Fatou's Lemma
The convergence theorems of Lebesgue's theory are a hierarchy of bargains. The
Monotone Convergence Theorem lets you swap a limit and an integral — but only if the
functions climb monotonically. Dominated Convergence lets you swap too — but
only if a single integrable function dominates the whole sequence. Both hand you an
equality, and both demand a hypothesis you must go out and verify.
Fatou's Lemma is the member of the family that asks for almost nothing. No
monotonicity. No dominating function. No convergence at all — the sequence need not even have a limit.
The single price of admission is non-negativity: f_n \ge 0.
In exchange for demanding so little, it pays you back with less — not an equality but an
inequality. It is the safety net you can always deploy, the one convergence
result that never asks whether its hypotheses hold, because they almost always do. This page teaches
that one idea: in the limit, mass can only be lost, never gained.
The statement: the integral of the liminf is at most the liminf of the integrals
Let (f_n) be any sequence of non-negative
measurable functions on
a measure space (X, \mathcal{M}, \mu). Then
\int \bigl(\liminf_{n\to\infty} f_n\bigr)\, d\mu \;\le\; \liminf_{n\to\infty} \int f_n \, d\mu.
Read it slowly, because the whole lesson is in the order of operations. On the left we first
take the \liminf of the functions — a pointwise construction that
builds a new function g = \liminf_n f_n — and only then integrate it. On the
right we first integrate each f_n to get a sequence of numbers
\int f_n, and take the \liminf of those.
The claim is that the first quantity can never exceed the second.
Think of \int f_n as the "mass" carried by f_n.
Fatou says that when you pass to the limit, some of that mass may leak away — the
limiting function can hold less than the sequence carried — but no mass is ever
conjured from nowhere. The limit is stingy. It keeps at most what the sequence
brought, and sometimes less.
The proof: two lines, once you have Monotone Convergence
Fatou's Lemma is not proved from scratch — it is a short corollary of the
Monotone Convergence Theorem (MCT). The trick is to unfold the definition of
\liminf into an increasing sequence, exactly the shape MCT wants.
Step 1 — build the running infima. For each n set
g_n \,=\, \inf_{k \ge n} f_k.
Each g_n is non-negative and measurable (a countable infimum of measurable
functions). As n grows we take the infimum over a smaller tail, so
g_n can only rise: g_1 \le g_2 \le g_3 \le \cdots.
And by the very definition of the limit inferior, this increasing sequence climbs to
g_n \,\uparrow\, \liminf_{n\to\infty} f_n.
Step 2 — compare each g_n to the tail. Since
g_n = \inf_{k\ge n} f_k \le f_k for every k \ge n,
monotonicity of the integral gives \int g_n \le \int f_k for all such
k. Taking the infimum over the tail on the right,
\int g_n \;\le\; \inf_{k \ge n} \int f_k.
Step 3 — apply MCT and let n \to \infty. Because
0 \le g_n \uparrow \liminf_n f_n, the Monotone Convergence Theorem lets us
pull the limit through the integral on the left. On the right, the infima
\inf_{k\ge n}\int f_k increase to \liminf_n \int f_n
by definition. Chaining it all together:
\int \liminf_{n} f_n \;=\; \int \lim_{n} g_n \;\overset{\text{MCT}}{=}\; \lim_{n} \int g_n \;\le\; \lim_{n} \Bigl(\inf_{k\ge n} \int f_k\Bigr) \;=\; \liminf_{n} \int f_n.
Two genuine ideas — replace f_n by the running infimum
g_n, then feed the monotone g_n to
MCT — and the lemma falls out. The inequality enters at exactly one place: Step 2, where
g_n throws away everything the tail had above its floor. That
discarded surplus is precisely the mass that can escape.
Why the inequality is real: mass that escapes to infinity
Is the \le ever strict? Emphatically yes — and understanding
how is understanding the lemma. There are two classic escape artists, and both start from the
same trick: keep the area at exactly 1 while pushing the function so that at
every fixed point it eventually vanishes.
The tall spike. On \mathbb{R} with Lebesgue measure, take
f_n = n\,\cdot\,\mathbf{1}_{(0,\,1/n)}, \qquad \int f_n \, d\mu = n \cdot \tfrac1n = 1 \ \text{ for every } n.
The spike grows taller and thinner, always enclosing area 1. But fix any
point x > 0: once n > 1/x the interval
(0, 1/n) no longer contains x, so
f_n(x) = 0 from then on. Hence f_n \to 0 pointwise
and \liminf_n f_n = 0. Now compare the two sides of Fatou:
\int \liminf_{n} f_n = \int 0 = 0 \qquad\text{but}\qquad \liminf_{n} \int f_n = \liminf_{n} 1 = 1.
So Fatou reads 0 \le 1 — strict. The whole unit of mass has
slipped out through the shrinking base; the pointwise limit never sees it. This is why the lemma
cannot be upgraded to an equality in general: here the gap is the entire mass.
The sliding bump. Same phenomenon, escaping the other way — to the right instead of
upward:
f_n = \mathbf{1}_{[n,\,n+1]}, \qquad \int f_n \, d\mu = 1 \ \text{ for every } n.
A unit block of area 1 marching off toward
+\infty. Fix any x: once
n > x the block has moved past it, so again
f_n(x) \to 0, \liminf_n f_n = 0, and
\int \liminf_n f_n = 0 < 1 = \liminf_n \int f_n. The mass has "escaped to
infinity" — carried off to where no fixed point can follow it. Drag the slider below to watch either
escape happen.
What Fatou is good for
A one-directional inequality with no hypotheses sounds weak. In practice it is one of the most-used
tools in analysis, precisely because you can reach for it unconditionally. Three staple uses:
-
It bounds the limit from the sequence. If you know
\int f_n \le M for all n and
f_n \to f pointwise, Fatou instantly gives
\int f = \int \liminf f_n \le \liminf \int f_n \le M. So the limit
function is integrable, with its integral controlled by the uniform bound — no monotonicity or
domination needed to get the bound.
-
It proves the Dominated Convergence Theorem. If
|f_n| \le g with g integrable and
f_n \to f, apply Fatou to the two non-negative sequences
g + f_n \ge 0 and g - f_n \ge 0. The first gives
\int f \le \liminf \int f_n; the second gives
-\int f \le \liminf(-\int f_n) = -\limsup \int f_n, i.e.
\limsup \int f_n \le \int f. Squeeze the two and
\int f_n \to \int f. Fatou is the engine inside DCT.
-
It guarantees finiteness / Fatou for probability. In probability
(\mu a probability measure, f_n = X_n random
variables \ge 0), Fatou reads
\mathbb{E}[\liminf X_n] \le \liminf \mathbb{E}[X_n] — the expected value of
the limiting outcome cannot exceed the limiting expectation. It is the workhorse behind many
almost-sure convergence arguments.
For non-negative measurable f_n \ge 0 on a measure space:
-
Statement:
\displaystyle \int \liminf_{n} f_n \, d\mu \le \liminf_{n} \int f_n \, d\mu
— the integral of the liminf is at most the liminf of the integrals.
-
Hypotheses: only that each f_n is measurable and
f_n \ge 0. No monotonicity, no dominating function, no convergence
required.
-
The inequality can be strict: for
f_n = n\,\mathbf{1}_{(0,1/n)} or
f_n = \mathbf{1}_{[n,n+1]} it reads
0 \le 1 — mass escapes and cannot be recovered.
-
Equality holds under the stronger hypotheses of MCT
(f_n \uparrow f) or DCT
(|f_n| \le g integrable), which upgrade the \le
to an =.
-
Fatou \Rightarrow DCT: apply it to
g \pm f_n to squeeze \int f_n \to \int f.
Picture the three convergence theorems as a nested set of deals. Monotone Convergence
needs f_n \uparrow f. Dominated Convergence relaxes that to
"bounded by an integrable g". Fatou drops even that
and asks only f_n \ge 0 — the weakest hypothesis of the three, and hence the
widest applicability. The trade is honest: with fewer hypotheses you get a weaker conclusion (an
inequality, not an equality). But "weaker conclusion" and "less useful" are not the same thing. Because
Fatou almost never fails to apply, it is often the first thing an analyst tries — a
one-directional bound in hand beats a two-directional equality you cannot invoke. And since Fatou
proves DCT, it sits logically underneath its stronger-looking sibling. The stingy
member holds up the whole family.
A clean mnemonic for the direction: the limit is stingy. When you interchange
\liminf and \int, doing the pointwise limit
first (integrating the \liminf) can only lose you mass, so it lands
on the smaller side. The \le always points from the "limit-first"
quantity to the "integral-first" quantity.
Five traps around Fatou's Lemma:
-
The inequality goes ONE way. It is
\int \liminf f_n \le \liminf \int f_n, never the reverse. Writing
\liminf \int f_n \le \int \liminf f_n is simply false — the tall-spike
example gives 1 \not\le 0.
-
You cannot replace \liminf with \lim in
general. Fatou makes no assumption that \int f_n or
f_n even converges. If the sequence of integrals genuinely oscillates,
only the \liminf is guaranteed on the right. (When
f_n \to f pointwise, the left side is
\int f, but the right side may still need \liminf.)
-
Non-negativity is REQUIRED. Drop f_n \ge 0 and the lemma
can fail: take f_n = -n\,\mathbf{1}_{(0,1/n)}, so each
\int f_n = -1 but \liminf f_n = 0, giving
0 \le -1 — false. Fatou needs a floor to stop mass leaking downward. (A
common fix: a one-sided bound f_n \ge h for an integrable
h also works.)
-
Strict inequality is NORMAL — it is not an error. Finding
\int \liminf f_n < \liminf \int f_n does not mean you slipped up; it means
mass escaped. The equality case is the special one (MCT/DCT), not the default.
-
Don't confuse the two liminfs. The left
\liminf_n f_n is a limit inferior of functions — computed
pointwise, producing a new function. The right \liminf_n \int f_n is a
limit inferior of real numbers. They live in different worlds; the lemma is the bridge
between them.