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Lebesgue's decomposition theorem

From Wikipedia, the free encyclopedia
Theorem in mathematical measure theory

Inmathematics, more precisely inmeasure theory, theLebesgue decomposition theorem[1] provides a way to decompose a measure into two distinct parts based on their relationship with another measure.

Formal Statement

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The theorem states that if(Ω,Σ){\displaystyle (\Omega ,\Sigma )} is ameasurable space andμ{\displaystyle \mu } andν{\displaystyle \nu } areσ-finitesigned measures onΣ{\displaystyle \Sigma }, then there exist two uniquely determined σ-finite signed measuresν0{\displaystyle \nu _{0}} andν1{\displaystyle \nu _{1}} such that:[2][3]

Refinement

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Lebesgue's decomposition theorem can be refined in a number of ways. First, as theLebesgue–Radon–Nikodym theorem. That is, let(Ω,Σ){\displaystyle (\Omega ,\Sigma )} be a measure space,μ{\displaystyle \mu } aσ-finitepositive measure onΣ{\displaystyle \Sigma } andλ{\displaystyle \lambda } acomplex measure onΣ{\displaystyle \Sigma }.[4]

The first assertion follows from the Lebesgue decomposition, the second is known as theRadon–Nikodym theorem. That is, the functionh{\displaystyle h} is a Radon–Nikodym derivative that can be expressed ash=dλadμ.{\displaystyle h={\frac {d\lambda _{a}}{d\mu }}.}

An alternative refinement is that of the decomposition of a regularBorel measure[5][6][7]ν=νac+νsc+νpp,{\displaystyle \nu =\nu _{ac}+\nu _{sc}+\nu _{pp},}where

The absolutely continuous measures are classified by theRadon–Nikodym theorem, and discrete measures are easily understood. Hence (singular continuous measures aside), Lebesgue decomposition gives a very explicit description of measures. TheCantor measure (theprobability measure on thereal line whosecumulative distribution function is theCantor function) is an example of a singular continuous measure.

Related concepts

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Lévy–Itō decomposition

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Main article:Lévy–Itō decomposition

The analogous[citation needed] decomposition for astochastic processes is theLévy–Itō decomposition: given aLévy processX, it can be decomposed as a sum of three independentLévy processesX=X(1)+X(2)+X(3){\displaystyle X=X^{(1)}+X^{(2)}+X^{(3)}} where:

See also

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Notes

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  1. ^Hewitt & Stromberg 1965, Chapter V, § 19, (19.42) Lebesgue Decomposition Theorem.
  2. ^Halmos 1974, Section 32, Theorem C.
  3. ^Swartz 1994, p. 141.
  4. ^Rudin 1974, Section 6.9, The Theorem of Lebesgue–Radon–Nikodym.
  5. ^Hewitt & Stromberg 1965, Chapter V, § 19, (19.61) Theorem.
  6. ^Reed & Simon 1981, pp. 22–25.
  7. ^Simon 2005, p. 43.

References

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This article incorporates material from Lebesgue decomposition theorem onPlanetMath, which is licensed under theCreative Commons Attribution/Share-Alike License.

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