- Lebesgue measure
In
mathematics , the Lebesgue measure, named afterHenri Lebesgue , is the standard way of assigning alength ,area orvolume tosubset s ofEuclidean space . It is used throughoutreal analysis , in particular to defineLebesgue integration . Sets which can be assigned a volume are called Lebesgue measurable; the volume or measure of the Lebesgue measurable set "A" is denoted by λ("A"). A Lebesgue measure of ∞ is possible, but even so, assuming theaxiom of choice , not all subsets of R"n" are Lebesgue measurable. The "strange" behavior ofnon-measurable set s gives rise to such statements as the Banach-Tarski paradox, a consequence of the axiom of choice.Lebesgue measure is often denoted , but this should not be confused with the distinct notion of a
volume form .Examples
* If "A" is a closed interval ["a", "b"] , then its Lebesgue measure is the length "b"−"a". The open interval ("a", "b") has the same measure, since the difference between the two sets has measure zero.
* If "A" is theCartesian product of intervals ["a", "b"] and ["c", "d"] , then it is a rectangle and its Lebesgue measure is the area ("b"−"a")("d"−"c").
* TheCantor set is an example of anuncountable set that has Lebesgue measure zero.Properties
The Lebesgue measure on R"n" has the following properties:
# If "A" is a
cartesian product of intervals "I"1 × "I"2 × ... × "I""n", then "A" is Lebesgue measurable and Here, |"I"| denotes the length of the interval "I".
# If "A" is adisjoint union of finitely many or countably many disjoint Lebesgue measurable sets, then "A" is itself Lebesgue measurable and λ("A") is equal to the sum (orinfinite series ) of the measures of the involved measurable sets.
# If "A" is Lebesgue measurable, then so is its complement.
# λ("A") ≥ 0 for every Lebesgue measurable set "A".
# If "A" and "B" are Lebesgue measurable and "A" is a subset of "B", then λ("A") ≤ λ("B"). (A consequence of 2, 3 and 4.)
# Countable unions and intersections of Lebesgue measurable sets are Lebesgue measurable. (Not a consequence of 2 and 3, because a family of sets that is closed under complements and disjoint countable unions need not be closed under countable unions: .)
# If "A" is an open or closed subset of R"n" (or evenBorel set , seemetric space ), then "A" is Lebesgue measurable.
# If "A" is a Lebesgue measurable set, then it is "approximately open" and "approximately closed" in the sense of Lebesgue measure (see theregularity theorem for Lebesgue measure ).
# Lebesgue measure is both locally finite and inner regular, and so it is aRadon measure .
# Lebesgue measure is strictly positive on non-empty open sets, and so its support is the whole of R"n".
# If "A" is a Lebesgue measurable set with λ("A") = 0 (anull set ), then every subset of "A" is also a null set.A fortiori , every subset of "A" is measurable.
# If "A" is Lebesgue measurable and "x" is an element of R"n", then the "translation of "A" by x", defined by "A" + "x" = {"a" + "x" : "a" ∈ "A"}, is also Lebesgue measurable and has the same measure as "A".
# If "A" is Lebesgue measurable and , then the "dilation of by " defined by is also Lebesgue measurable and has measure .
# More generally, if "T" is alinear transformation and "A" is a measurable subset of R"n", then "T"("A") is also Lebesgue measurable and has the measure .All the above may be succinctly summarized as follows:
: The Lebesgue measurable sets form a σ-algebra containing all products of intervals, and λ is the unique complete translation-invariant measure on that σ-algebra with
The Lebesgue measure also has the property of being σ-finite.
Null sets
A subset of R"n" is a "null set" if, for every ε > 0, it can be covered with countably many products of "n" intervals whose total volume is at most ε. All
countable sets are null sets.If a subset of R"n" has
Hausdorff dimension less than "n" then it is a null set with respect to "n"-dimensional Lebesgue measure. Here Hausdorff dimension is relative to theEuclidean metric on R"n" (or any metricLipschitz equivalent to it). On the other hand a set may havetopological dimension less than "n" and have positive "n"-dimensional Lebesgue measure. An example of this is theSmith-Volterra-Cantor set which has topological dimension 0 yet has positive 1-dimensional Lebesgue measure.In order to show that a given set "A" is Lebesgue measurable, one usually tries to find a "nicer" set "B" which differs from "A" only by a null set (in the sense that the
symmetric difference ("A" − "B") ("B" − "A") is a null set) and then show that "B" can be generated using countable unions and intersections from open or closed sets.Construction of the Lebesgue measure
The modern construction of the Lebesgue measure, based on
outer measure s, is due to Carathéodory. It proceeds as follows.Fix . A box in is a set of the form , where . The volume of this box is defined to be
For "any" subset "A" of R"n", we can define its outer measure by:
:
We then define the set "A" to be Lebesgue measurable if
:
for all sets . These Lebesgue measurable sets form a
σ-algebra , and the Lebesgue measure is defined by λ("A") = λ*("A") for any Lebesgue measurable set "A".According to the Vitali theorem there exists a subset of the real numbers R that is not Lebesgue measurable. Much more is true: if "A" is any subset of of positive measure, then "A" has subsets which are not Lebesgue measurable.
Relation to other measures
The
Borel measure agrees with the Lebesgue measure on those sets for which it is defined; however, there are many more Lebesgue-measurable sets than there are Borel measurable sets. The Borel measure is translation-invariant, but not complete.The
Haar measure can be defined on anylocally compact group and is a generalization of the Lebesgue measure (R"n" with addition is a locally compact group).The Hausdorff measure (see
Hausdorff dimension ) is a generalization of the Lebesgue measure that is useful for measuring the subsets of R"n" of lower dimensions than "n", likesubmanifold s, for example, surfaces or curves in R³ andfractal sets. The Hausdorff measure is not to be confused with the notion of Hausdorff dimension.It can be shown that there is no infinite-dimensional analogue of Lebesgue measure.
History
Henri Lebesgue described his measure in 1901, followed the next year by his description of the Lebesgue integral. Both were published as part of his dissertation in 1902.ee also
*
Lebesgue's density theorem
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