Product measure explained

In mathematics, given two measurable spaces and measures on them, one can obtain a product measurable space and a product measure on that space. Conceptually, this is similar to defining the Cartesian product of sets and the product topology of two topological spaces, except that there can be many natural choices for the product measure.

Let

(X1,\Sigma1)

and

(X2,\Sigma2)

be two measurable spaces, that is,

\Sigma1

and

\Sigma2

are sigma algebras on

X1

and

X2

respectively, and let

\mu1

and

\mu2

be measures on these spaces. Denote by

\Sigma1\Sigma2

the sigma algebra on the Cartesian product

X1 x X2

generated by subsets of the form

B1 x B2

, where

B1\in\Sigma1

and

B2\in\Sigma2.

This sigma algebra is called the tensor-product σ-algebra on the product space.

A product measure

\mu1 x \mu2

(also denoted by

\mu1\mu2

by many authors)is defined to be a measure on the measurable space

(X1 x X2,\Sigma1\Sigma2)

satisfying the property

(\mu1 x \mu2)(B1 x B2)=\mu1(B1)\mu2(B2)

for all

B1\in\Sigma1,B2\in\Sigma2

.

(In multiplying measures, some of which are infinite, we define the product to be zero if any factor is zero.)

In fact, when the spaces are

\sigma

-finite, the product measure is uniquely defined, and for every measurable set E,

(\mu1 x \mu2)(E)=

\int
X2
y)d\mu
\mu
2(y)

=

\int
X1

\mu2(Ex)d\mu1(x),

where

Ex=\{y\inX2|(x,y)\inE\}

and

Ey=\{x\inX1|(x,y)\inE\}

, which are both measurable sets.

The existence of this measure is guaranteed by the Hahn–Kolmogorov theorem. The uniqueness of product measure is guaranteed only in the case that both

(X1,\Sigma1,\mu1)

and

(X2,\Sigma2,\mu2)

are σ-finite.

The Borel measures on the Euclidean space Rn can be obtained as the product of n copies of Borel measures on the real line R.

Even if the two factors of the product space are complete measure spaces, the product space may not be. Consequently, the completion procedure is needed to extend the Borel measure into the Lebesgue measure, or to extend the product of two Lebesgue measures to give the Lebesgue measure on the product space.

The opposite construction to the formation of the product of two measures is disintegration, which in some sense "splits" a given measure into a family of measures that can be integrated to give the original measure.

Examples

See also

References

. Michel Loève. Probability Theory vol. I . 4th . Springer . 1977 . 0-387-90210-4 . 8.2. Product measures and iterated integrals . 135 - 137 . loe1978.

. Paul Halmos . Measure theory . Springer . 1974 . 0-387-90088-8 . 35. Product measures . 143 - 145 . loe1978 . registration .