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
An inner measure is a set function
φ
:
2
X
→
[
0
,
∞
]
,
{\displaystyle \varphi :2^{X}\to [0,\infty ],}
defined on all subsets of a set
X
,
{\displaystyle X,}
that satisfies the following conditions:
- Null empty set: The empty set has zero inner measure (see also: measure zero); that is,
φ
(
∅
)
=
0
{\displaystyle \varphi (\varnothing )=0}
- Superadditive: For any disjoint sets
A
{\displaystyle A}
and B , {\displaystyle B,}
φ ( A ∪ B ) ≥ φ ( A ) + φ ( B ) . {\displaystyle \varphi (A\cup B)\geq \varphi (A)+\varphi (B).}
- Limits of decreasing towers: For any sequence
A
1
,
A
2
,
…
{\displaystyle A_{1},A_{2},\ldots }
of sets such that A j ⊇ A j + 1 {\displaystyle A_{j}\supseteq A_{j+1}}
for each j {\displaystyle j}
and φ ( A 1 ) < ∞ {\displaystyle \varphi (A_{1})<\infty }
φ ( ⋂ j = 1 ∞ A j ) = lim j → ∞ φ ( A j ) {\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
A
{\displaystyle A}
with φ ( A ) = ∞ {\displaystyle \varphi (A)=\infty }
, then this infinity must be approached. More precisely, if φ ( A ) = ∞ {\displaystyle \varphi (A)=\infty }
for a set A {\displaystyle A}
then for every positive real number r , {\displaystyle r,}
there exists some B ⊆ A {\displaystyle B\subseteq A}
such that r ≤ φ ( B ) < ∞ . {\displaystyle r\leq \varphi (B)<\infty .}
The inner measure induced by a measure
Let
Σ
{\displaystyle \Sigma }
be a σ-algebra over a set
X
{\displaystyle X}
and
μ
{\displaystyle \mu }
be a measure on
Σ
.
{\displaystyle \Sigma .}
Then the inner measure
μ
∗
{\displaystyle \mu _{*}}
induced by
μ
{\displaystyle \mu }
is defined by
μ
∗
(
T
)
=
sup
{
μ
(
S
)
:
S
∈
Σ
and
S
⊆
T
}
.
{\displaystyle \mu _{*}(T)=\sup\{\mu (S):S\in \Sigma {\text{ and }}S\subseteq T\}.}
Essentially
μ
∗
{\displaystyle \mu _{*}}
gives a lower bound of the size of any set by ensuring it is at least as big as the
μ
{\displaystyle \mu }
-measure of any of its
Σ
{\displaystyle \Sigma }
-measurable subsets. Even though the set function
μ
∗
{\displaystyle \mu _{*}}
is usually not a measure,
μ
∗
{\displaystyle \mu _{*}}
shares the following properties with measures:
-
μ
∗
(
∅
)
=
0
,
{\displaystyle \mu _{*}(\varnothing )=0,}
-
μ
∗
{\displaystyle \mu _{*}}
is non-negative,
- If
E
⊆
F
{\displaystyle E\subseteq F}
then μ ∗ ( E ) ≤ μ ∗ ( F ) . {\displaystyle \mu _{*}(E)\leq \mu _{*}(F).}
Measure completion
Induced inner measures are often used in combination with outer measures to extend a measure to a larger σ-algebra. If
μ
{\displaystyle \mu }
is a finite measure defined on a σ-algebra
Σ
{\displaystyle \Sigma }
over
X
{\displaystyle X}
and
μ
∗
{\displaystyle \mu ^{*}}
and
μ
∗
{\displaystyle \mu _{*}}
are corresponding induced outer and inner measures, then the sets
T
∈
2
X
{\displaystyle T\in 2^{X}}
such that
μ
∗
(
T
)
=
μ
∗
(
T
)
{\displaystyle \mu _{*}(T)=\mu ^{*}(T)}
form a σ-algebra
Σ
^
{\displaystyle {\hat {\Sigma }}}
with
Σ
⊆
Σ
^
{\displaystyle \Sigma \subseteq {\hat {\Sigma }}}
.[1]
The set function
μ
^
{\displaystyle {\hat {\mu }}}
defined by
μ
^
(
T
)
=
μ
∗
(
T
)
=
μ
∗
(
T
)
{\displaystyle {\hat {\mu }}(T)=\mu ^{*}(T)=\mu _{*}(T)}
for all
T
∈
Σ
^
{\displaystyle T\in {\hat {\Sigma }}}
is a measure on
Σ
^
{\displaystyle {\hat {\Sigma }}}
known as the completion of
μ
.
{\displaystyle \mu .}
See also
- Lebesgue measurable set – Broadest definition of sizes in integer-dimensional spacesPages displaying short descriptions of redirect targets
References
- 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)