Our starting point again is a measurable space with the assumptions and notation in Section 1. In particular, is a measurable semigroup that satisfies the left cancellation property. Recall also that the graph associated with is defined by if and only if for so that for some . In the case of a positive semigroup, studied in Section 2, the relation is a partial order.
Basics
Suppose that we have a fixed -finite reference measure for . The following restates a definition from Section 1.1, but in the notation of semigroups.
The semigroup is (right) positive (with respect to if for .
We usually assume that the semigroup is positive with respect to the reference measure, so that the measure and the semigroup (and its graph) are connected in a fundamental way. In particular, recall that is the set of (right) neighbors of and that the -algebra associated with the semigroup (or its graph) is . Left invariance of a measure on with respect to the semigroup is the abstract version of translation invariance for Lebesgue measure and counting measure, and is very important for our study of probability on semigroups.
Suppose that is a semigroup. A -finite measure is left invariant for if for every and .
We always assume that , so trivially is positive with respect to a left-invariant measure . Naturally there is a parallel definition for a right invariant measure which leads in turn to the definition for an invariant measrue that is both left and right invariant. Invariant measures (left, right, or both) are also known as Haar measures in honor of Alfred Haar, who first studied them. Left invariance is the property that is important for our study of abstract reliability.
Suppose that is left invariant for . Then for and ,
Details:
Recall that for and . Hence
In partiular, if and with . The left cancellation property would seem to be a necessary condition for left invariance to make sense, since is an isomorphism from the graph to the graph for each . Trivially, if is left invariant for then so is where . So we are particularly interested in the case where a left-invariant measure exists and is unique up to multiplication by positive constants, either on the associated -algebra or the reference -algebra . The next example and proposition give a case where uniqueness fails in the extreme, and an important case where uniqueness holds.
Suppose that is the right zero semigroup on , so that for . Then for and , so trivially every measure on is left invariant.
Suppose that is a discrete semigroup.
- Counting measure is left invariant.
- If has an identity then is the unique left-invariant measure, up to multiplication by positive constants.
Details:
Recall that the term discrete means that is countable and is the power set of .
- If and then and have the same cardinality by the left cancellation property so . Hence is left invariant.
- Suppose that has an identity element . If is a left-invariant measure then for . Hence .
Here is the classical existence and uniqueness theorem in the special case of a topological group:
Suppose that is a locally compact topological space. If is a topological group then there exists a regular left-invariant Borel measure that is unique up to multiplication by positive constants.
Details:
Recall that is given the Borel -algebra . The term topological group means that the function from (with the product topology) into is continuous. The term Borel measure means that if is open, and the term regular means that for
The first condition is inner regularity and the second condition is outer regularity. The proof of the theorem can be found in the book by Halmos.
However, a full group is usually not the proper object of study in the abstract reliability setting. Rather, we are usually interested in a sub-semigroup of positive elements
.
Suppose again that is a locally compact topological space and that is a topological group. If is a (measurable) positive sub-semigroup of and has nonempty interior, then the regular left-invariant measure for is also left invariant for .
Details:
The assumptions mean that the identity and that if then , where as usual, . The fact that has nonempty interior ensures that . The left-invariance property trivially holds for and with since it holds more generally for and .
Fix and let for . Recall that maps one-to-one onto and has inverse function given by for . Both are measurable. By definition, if the measure is left invariant for then the functions and preserve measure:
The standard change of variables theorem then gives integral versions of left invariance.
Suppose that is left invariant for and that is measurable. Then for (and assuming that the integrals exist),
The fundamental mapping in Section 1 gives a two-dimensional version. As before, let for , so that maps one-to-one onto
and has inverse function given by for . Both are measurable, and it is worth noting again that the co-domain is the realtion as a set of ordered pairs. If is left invariant then preserves measure:
Suppose that is left invariant for . Then
Details:
For , let denote the cross section of at . Then . Hence by Fubini's theorem and left invariance
As before, the standard change of variables theorem for integrals gives us the following:
Suppose that is left invariant for and that is measurable. Then (assuming that the integrals exist),
Convolution
Functions
The concept of convolution of functions makes sense in a semigroup with a left invariant reference measure. So for the remainder of this section, suppose that the -finite measure is left invariant for the semigroup , and let denote the relation associated with . We are only going to need convolution for nonnegative functions.
For measurble , the convolution of with is the function defined by
Note that the definition makes sense. Recall that if and only if , so is defined. Moreover, the function from to is measurable. Like the semigroup itself, convolution is associative, but not commutative in general.
For measurable ,
Details:
First,
On the other hand, for ,
But if and then . Our basic measure preserving mapping , transforms the domain one-to-one onto the domain . Hence from [10],
Measures
Convolution can also be defined for finite measures without reference to an underlying left-invariant measure. Probability measures, of course, are the most important special case.
Suppose that and are finite measures on . The convolution of with is the finite measure defined by
There are several variations.
Suppose again that and are finite measures on . Then
Details:
The first and second representations follows from the definition by Fubini's theorem. The third representation follows from the second since if and only if .
Once again, convolution is associative.
Suppose that , , and are finite measures on . Then so we can write without ambiguity.
Details:
The common value is
Given definition [13], the following result is not surprising.
Suppose that and are finite measures and that is measurable. Then
Details:
The first representation follows from definition [13] by a standard boot-strapping argument. The second representation follows from the first by Fubini's theorem.
This result holds more generally for measurable , assuming that the integrals exist.
Examples
Positive Semigroups
Positive semigroups are a particularly important special case. Suppose that is a positive semigroup with identity , so that the associated relation is a partial order . We assume again that we have a fixed, left-invariant measure , and as usual, we let denote the adjacency kernel and the (left) walk function of order (with respect to of course).
For ,
Details:
Suppose that and . The simple combinatorial argument
is that
is a walk of length from to if and only if
is a walk of length from to , if and only if
is a walk of length terminating in . As will be shown in Section 7, the product measure is left invariant for the product semigroup . Hence the three sets of walks have the same measure.
Standard Spaces
Consider the standard continuous semigroup . Recall that the underlying measure space is where is the -algebra of Borel sets and is Lebesgue measure.
- is the unique left-invariant measure, up to multiplication by positive constants.
- For ,
Consider the standard discrete semigroup . The underlying measure space is .
- is the unique left-invariant measure, up to multiplication by positive constants.
- For ,