Finite measure

In measure theory, a branch of mathematics, a finite measure or totally finite measure[1] is a special measure that always takes on finite values. Among finite measures are probability measures. The finite measures are often easier to handle than more general measures and show a variety of different properties depending on the sets they are defined on.

Definition

A measureμ{\displaystyle \mu } on measurable space(X,A){\displaystyle (X,{\mathcal {A}})} is called a finite measure if it satisfies

μ(X)<.{\displaystyle \mu (X)<\infty .}

By the monotonicity of measures, this implies

μ(A)< for all AA.{\displaystyle \mu (A)<\infty {\text{ لكل }}A\in {\mathcal {A}}.}

If μ{\displaystyle \mu } is a finite measure, the measure space(X,A,μ){\displaystyle (X,{\mathcal {A}},\mu )} is called a finite measure space or a totally finite measure space.[1]

Properties

General case

For any measurable space, the finite measures form a convex cone in the Banach space of signed measures with the total variation norm. Important subsets of the finite measures are the sub-probability measures, which form a convex subset, and the probability measures, which are the intersection of the unit sphere in the normed space of signed measures and the finite measures.

Topological spaces

If X{\displaystyle X} is a Hausdorff space and A{\displaystyle {\mathcal {A}}} contains the Borel σ{\displaystyle \sigma }-algebra then every finite measure is also a locally finiteBorel measure.

Metric spaces

If X{\displaystyle X} is a metric space and the A{\displaystyle {\mathcal {A}}} is again the Borel σ{\displaystyle \sigma }-algebra, the weak convergence of measures can be defined. The corresponding topology is called weak topology and is the initial topology of all bounded continuous functions on X{\displaystyle X}. The weak topology corresponds to the weak* topology in functional analysis. If X{\displaystyle X} is also separable, the weak convergence is metricized by the Lévy–Prokhorov metric.[2]

Polish spaces

If X{\displaystyle X} is a Polish space and A{\displaystyle {\mathcal {A}}} is the Borel σ{\displaystyle \sigma }-algebra, then every finite measure is a regular measure and therefore a Radon measure.[3] If X{\displaystyle X} is Polish, then the set of all finite measures with the weak topology is Polish too.[4]

See also

References

  1. 1 2 أنوسوف، د. ف. (2001) [1994]، "فضاء القياس" ، موسوعة الرياضيات ، دار نشر EMS
  2. كلينكه، آخيم (2008). نظرية الاحتمالات . برلين: سبرينغر . ص 252. doi : 10.1007/978-1-84800-048-3 . ISBN  978-1-84800-047-6.
  3. كلينكه، آخيم (2008). نظرية الاحتمالات . برلين: سبرينغر . ص 248. doi : 10.1007/978-1-84800-048-3 . ISBN  978-1-84800-047-6.
  4. كالينبيرغ، أولاف (2017). المقاييس العشوائية: النظرية والتطبيقات . نظرية الاحتمالات والنمذجة العشوائية. المجلد 77. سويسرا: سبرينغر. ص 112. doi : 10.1007/978-3-319-41598-7 . ISBN   978-3-319-41596-3.