Abstract

In this note we show that some concepts of modern measure theory may be relevant to the formulation of theories in continuum physics. In particular we observe that a large class of measure spaces possesses a decomposition property which is useful in applications. This decomposition property is obtained as a corollary to a theorem of Kelley [10] concerning the "Lebesgue decomposition property," which result is based upon the investigations of Segal [3]. The mathematical notation and definitions (following Kelley [10]), are presented first; then a Lemma and the Decomposition are given. The relationship between these results and physical theories is presented in a series of remarks at the end . As a preliminary we establish some useful definitions and notation. I Let be a set and let sg/a be a ring of subsets of M whose union is ~ . We further assume that d / ~ has the property: if {d~ } is a sequence of sets in d¢ "~ such that if ~¢. _ d E d¢ '~, for all n and some d in d /~ , then U . d . ~ d¢ 'a~. By a measure v in we mean a non-negative, finite valued, countably additive set function defined on ~ ' a with the following additional property: if {~ ' . } is a disjoint sequence in ~.¢/a such that g . v ( d . ) converges, then U . d . a jfa~.2 A subfamily q / i n ~ ' a is called a a-ideal in d¢ 'a~ if and only if it is a ring of sets, the intersection of a member of q /wi th a member o f ~ / a is a member of q/, and any member of~¢¢ '~ which is a countable union of sets in ~ is itself a set in q/. A set ~ _ ~ is (locally) measurable if and only if ~¢ n ~ e J / fa for all ~¢ in J/¢'~. We denote the class of measurable sets in ~ by ~//¢ and observe that J g is a or-algebra of subsets of ~ containing ~ ,a .3 I f~¢ and cg are in J r , we write ~¢Ro~ if and only i f c ~ ~ ¢ contains no set

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