Inner measure
In mathematics, in particular in measure theory, an inner measure is a function on the power set of a given set, with values in the extended real numbers, satisfying some technical conditions. Intuitively, the inner measure of a set is a lower bound of the size of that set.
Definition
[edit ]An inner measure is a set function {\displaystyle \varphi :2^{X}\to [0,\infty ],} defined on all subsets of a set {\displaystyle X,} that satisfies the following conditions:
- Null empty set: The empty set has zero inner measure (see also: measure zero ); that is, {\displaystyle \varphi (\varnothing )=0}
- Superadditive: For any disjoint sets {\displaystyle A} and {\displaystyle B,} {\displaystyle \varphi (A\cup B)\geq \varphi (A)+\varphi (B).}
- Limits of decreasing towers: For any sequence {\displaystyle A_{1},A_{2},\ldots } of sets such that {\displaystyle A_{j}\supseteq A_{j+1}} for each {\displaystyle j} and {\displaystyle \varphi (A_{1})<\infty } {\displaystyle \varphi \left(\bigcap _{j=1}^{\infty }A_{j}\right)=\lim _{j\to \infty }\varphi (A_{j})}
- If the measure is not finite, that is, if there exist sets {\displaystyle A} with {\displaystyle \varphi (A)=\infty }, then this infinity must be approached. More precisely, if {\displaystyle \varphi (A)=\infty } for a set {\displaystyle A} then for every positive real number {\displaystyle r,} there exists some {\displaystyle B\subseteq A} such that {\displaystyle r\leq \varphi (B)<\infty .}
The inner measure induced by a measure
[edit ]Let {\displaystyle \Sigma } be a σ-algebra over a set {\displaystyle X} and {\displaystyle \mu } be a measure on {\displaystyle \Sigma .} Then the inner measure {\displaystyle \mu _{*}} induced by {\displaystyle \mu } is defined by {\displaystyle \mu _{*}(T)=\sup\{\mu (S):S\in \Sigma {\text{ and }}S\subseteq T\}.}
Essentially {\displaystyle \mu _{*}} gives a lower bound of the size of any set by ensuring it is at least as big as the {\displaystyle \mu }-measure of any of its {\displaystyle \Sigma }-measurable subsets. Even though the set function {\displaystyle \mu _{*}} is usually not a measure, {\displaystyle \mu _{*}} shares the following properties with measures:
- {\displaystyle \mu _{*}(\varnothing )=0,}
- {\displaystyle \mu _{*}} is non-negative,
- If {\displaystyle E\subseteq F} then {\displaystyle \mu _{*}(E)\leq \mu _{*}(F).}
Measure completion
[edit ]Induced inner measures are often used in combination with outer measures to extend a measure to a larger σ-algebra. If {\displaystyle \mu } is a finite measure defined on a σ-algebra {\displaystyle \Sigma } over {\displaystyle X} and {\displaystyle \mu ^{*}} and {\displaystyle \mu _{*}} are corresponding induced outer and inner measures, then the sets {\displaystyle T\in 2^{X}} such that {\displaystyle \mu _{*}(T)=\mu ^{*}(T)} form a σ-algebra {\displaystyle {\hat {\Sigma }}} with {\displaystyle \Sigma \subseteq {\hat {\Sigma }}}.[1] The set function {\displaystyle {\hat {\mu }}} defined by {\displaystyle {\hat {\mu }}(T)=\mu ^{*}(T)=\mu _{*}(T)} for all {\displaystyle T\in {\hat {\Sigma }}} is a measure on {\displaystyle {\hat {\Sigma }}} known as the completion of {\displaystyle \mu .}
See also
[edit ]- Lebesgue measurable set – Concept of area in any dimensionPages displaying short descriptions of redirect targets
References
[edit ]- ^ Halmos 1950, § 14, Theorem F
- Halmos, Paul R., Measure Theory, D. Van Nostrand Company, Inc., 1950, pp. 58.
- A. N. Kolmogorov & S. V. Fomin, translated by Richard A. Silverman, Introductory Real Analysis, Dover Publications, New York, 1970, ISBN 0-486-61226-0 (Chapter 7)