In mathematics, signed measure is a generalization of the concept of measure by allowing it to have negative values. In the theory of measures a signed measure is sometimes called a charge.[1]
Definition
There are two slightly different concepts of a signed measure, depending on whether or not one allows it to take infinite values. Signed measures are usually only allowed to take finite real values, while some textbooks allow them to take infinite values. To avoid confusion, this article will call these two cases "finite signed measures" and "extended signed measures".
Given a measurable space (X, Σ) (that is, a set X with a sigma algebra Σ on it), an extended signed measure is a function
\( {\displaystyle \mu :\Sigma \to \mathbb {R} \cup \{\infty ,-\infty \}} \)
such that \( \mu(\emptyset) = 0 \) and \( \mu \) is σ-additive – that is, it satisfies the equality
\( {\displaystyle \mu \left(\bigcup _{n=1}^{\infty }A_{n}\right)=\sum _{n=1}^{\infty }\mu (A_{n}).} \)
The series on the right must converge absolutely, for any sequence A1, A2, ..., An, ... of disjoint sets in Σ, when the value of the left-hand side is finite. One consequence is that any extended signed measure can take +∞ as a value, or it can take −∞ as a value, but both are not available. The expression ∞ − ∞ is undefined[2] and must be avoided.
A finite signed measure (a.k.a. real measure) is defined in the same way, except that it is only allowed to take real values. That is, it cannot take +∞ or −∞.
Finite signed measures form a real vector space, while extended signed measures do not because they are not closed under addition. On the other hand, measures are extended signed measures, but are not in general finite signed measures.
Examples
Consider a non-negative measure \( \nu \) on the space (X, Σ) and a measurable function f: X → R such that
\( {\displaystyle \int _{X}\!|f(x)|\,d\nu (x)<\infty .} \)
Then, a finite signed measure is given by
\( {\displaystyle \mu (A)=\int _{A}\!f(x)\,d\nu (x)} \)
for all A in Σ.
This signed measure takes only finite values. To allow it to take +∞ as a value, one needs to replace the assumption about f being absolutely integrable with the more relaxed condition
\( {\displaystyle \int _{X}\!f^{-}(x)\,d\nu (x)<\infty ,} \)
where f−(x) = max(−f(x), 0) is the negative part of f.
Properties
What follows are two results which will imply that an extended signed measure is the difference of two non-negative measures, and a finite signed measure is the difference of two finite non-negative measures.
The Hahn decomposition theorem states that given a signed measure μ, there exist two measurable sets P and N such that:
P∪N = X and P∩N = ∅;
μ(E) ≥ 0 for each E in Σ such that E ⊆ P — in other words, P is a positive set;
μ(E) ≤ 0 for each E in Σ such that E ⊆ N — that is, N is a negative set.
Moreover, this decomposition is unique up to adding to/subtracting μ-null sets from P and N.
Consider then two non-negative measures μ+ and μ− defined by
\( \mu ^{+}(E)=\mu (P\cap E)
and
\( \mu ^{-}(E)=-\mu (N\cap E) \)
for all measurable sets E, that is, E in Σ.
One can check that both μ+ and μ− are non-negative measures, with one taking only finite values, and are called the positive part and negative part of μ, respectively. One has that μ = μ+ − μ−. The measure |μ| = μ+ + μ− is called the variation of μ, and its maximum possible value, ||μ|| = |μ|(X), is called the total variation of μ.
This consequence of the Hahn decomposition theorem is called the Jordan decomposition. The measures μ+, μ− and |μ| are independent of the choice of P and N in the Hahn decomposition theorem.
Usage
A measure is given by the area function on regions of the Cartesian plane. This measure becomes a charge in certain instances. For example, when the natural logarithm is defined by the area under the curve y = 1/x for x in the positive real numbers, the region with 0 < x< 1 is considered negative.[3]
A region defined by a continuous function y = f(x), the x-axis, and lines x = a and x = b can be evaluated by Riemann integration. In this case the evaluation is a charge with the sign of the charge corresponding to the sign of y.
The space of signed measures
The sum of two finite signed measures is a finite signed measure, as is the product of a finite signed measure by a real number – that is, they are closed under linear combinations. It follows that the set of finite signed measures on a measurable space (X, Σ) is a real vector space; this is in contrast to positive measures, which are only closed under conical combinations, and thus form a convex cone but not a vector space. Furthermore, the total variation defines a norm in respect to which the space of finite signed measures becomes a Banach space. This space has even more structure, in that it can be shown to be a Dedekind complete Banach lattice and in so doing the Radon–Nikodym theorem can be shown to be a special case of the Freudenthal spectral theorem.
If X is a compact separable space, then the space of finite signed Baire measures is the dual of the real Banach space of all continuous real-valued functions on X, by the Riesz–Markov–Kakutani representation theorem.
See also
Complex measure
Spectral measure
Vector measure
Riesz–Markov–Kakutani representation theorem
Total variation
Notes
Bhaskara Rao 1983
See the article "Extended real number line" for more information.
The logarithm defined as an integral from University of California, Davis
References
Bartle, Robert G. (1966), The Elements of Integration, New York: John Wiley and Sons, Zbl 0146.28201
Bhaskara Rao, K. P. S.; Bhaskara Rao, M. (1983), Theory of Charges: A Study of Finitely Additive Measures, Pure and Applied Mathematics, London: Academic Press, ISBN 0-12-095780-9, Zbl 0516.28001
Cohn, Donald L. (1997) [1980], Measure theory, Boston: Birkhäuser Verlag, ISBN 3-7643-3003-1, Zbl 0436.28001
Diestel, J. E.; Uhl, J. J. Jr. (1977), Vector measures, Mathematical Surveys and Monographs, 15, Providence, R.I.: American Mathematical Society, ISBN 0-8218-1515-6, Zbl 0369.46039
Dunford, Nelson; Schwartz, Jacob T. (1959), Linear Operators. Part I: General Theory. Part II: Spectral Theory. Self Adjoint Operators in Hilbert Space. Part III: Spectral Operators., Pure and Applied Mathematics, 6, New York and London: Interscience Publishers, pp. XIV+858, ISBN 0-471-60848-3, Zbl 0084.10402
Dunford, Nelson; Schwartz, Jacob T. (1963), Linear Operators. Part I: General Theory. Part II: Spectral Theory. Self Adjoint Operators in Hilbert Space. Part III: Spectral Operators., Pure and Applied Mathematics, 7, New York and London: Interscience Publishers, pp. IX+859–1923, ISBN 0-471-60847-5, Zbl 0128.34803
Dunford, Nelson; Schwartz, Jacob T. (1971), Linear Operators. Part I: General Theory. Part II: Spectral Theory. Self Adjoint Operators in Hilbert Space. Part III: Spectral Operators., Pure and Applied Mathematics, 8, New York and London: Interscience Publishers, pp. XIX+1925–2592, ISBN 0-471-60846-7, Zbl 0243.47001
Zaanen, Adriaan C. (1996), Introduction to Operator Theory in Riesz spaces, Springer Publishing, ISBN 3-540-61989-5
This article incorporates material from the following PlanetMath articles, which are licensed under the Creative Commons Attribution/Share-Alike License: Signed measure, Hahn decomposition theorem, Jordan decomposition.
Undergraduate Texts in Mathematics
Graduate Studies in Mathematics
Hellenica World - Scientific Library
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