,0,1\) approach respectively \(2,2,5\), the values at those points. The function is nondecreasing, and its tail limits are \(0\) and \(5\), equal to the total mass \(2+3=5\).

Why Finiteness Matters

The proof of right continuity used continuity from above for decreasing sets whose first set has finite measure. That condition is not automatic for an infinite measure. For a concrete example, define the Borel measure \(\nu=\sum_{n=1}^{\infty}\delta_{1/n}\), which assigns unit mass to each point \(1/n\). It is not finite: \(\nu(\mathbb{R})=\infty\). At \(t=0\), no point \(1/n\) is at most \(0\), so \(F(0)=0\). For every \(t>0\), infinitely many points \(1/n\) satisfy \(1/n\le t\), so \(F(t)=\infty\). In particular, \(F(1/k)=\infty\) for each positive integer \(k\), although \(1/k\downarrow0\); thus the right limit at \(0\) does not equal \(F(0)\).

A common mistake is to apply continuity from above to a decreasing sequence without checking that its first set has finite measure. For \(A_k=(-\infty,1/k]\) in this example, \(A_k\downarrow(-\infty,0]\), but every \(A_k\) has infinite measure, while the intersection has measure \(0\). The finite-measure hypothesis is exactly what licenses the continuity-from-above step in the theorem.

For a finite measure, the three properties have distinct sources: nested half-lines give monotonicity, decreasing half-lines and finite-measure continuity from above give right continuity, and continuity from below or above gives the two tail limits. The total mass need not be one, but it is always the limit at plus infinity.

Check Your Understanding

Use the definitions and the finite-measure hypotheses to answer each question.

  1. For a finite Borel measure \(\nu\), explain why \(s\le t\) implies \(F(s)\le F(t)\).
  2. In the right-continuity proof, what is the intersection of the sets \((-\infty,t+1/n]\), and where is finiteness used?
  3. If \(\nu(\mathbb{R})=7\), what are the limits of \(F(t)\) as \(t\to-\infty\) and \(t\to+\infty\)?
  4. Let \(\nu=4\delta_2+m|_{[0,1]}\). Compute \(F(0)\), \(F(2)\), and \(\nu(\mathbb{R})\).
  5. For \(\nu=\sum_{n=1}^{\infty}\delta_{1/n}\), compute \(F(0)\) and \(F(1/k)\). Which finite-measure conclusion fails at \(0\)?