Borel measure – Wikipedia
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Measure defined on all open sets of a topological space
In mathematics, specifically in measure theory, a Borel measure on a topological space is a measure that is defined on all open sets (and thus on all Borel sets).[1] Some authors require additional restrictions on the measure, as described below.
Formal definition[edit]
Let
be a locally compact Hausdorff space, and let
be the smallest σ-algebra that contains the open sets of
; this is known as the σ-algebra of Borel sets. A Borel measure is any measure
defined on the σ-algebra of Borel sets.[2] A few authors require in addition that
is locally finite, meaning that
for every compact set
. If a Borel measure
is both inner regular and outer regular, it is called a regular Borel measure. If
is both inner regular, outer regular, and locally finite, it is called a Radon measure.
On the real line[edit]
The real line
with its usual topology is a locally compact Hausdorff space; hence we can define a Borel measure on it. In this case,
is the smallest σ-algebra that contains the open intervals of
. While there are many Borel measures μ, the choice of Borel measure that assigns
for every half-open interval
is sometimes called “the” Borel measure on
. This measure turns out to be the restriction to the Borel σ-algebra of the Lebesgue measure
, which is a complete measure and is defined on the Lebesgue σ-algebra. The Lebesgue σ-algebra is actually the completion of the Borel σ-algebra, which means that it is the smallest σ-algebra that contains all the Borel sets and can be equipped with a complete measure. Also, the Borel measure and the Lebesgue measure coincide on the Borel sets (i.e.,
for every Borel measurable set, where
is the Borel measure described above).
Product spaces[edit]
If X and Y are second-countable, Hausdorff topological spaces, then the set of Borel subsets
of their product coincides with the product of the sets
of Borel subsets of X and Y.[3] That is, the Borel functor
from the category of second-countable Hausdorff spaces to the category of measurable spaces preserves finite products.
Applications[edit]
Lebesgue–Stieltjes integral[edit]
The Lebesgue–Stieltjes integral is the ordinary Lebesgue integral with respect to a measure known as the Lebesgue–Stieltjes measure, which may be associated to any function of bounded variation on the real line. The Lebesgue–Stieltjes measure is a regular Borel measure, and conversely every regular Borel measure on the real line is of this kind.[4]
Laplace transform[edit]
One can define the Laplace transform of a finite Borel measure μ on the real line by the Lebesgue integral[5]
An important special case is where μ is a probability measure or, even more specifically, the Dirac delta function. In operational calculus, the Laplace transform of a measure is often treated as though the measure came from a distribution function f. In that case, to avoid potential confusion, one often writes
where the lower limit of 0− is shorthand notation for
This limit emphasizes that any point mass located at 0 is entirely captured by the Laplace transform. Although with the Lebesgue integral, it is not necessary to take such a limit, it does appear more naturally in connection with the Laplace–Stieltjes transform.
Hausdorff dimension and Frostman’s lemma[edit]
Given a Borel measure μ on a metric space X such that μ(X) > 0 and μ(B(x, r)) ≤ rs holds for some constant s > 0 and for every ball B(x, r) in X, then the Hausdorff dimension dimHaus(X) ≥ s. A partial converse is provided by the Frostman lemma:[6]
Lemma: Let A be a Borel subset of Rn, and let s > 0. Then the following are equivalent:
- Hs(A) > 0, where Hs denotes the s-dimensional Hausdorff measure.
- There is an (unsigned) Borel measure μ satisfying μ(A) > 0, and such that
-
- holds for all x ∈ Rn and r > 0.
Cramér–Wold theorem[edit]
The Cramér–Wold theorem in measure theory states that a Borel probability measure on
is uniquely determined by the totality of its one-dimensional projections.[7] It is used as a method for proving joint convergence results. The theorem is named after Harald Cramér and Herman Ole Andreas Wold.
References[edit]
- ^ D. H. Fremlin, 2000. Measure Theory Archived 2010-11-01 at the Wayback Machine. Torres Fremlin.
- ^ Alan J. Weir (1974). General integration and measure. Cambridge University Press. pp. 158–184. ISBN 0-521-29715-X.
- ^ Vladimir I. Bogachev. Measure Theory, Volume 1. Springer Science & Business Media, Jan 15, 2007
- ^ Halmos, Paul R. (1974), Measure Theory, Berlin, New York: Springer-Verlag, ISBN 978-0-387-90088-9
- ^ Feller 1971, §XIII.1
- ^ Rogers, C. A. (1998). Hausdorff measures. Cambridge Mathematical Library (Third ed.). Cambridge: Cambridge University Press. pp. xxx+195. ISBN 0-521-62491-6.
- ^ K. Stromberg, 1994. Probability Theory for Analysts. Chapman and Hall.
Further reading[edit]
- Gaussian measure, a finite-dimensional Borel measure
- Feller, William (1971), An introduction to probability theory and its applications. Vol. II., Second edition, New York: John Wiley & Sons, MR 0270403.
- J. D. Pryce (1973). Basic methods of functional analysis. Hutchinson University Library. Hutchinson. p. 217. ISBN 0-09-113411-0.
- Ransford, Thomas (1995). Potential theory in the complex plane. London Mathematical Society Student Texts. Vol. 28. Cambridge: Cambridge University Press. pp. 209–218. ISBN 0-521-46654-7. Zbl 0828.31001.
- Teschl, Gerald, Topics in Real and Functional Analysis, (lecture notes)
- Wiener’s lemma related
External links[edit]
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