This post is inspired by Professor Tom Fischer’s writeup.
Recall the Hahn decomposition theorem:
Theorem 1. If is a signed measure on
, then there exist disjoint measurable subsets
such that
We call a positive set, denoted
, and
a negative set, denoted
, and we call the pair
a Hahn decomposition for
.
Call a set is
–null if it is positive and negative:
.
Define the symmetric difference by
We leave it as an exercise to verify that
Problem 1. Let be a signed measure on
and
,
be two Hahn decompositions for
. Show that
and
are
-null.
(Click for Solution)
Solution. Fix . Then
Using Theorem 1,
so , as required.
We now state the Jordan decomposition theorem.
Problem 2. Let be a finite signed measure on
. Construct unique finite measures
on
such that:
, and
- for any Hahn decomposition
of
,
for
and
for
.
We call the (unique) Jordan decomposition of
.
(Click for Solution)
Solution. Use Theorem 1 to construct a Hahn decomposition . Define
Then for any ,
Hence, .
Now fix any Hahn decomposition . Then
Fix . Then
Similarly, implies
.
Finally, we establish the uniqueness of the measures. Suppose
We need to check that . To that end, fix any Hahn decomposition
. For any
,
and
so that
Hence, for any ,
—Joel Kindiak, 7 Jan 26, 1212H
Leave a comment