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Taken from C*-algebras and Operator Theory by Gerald Murphy.
If and
are vector spaces, we denote by
their algebraic tensor product. This is linearly spanned by the elements
(
,
).
One reason why tensor products are useful is that they turn bilinear maps (a bilinear map has
) into linear maps (
). More precisely, if
is a bilinear map, where
and
are vector spaces, then there is a unique linear map
such that
for all
and
.
If are linear functionals on the vector spaces
respectively, then there is a unique linear functional
on
such that
since the function
,
,
is bilinear.
Suppose that the finite sum , where
and
. If
are linearly independent, then
. For, in this case, there exist linear functionals
such that
. If
is linear, we have
.
Thus for arbitrary
and this shows that all the
.
Similarly if the finite sum with the
linearly independent, implies that all the
are zero.
Taken from C*-algebras and Operator Theory by Gerald Murphy.
We prepare the way for the density theorem with some useful results on strong convergence.
Theorem 4.3.1
If is a Hilbert space, the involution
is strongly continuous when restricted to the set of normal operators of
.
Proof
Let and suppose that
are normal operators in
. Then
If is a net of normal operators strongly convergent to a normal operator
, then the net
is convergent to
and the net
is convergent to
, so
is convergent to
. Therefore,
is strongly convergent to
Taken from C*-algebras and Operator Theory by Gerald Murphy.
Preparatory to our introduction of the weak and ultraweak topologiesm we show now that is the dual of
, and
is the dual of
.
Let be a Hilbert space, and suppose that
. It follows from Theorem 2.4.16 (https://jpmccarthymaths.wordpress.com/2011/01/18/c-algebras-and-operator-theory-2-4-compact-hilbert-space-operators/) that the function
,
,
is linear and bounded, and . We therefore have a map
,
,
which is clearly linear and norm-decreasing. We call this map the canonical map from to
.
Theorem 4.2.1
If is a Hilbert space, then the canonical map from
to
is an isometric linear isomorphism.
Taken from C*-algebras and Operator Theory by Gerald Murphy.
A useful way of thinking of the theory of C*-algebras is as “non-commutative topology”. This is justified by the correspondence between abelian C*-algebras and locally compact Hausdorff spaces given by the Gelfand representation. The algebras studied in this chapter, von Neumann algebras, are a class of C*-algebras whose study can be thought of as “non-commutative measure theory”. The reason for the analogy in this case is that the abelian von Neumann algebras are (up to isomorphism) of the form , where
is a measure space.
The theory of von Neumann algebras is a vast and very well-developed area of the theory of operator algebras. We shall be able only to cover some of the basics. The main results of this chapter are the von Neumann double commutant theorem and the Kaplansky density theorem.
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Question 1
Let be normal elements of a C*-algebra
, and
an element of
such that
. Show that
, using Fuglede’s theorem and the fact that the element
is normal in and commutes with
.
This more general result is called the Putnam-Fuglede theorem.
Solution
Fuglede’s theorem states that if is a normal element commuting with some
, then
also commutes with
. Now we can show that
using the normality of
and
. We can also show that
and
commute. Hence by the theorem
and
commute. This yields:
.
Taking conjugates:
,
as required
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In this section we introduce the important GNS construction and prove that every C*-algebra can be regarded as a C*-subalgebra of for some Hilbert space
. It is partly due to this concrete realisation of the C*-algebras that their theory is so accessible in comparison with more general Banach spaces.
A representation of a C*-algebra is a pair
where
is a Hilbert space and
is a *-homomorphism. We say
is faithful if
is injective.
For abelian C*-algebras we were able to completely determine the structure of the algebra in terms of the character space, that is, in terms of the one-dimensional representations. For the non-abelian case this is quite inadequate, and we have to look at representations of arbitrary dimension. There is a deep inter-relationship between the representations and the positive linear functionals of a C*-algebra. Representations will be defined and some aspects of this inter-relationship investigated in the next section. In this section we establish the basis properties of positive linear functionals.
I’m getting the impression that the bra-ket notation is more useful for linear ON THE LEFT!
An approximate unit for a C*-algebra is an increasing net of positive elements in the closed unit ball of
such that
for all
.
Example
Let be a Hilbert space with infinite orthonormal basis
. The C*-algebra
is now non-unital. If
is the projection onto
, then the increasing sequence
is an approximate unit for
. It will suffice to show that
if
, since
is dense in
. Now if
, there exist
,
such that:
.
Hence,
.
Since for all
, therefore for each $k$:
.
Hence, .
Question 1
Let be a Banach algebra such that for all
the implication
or
holds. Let ,
be linear mappings from
to itself such that for all
,
,
, and
.
Show that and
are necessarily continuous.
Question 2
Let be a unital C*-algebra.
(a)
If are positive elements of
, show that
.
Solution (Wills)
For elements of a unital algebra
:
If then
so that
Now if , for any
,
. Hence
and the result follows (note that
need not be hermitian)
Let be a compact Hausdorff space and
a Hilbert Space. A spectral measure
relative to
is a map from the
-algebra of all Borel sets of
to the set of projections in
such that
,
;
for all Borel sets
of
;
- for all
, the function
, is a regular Borel complex measure on
.
A Borel measure is a measure defined on Borel sets. If every Borel set in
is both outer and inner regular, then
is called regular. A measurable
is inner and outer regular if
, and
Denote by the Banach space of all regular Borel complex measures on
, and by
the C*-algebra of all bounded Borel-measurable complex-valued functions on
(I assume with respect to the Borel
-algebra on
).

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