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06 June 2026 · 5 min read · updated 13 June 2026

Uniform Integrability and the Vitali Theorem

Convergence almost everywhere does not imply convergence in the mean unless mass is prevented from escaping, and uniform integrability is the precise condition that prevents it. We define uniform integrability, characterise it on a finite measure space as boundedness together with uniform absolute continuity, and prove the Vitali convergence theorem that a sequence converging in measure converges in L-one if and only if it is uniformly integrable. This sharpens the dominated convergence theorem and is the hypothesis behind the convergence of martingales in the mean.

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  • Uniform integrability
  • The Vitali convergence theorem
  • Uniform integrability in probability

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  • Uniform integrability1m
  • The Vitali convergence theorem3m
  • Uniform integrability in probability1m

The dominated convergence theorem trades pointwise convergence for convergence in the mean by assuming a single integrable dominator, but the dominator is more than is needed. The exact requirement is that the integral over the region where the functions are large is uniformly small, a condition called uniform integrability, and under it convergence in measure upgrades to convergence in L-one. This post proves the Vitali convergence theorem, the sharp form of dominated convergence, on a finite measure space (Ω,A,μ)(\Omega,\mathcal A,\mu)(Ω,A,μ) with μ(Ω)<∞\mu(\Omega)<\inftyμ(Ω)<∞ [1], [2].

#Uniform integrability

Definition1

A family F⊆L1(μ)\mathcal F\subseteq L^1(\mu)F⊆L1(μ) is uniformly integrable when

lim⁡M→∞sup⁡f∈F∫{∣f∣>M}∣f∣ dμ=0.(1)\lim_{M\to\infty}\sup_{f\in\mathcal F}\int_{\{\abs f>M\}}\abs f\,d\mu=0. \tag{1}M→∞lim​f∈Fsup​∫{∣f∣>M}​∣f∣dμ=0.(1)

A single integrable function is uniformly integrable, since ∫{∣f∣>M}∣f∣→0\int_{\{\abs f>M\}}\abs f\to 0∫{∣f∣>M}​∣f∣→0 as M→∞M\to\inftyM→∞ by dominated convergence, and so is any family dominated by one integrable ggg, because ∫{∣f∣>M}∣f∣≤∫{g>M}g\int_{\{\abs f>M\}} \abs f\le\int_{\{g>M\}}g∫{∣f∣>M}​∣f∣≤∫{g>M}​g. Uniform integrability is exactly the strengthening of this to a uniform bound across the family, and on a finite measure space it has a clean characterisation.

Proposition2

On a finite measure space, F\mathcal FF is uniformly integrable if and only if it is bounded in L1L^1L1 and uniformly absolutely continuous, meaning for every ε>0\varepsilon>0ε>0 there is a δ>0\delta>0δ>0 with ∫A∣f∣ dμ<ε\int_A\abs f\,d\mu<\varepsilon∫A​∣f∣dμ<ε for all f∈Ff\in\mathcal Ff∈F whenever μ(A)<δ\mu(A)<\deltaμ(A)<δ.

Proof

Suppose F\mathcal FF is uniformly integrable and fix ε\varepsilonε. Take MMM with sup⁡f∫{∣f∣>M}∣f∣<ε/2\sup_f\int_{\{\abs f>M\}} \abs f<\varepsilon/2supf​∫{∣f∣>M}​∣f∣<ε/2. Then ∫∣f∣≤Mμ(Ω)+ε/2\int\abs f\le M\mu(\Omega)+\varepsilon/2∫∣f∣≤Mμ(Ω)+ε/2 gives the L1L^1L1 bound, and for any set AAA, ∫A∣f∣≤Mμ(A)+∫{∣f∣>M}∣f∣<Mμ(A)+ε/2\int_A\abs f\le M\mu(A)+\int_{\{\abs f>M\}}\abs f<M\mu(A)+\varepsilon/2∫A​∣f∣≤Mμ(A)+∫{∣f∣>M}​∣f∣<Mμ(A)+ε/2, which is below ε\varepsilonε once μ(A)<δ:=ε/(2M)\mu(A)<\delta:=\varepsilon/(2M)μ(A)<δ:=ε/(2M), the uniform absolute continuity. Conversely, suppose the family is L1L^1L1-bounded by CCC and uniformly absolutely continuous, and fix ε\varepsilonε with its δ\deltaδ. By Markov's inequality, μ({∣f∣>M})≤C/M<δ\mu(\{\abs f>M\})\le C/M<\deltaμ({∣f∣>M})≤C/M<δ once M>C/δM>C/ \deltaM>C/δ, so ∫{∣f∣>M}∣f∣<ε\int_{\{\abs f>M\}}\abs f<\varepsilon∫{∣f∣>M}​∣f∣<ε for all fff by uniform absolute continuity, which is uniform integrability.

#The Vitali convergence theorem

Theorem3

On a finite measure space, let fnf_nfn​ converge to fff in measure. Then fn→ff_n\to ffn​→f in L1L^1L1 if and only if (fn)(f_n)(fn​) is uniformly integrable, and in that case f∈L1f\in L^1f∈L1.

Proof

Suppose (fn)(f_n)(fn​) is uniformly integrable. It is then bounded in L1L^1L1, and since fn→ff_n\to ffn​→f in measure, the Riesz theorem yields a subsequence fnk→ff_{n_k}\to ffnk​​→f almost everywhere. Applying Fatou's lemma along it gives ∫∣f∣≤lim inf⁡k∫∣fnk∣≤sup⁡n∥fn∥1<∞\int\abs f\le\liminf_k\int\abs{f_{n_k}}\le \sup_n\norm{f_n}_1<\infty∫∣f∣≤liminfk​∫∣fnk​​∣≤supn​∥fn​∥1​<∞, so f∈L1f\in L^1f∈L1. Let φM(x)=max⁡(−M,min⁡(M,x))\varphi_M(x)=\max(-M,\min(M,x))φM​(x)=max(−M,min(M,x)) be the truncation at level MMM, which is 111-Lipschitz and satisfies ∣x−φM(x)∣=(∣x∣−M)+≤∣x∣ 1{∣x∣>M}\abs{x-\varphi_M(x)}=(\abs x-M)^+\le\abs x\,\mathbf 1_{\{\abs x>M\}}∣x−φM​(x)∣=(∣x∣−M)+≤∣x∣1{∣x∣>M}​. Split

∫∣fn−f∣≤∫∣fn−φM(fn)∣+∫∣φM(fn)−φM(f)∣+∫∣φM(f)−f∣.(2)\int\abs{f_n-f}\le\int\abs{f_n-\varphi_M(f_n)}+\int\abs{\varphi_M(f_n)-\varphi_M(f)}+\int\abs{\varphi_M(f)- f}. \tag{2}∫∣fn​−f∣≤∫∣fn​−φM​(fn​)∣+∫∣φM​(fn​)−φM​(f)∣+∫∣φM​(f)−f∣.(2)

Given ε>0\varepsilon>0ε>0, uniform integrability and f∈L1f\in L^1f∈L1 provide an MMM with sup⁡n∫{∣fn∣>M}∣fn∣<ε\sup_n\int_{\{\abs{f_n}>M\}} \abs{f_n}<\varepsilonsupn​∫{∣fn​∣>M}​∣fn​∣<ε and ∫{∣f∣>M}∣f∣<ε\int_{\{\abs f>M\}}\abs f<\varepsilon∫{∣f∣>M}​∣f∣<ε, so the first and third terms of Equation (2) are each below ε\varepsilonε for every nnn. The middle term has integrand bounded by 2M2M2M and, because φM\varphi_MφM​ is Lipschitz and fn→ff_n\to ffn​→f in measure, φM(fn)→φM(f)\varphi_M(f_n)\to\varphi_M (f)φM​(fn​)→φM​(f) in measure. Write gn:=∣φM(fn)−φM(f)∣g_n:=\abs{\varphi_M(f_n)-\varphi_M(f)}gn​:=∣φM​(fn​)−φM​(f)∣, so gn→0g_n\to 0gn​→0 in measure with 0≤gn≤2M0\le g_n\le 2M0≤gn​≤2M and the constant 2M2M2M integrable on the finite measure space. The ordinary bounded convergence theorem needs almost-everywhere convergence, so argue through subsequences. Every subsequence of (gn)(g_n)(gn​) has, by the Riesz theorem, a further subsequence converging to 000 almost everywhere, and the ordinary bounded convergence theorem sends ∫gn→0\int g_n\to 0∫gn​→0 along it; since every subsequence of the nonnegative sequence (∫gn)(\int g_n)(∫gn​) thus has a sub-subsequence tending to 000, the full sequence ∫∣φM(fn)−φM(f)∣→0\int\abs{\varphi_M(f_n)-\varphi_M( f)}\to 0∫∣φM​(fn​)−φM​(f)∣→0. Hence lim sup⁡n∫∣fn−f∣≤2ε\limsup_n\int\abs{f_n-f}\le 2\varepsilonlimsupn​∫∣fn​−f∣≤2ε, and ε\varepsilonε being arbitrary, fn→ff_n\to ffn​→f in L1L^1L1.

Conversely, suppose fn→ff_n\to ffn​→f in L1L^1L1. Convergence in measure follows from Markov's inequality, μ({∣fn−f∣>ε})≤∥fn−f∥1/ε→0\mu(\{\abs{f_n-f}>\varepsilon\})\le\norm{f_n-f }_1/\varepsilon\to 0μ({∣fn​−f∣>ε})≤∥fn​−f∥1​/ε→0. For uniform integrability, ∫{∣fn∣>M}∣fn∣≤∫{∣fn∣>M}∣f∣+∥fn−f∥1\int_{\{\abs{f_n}>M\}}\abs{f_n}\le\int_{\{\abs{f_n}>M\}} \abs f+\norm{f_n-f}_1∫{∣fn​∣>M}​∣fn​∣≤∫{∣fn​∣>M}​∣f∣+∥fn​−f∥1​, and the single function fff is uniformly integrable while μ({∣fn∣>M})≤(sup⁡n∥fn∥1)/M→0\mu(\{\abs{f_n}>M\})\le (\sup_n\norm{f_n}_1)/M\to 0μ({∣fn​∣>M})≤(supn​∥fn​∥1​)/M→0 uniformly in nnn. The first term is uniformly small for large MMM by the absolute continuity of ∫∣f∣\int\abs f∫∣f∣, and the second is small once nnn is large. The finitely many remaining fnf_nfn​ are each uniformly integrable on their own, so the whole family is.

The Vitali theorem contains the dominated convergence theorem, since a dominated sequence is uniformly integrable and convergence almost everywhere implies convergence in measure on a finite measure space, but it is strictly stronger, because it replaces the dominator with the weaker tail condition and gives an exact characterisation rather than a mere sufficient condition. The cost is the finiteness of the measure, which the truncation argument uses through the bounded convergence theorem.

#Uniform integrability in probability

On a probability space, where μ\muμ is a probability and integrals are expectations, uniform integrability is the hinge of the convergence theory of martingales. A martingale converges in L1L^1L1 if and only if it is uniformly integrable, the condition that lets the almost-sure limit also be the mean limit. The de la Vallee Poussin criterion makes the condition checkable, since a family with sup⁡f∫Φ(∣f∣) dμ<∞\sup_f\int\Phi(\abs f)\,d\mu<\inftysupf​∫Φ(∣f∣)dμ<∞ for some nonnegative measurable Φ\PhiΦ with Φ(t)/t→∞\Phi(t)/t\to\inftyΦ(t)/t→∞ as t→∞t\to\inftyt→∞, such as Φ(t)=t2\Phi(t)=t^2Φ(t)=t2, is uniformly integrable. On {∣f∣>M}\{\abs f>M\}{∣f∣>M} one has ∣f∣≤Φ(∣f∣)/inf⁡t>M(Φ(t)/t)\abs f\le\Phi(\abs f)/\inf_{t>M}(\Phi(t)/t)∣f∣≤Φ(∣f∣)/inft>M​(Φ(t)/t), so the tail integral is bounded by sup⁡f∫Φ(∣f∣) dμ\sup_f\int\Phi(\abs f)\,d\musupf​∫Φ(∣f∣)dμ divided by a quantity tending to infinity with MMM, hence controlled by the superlinear moment. Uniform integrability is therefore the precise dividing line between the sequences whose limits keep their mass and those that leak it to infinity. It is what turns a limit in distribution into a limit of expectations and what closes a martingale at its terminal value.

[1]
G. B. Folland, Real Analysis: Modern Techniques and Their Applications, 2nd ed. Wiley, 1999.
[2]
P. Billingsley, Probability and Measure, 3rd ed. Wiley, 1995.

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cite
@misc{uniform-integrability,
  author = {Zac Kienzle},
  title  = {Uniform Integrability and the Vitali Theorem},
  year   = {2026},
  month  = {06},
  url    = {https://zackienzle.com/blog/uniform-integrability}
}