In mathematics, the Lebesgue differentiation theorem is a theorem of real analysis, which states that for almost every point, the value of an integrable function is the limiting average taken around the point. The theorem is named for Henri Lebesgue.
For a Lebesgue integrable real or complex-valued function f on Rn, the indefinite integral is a set function which maps a measurable set A to the Lebesgue integral of
f ⋅ 1A
1A
The derivative of this integral at x is defined to be
A more general version also holds. One may replace the balls B  by a family
l{V}
|U|\gec|B|
l{V}
The family of cubes is an example of such a family
l{V}
l{V}
The one-dimensional case was proved earlier by . If f is integrable on the real line, the functionis almost everywhere differentiable, with
F'(x)=f(x).
F
The theorem in its stronger form—that almost every point is a Lebesgue point of a locally integrable function f—can be proved as a consequence of the weak - L1 estimates for the Hardy–Littlewood maximal function. The proof below follows the standard treatment that can be found in,, and .
Since the statement is local in character, f can be assumed to be zero outside some ball of finite radius and hence integrable. It is then sufficient to prove that the set
E\alpha=l\{x\inRn:\limsup|B| →
1 | |
|B| |
|\intBf(y)-f(x)dy|>2\alphar\}
Let ε > 0 be given. Using the density of continuous functions of compact support in L1(Rn), one can find such a function g satisfying
\|f-
g\| | |
L1 |
=
\int | |
Rn |
|f(x)-g(x)|dx<\varepsilon.
1 | |
|B| |
\intBf(y)dy-f(x)=l(
1 | |
|B| |
\intBl(f(y)-g(y)r)dyr)+l(
1 | |
|B| |
\intBg(y)dy-g(x)r)+l(g(x)-f(x)r).
(f-g)*(x)
1 | |
|B| |
\intB|f(y)-g(y)|dy\leq\supr>0
1 | |
|Br(x)| |
\int | |
Br(x) |
|f(y)-g(y)|dy=(f-g)*(x).
l|\left\{x:(f-g)*(x)>\alpha\right\}r|\leq
An | |
\alpha |
\|f-
g\| | |
L1 |
<
An | |
\alpha |
\varepsilon,
l|\left\{x:|f(x)-g(x)|>\alpha\right\}r|\leq
1 | |
\alpha |
\|f-
g\| | |
L1 |
<
1 | |
\alpha |
\varepsilon
|E\alpha|\leq
An+1 | |
\alpha |
\varepsilon.
The Vitali covering lemma is vital to the proof of this theorem; its role lies in proving the estimate for the Hardy–Littlewood maximal function.
The theorem also holds if balls are replaced, in the definition of the derivative, by families of sets with diameter tending to zero satisfying the Lebesgue's regularity condition, defined above as family of sets with bounded eccentricity. This follows since the same substitution can be made in the statement of the Vitali covering lemma.
This is an analogue, and a generalization, of the fundamental theorem of calculus, which equates a Riemann integrable function and the derivative of its (indefinite) integral. It is also possible to show a converse – that every differentiable function is equal to the integral of its derivative, but this requires a Henstock–Kurzweil integral in order to be able to integrate an arbitrary derivative.
A special case of the Lebesgue differentiation theorem is the Lebesgue density theorem, which is equivalent to the differentiation theorem for characteristic functions of measurable sets. The density theorem is usually proved using a simpler method (e.g. see Measure and Category).
This theorem is also true for every finite Borel measure on Rn instead of Lebesgue measure (a proof can be found in e.g.). More generally, it is true of any finite Borel measure on a separable metric space such that at least one of the following holds:
A proof of these results can be found in sections 2.8–2.9 of (Federer 1969).
. Henri Lebesgue. Leçons sur l'Intégration et la recherche des fonctions primitives. Gauthier-Villars. Paris. 1904.
. Stein. Elias M.. Elias M. Stein. Shakarchi. Rami. Real analysis. Princeton Lectures in Analysis, III. Princeton University Press. Princeton, NJ. 2005. xx+402. 0-691-11386-6.
. Herbert Federer. Geometric measure theory. Springer-Verlag New York Inc.. New York. 1969. Die Grundlehren der mathematischen Wissenschaften, Band. 153.