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11 - Measure theory and integration

Published online by Cambridge University Press:  05 September 2012

Peter Szekeres
Affiliation:
University of Adelaide
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Summary

Topology does not depend on the notion of ‘size’. We do not need to know the length, area or volume of subsets of a given set to understand the topological structure. Measure theory is that area of mathematics concerned with the attribution of precisely these sorts of properties. The structure that tells us which subsets are measurable is called a measure space. It is somewhat analogous with a topological structure, telling us which sets are open, and indeed there is a certain amount of interaction between measure theory and topology. A measure space requires firstly an algebraic structure known as a σ-algebra imposed on the power set of the underlying space. A measure is a positive-valued real function on the σ-algebra that is countably additive, whereby the measure of a union of disjoint measurable sets is the sum of their measures. The measure of a set may well be zero or infinite. Full introductions to this subject are given in [1–5], while the flavour of the subject can be found in [6–8].

It is important that measure be not just finitely additive, else it is not far-reaching enough, yet to allow it to be additive on arbitrary unions of disjoint sets would lead to certain contradictions – either all sets would have to be assigned zero measure, or the measure of a set would not be well-defined. By general reckoning the broadest useful measure on the real line or its cartesian products is that due to Lebesgue (1875–1941), and Lebesgue's theory of integration based on this theory is in most ways the best definition of integration available.

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A Course in Modern Mathematical Physics
Groups, Hilbert Space and Differential Geometry
, pp. 287 - 307
Publisher: Cambridge University Press
Print publication year: 2004

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