Abstract
Recall that a non-empty collection Γ of subsets of the set X is called a ring of subsets of X if A ∈ Γ, B ∈ Γ implies A ∪ B ∈ Γ and A\B ∈ Γ (see Example 3.4(i)). It follows then that finite unions and finite intersections of sets in Γ are sets in Γ. The ring Γ is called an algebra of subsets of X if X itself is a member of Γ. The algebra Γ is called a σ-algebra if any countable union of sets in Γ is again a set in Γ (see Example 3.4(ii)). The mapping v from the algebra Γ into ℝ is called a (real) finitely additive signed measure (or a charge) on Γ if v(A1 ∪ A2) = v (A1) + v (A2) holds for all disjoint Al and A2 in Γ (see Example 4.3(7)). If Γ is a σ-algebra and v \( \left( { \cup _1^\infty {A_n}} \right) = \sum\nolimits_1^\infty {v\left( {{A_n}} \right)} \)holds for every disjoint sequence (A n : n = 1, 2,…) in Γ, then v is called a σ-additive signed measure on Γ. In this section we shall briefly say “signed measure” when a σ-additive signed measure is meant. If there is only finite additivity, this will be explicitly mentioned.
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© 1997 Springer-Verlag Berlin Heidelberg
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Zaanen, A.C. (1997). Signed Measures and the Radon-Nikodym Theorem. In: Introduction to Operator Theory in Riesz Spaces. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-60637-3_14
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DOI: https://doi.org/10.1007/978-3-642-60637-3_14
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-642-64487-0
Online ISBN: 978-3-642-60637-3
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