Complex measure

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In mathematics, or more specifically in measure theory, a complex measure is a generalisation of the concept of measure by letting it have complex values. In other words, one allows for sets whose size (length, area, volume) is a complex number.

1 Definition
2 Integration in respect to a complex measure
3 Variation of a complex measure and polar decomposition
4 The space of complex measures
5 See also
6 External links

[edit] Definition

Formally, a complex measure μ on a measurable space (X,Σ) is a function

$\mu:\Sigma\to \mathbb{C}$

defined on Σ and taking complex values, which is sigma-additive; that is, for any sequence (A_n)_n of disjoint sets in Σ one has

$\mu\left(\bigcup_{n=1}^\infty A_n\right) = \sum_{n=1}^\infty \mu(A_n).$

[edit] Integration in respect to a complex measure

One can define the integral of a complex-valued measurable function in respect to a complex measure in the same way as the Lebesgue integral of a real-valued measurable function in respect to a non-negative measure, by approximating a measurable function with simple functions. Just as in the case of ordinary integration, this more general integral might fail to exist, or its value might be infinite (the complex infinity).

Another approach is to not develop a theory of integration from scratch, but rather use the already available concept of integral of a real-valued function in respect to a non-negative measure. To that end, it is a quick check that the real and imaginary parts μ₁ and μ₂ of a complex measure μ are finite-valued signed measures. One can apply the Hahn-Jordan decomposition to these measures to split them as

$\mu_1=\mu_1^+-\mu_1^-$

and

$\mu_2=\mu_2^+-\mu_2^-$

where μ₁⁺, μ₁^-, μ₂⁺, μ₂^- are finite-valued non-negative measures (unique in some sense). Then, for a measurable function f which is real-valued for the moment, one can define

$\int_X \! f \, d\mu = \left(\int_X \! f \, d\mu_1^+ - \int_X \! f \, d\mu_1^-\right) + i \left(\int_X \! f \, d\mu_2^+ - \int_X \! f \, d\mu_2^-\right)$

as long as the expression on the right-hand side is defined, that is, all four integrals exist and when adding them up one does not encounter the indeterminate ∞−∞.

Given now a complex-valued measurable function, one can integrate its real and imaginary components separately as illustrated above and define, as expected,

$\int_X \! f \, d\mu = \int_X \! \Re(f) \, d\mu + i \int_X \! \Im(f) \, d\mu.$

[edit] Variation of a complex measure and polar decomposition

For a complex measure μ, one defines its variation, or absolute value, |μ| by the formula

$|\mu|(A)= \sup\sum_{n=1}^\infty |\mu(A_n)|$

where A is in Σ and the supremum runs over all sequences of disjoint sets (A_n)_n whose union is A. Taking only finite partitions of the set A into measurable subsets, one obtains an equivalent definition.

It turns out that |μ| is a non-negative finite measure. In the same way as a complex number can be represented in a polar form, one has a polar decomposition for a complex measure: There exists a measurable function θ with real values such that

$d\mu = e ^{i \theta}d |\mu|\,$

meaning

$\int_X f\, d\mu = \int_X f e ^{i \theta} \, d |\mu|$

for any absolutely integrable measurable function f, i.e., f satisfying

$\int_X |f|\, d|\mu|<\infty.$

One can use the Radon-Nikodym theorem to prove that the variation is a measure and the existence of the polar decomposition.

[edit] The space of complex measures

The sum of two complex measures is a complex measure, as is the product of a complex measure by a complex number. That is to say, the set of all complex measures on a measure space (X, Σ) forms a vector space. Moreover, the total variation ||μ|| defined as

$\|\mu\| = |\mu| (X)\,$