A the beginning I want to remind you of things I think you already know and then go on to show the direction the course will be taking. Let me first try to set the context.
One basic notion I assume you are reasonably familiar with is that of a
metric space ([5] p.9). This consists of a set,
and a
distance function
The basic theory of metric spaces deals with properties of subsets (open, closed, compact, connected), sequences (convergent, Cauchy) and maps (continuous) and the relationship between these notions. Let me just remind you of one such result.
The basic example of a metric space is Euclidean space. Real
-dimensional Euclidean space,
, is the set of ordered
-tuples of real numbers
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Let us abstract this immediately to the notion of a normed vector
space, or normed space. This is a vector space
(over
or
) equipped with a norm, which is to say a function
The case of a finite dimensional normed space is not very
interesting because, apart from the dimension, they are all ``the
same''. We shall say (in general) that two norms
and
on
are equivalent of there exists
such that
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So, we are mainly interested in the infinite dimensional case. I
will start the course, in a slightly unorthodox manner, by
concentrating on one such normed space (really one class). Let
be
a metric space. The case of a continuous function,
(or
) is a special case of Proposition 1.1
above. We then define
In fact the same notation is generally used for the space of
complex-valued functions. If we want to distinguish between
these two possibilities we can use the more pedantic notation
and
. Now, the `obvious' norm on this
linear space is the supremum (or `uniform') norm
Here
is an arbitrary metric space. For the moment
is
supposed to be a ``physical'' space, something like
.
Corresponding to the finite-dimensionality of
we often
assume (or demand) that
is locally compact. This just
means that every point has a compact neighborhood, i.e., is in
the interior of a compact set. Whether locally compact or not we
can consider
If
is a normed linear space we are particularly interested in
the continuous linear functionals on
. Here `functional' just
means function but
is allowed to be `large' (not like
) so `functional' is used for historical reasons.
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In view of this identification, continuous linear functionals are
often said to be bounded. One of the important ideas that
we shall exploit later is that of `duality'. In particular this
suggests that it is a good idea to examine the totality of
bounded linear functionals on
. The dual space is
The natural norm on
is
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One of the basic questions I wish to pursue in the first part of the course
is: What is the dual of
for a locally compact metric
space
? The answer is given by Riesz' representation theorem, in terms
of (Borel) measures.
Let me give you a vague picture of `regularity of functions' which is what
this course is about, even though I have not introduced most of these
spaces yet. Smooth functions (and small spaces) are towards the
top. Duality flips up and down and as we shall see
the space of
Lebesgue square-integrable functions, is generally `in the middle'. What I
will discuss first is the right side of the diagramme, where we have the
space of continuous functions on
which vanish at infinity
and its dual space,
the space of finite Borel
measures. There are many other spaces that you may encounter, here I only
include test functions, Schwartz functions, Sobolev spaces and their duals;
is a general positive integer.
I have set the goal of understanding the dual space
of
, where
is a locally compact metric space. This will
force me to go through the elements of measure theory and Lebesgue
integration. It does require a little forcing!
The basic case of interest is
Then an obvious example of a
continuous linear functional on
is given by
Riemann integration, for instance over the unit cube
:
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One special feature of
, compared to general normed
spaces, is that there is a notion of positivity for its
elements. Thus
just means
.
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We can similarly split elements of the dual space into positive
and negative parts although it is a little bit more delicate. We say that
is positive if
For a general (real)
and for each
set
Conversely,
if
set
and
. Then
and
. Taking
the supremum over
,
, so we
find
Having shown this effective linearity on the positive functions we can obtain a linear functional by setting
The idea behind the definition of
is that
itself is, more or less,
``integration against a function'' (even though we do not
know how to interpret this yet). We are trying to throw away the
negative part of that function. The next step is to show that a
positive functional corresponds to a `measure' meaning a function
measuring the size of sets. To define this we really want to
evaluate
on the characteristic function of a set
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If
and
is open,
set1
Suppose we try to measure general sets in this way. We can do this by defining
To prove this we need to find enough continuous functions. I have relegated the proof of the following result to Problem 2.
Since
we conclude that
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Thus (1.14) holds when the
are open. In the general
case if
with the
open then, from the
definition,
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