Hilbert C*-module explained
Hilbert C*-modules are mathematical objects that generalise the notion of Hilbert spaces(which are themselves generalisations of Euclidean space), in that they endow a linear space with an "inner product" that takes values in aC*-algebra.
They were first introduced in the work of Irving Kaplansky in 1953, which developed the theory for commutative, unital algebras (though Kaplansky observed that the assumption of a unit element was not "vital").[1]
In the 1970s the theory was extended to non-commutative C*-algebras independently by William Lindall Paschke[2] and Marc Rieffel, the latter in a paper that used Hilbert C*-modules to construct a theory of induced representations of C*-algebras.[3]
Hilbert C*-modules are crucial to Kasparov's formulation of KK-theory,[4] and provide the right framework to extend the notionof Morita equivalence to C*-algebras.[5] They can be viewed as the generalizationof vector bundles to noncommutative C*-algebras and as such play an important role in noncommutative geometry, notably in C*-algebraic quantum group theory,[6] [7] and groupoid C*-algebras.
Definitions
Inner-product C*-modules
Let
be a C*-algebra (not assumed to be commutative or unital), its
involution denoted by
. An
inner-product
-module (or
pre-Hilbert
-module) is a
complex linear space
equipped with a compatible right
-module structure, together with a map
\langle ⋅ , ⋅ \rangleA:E x E → A
that satisfies the following properties:
,
,
in
, and
,
in
:
\langlex,y\alpha+z\beta\rangleA=\langlex,y\rangleA\alpha+\langlex,z\rangleA\beta
(i.e. the inner product is
-linear in its second argument).
,
in
, and
in
:
\langlex,ya\rangleA=\langlex,y\rangleAa
,
in
:
\langlex,y\rangleA=\langley,x
from which it follows that the inner product is conjugate linear in its first argument (i.e. it is a sesquilinear form).
in
:
in the sense of being a positive element of A, and
\langlex,x\rangleA=0\iffx=0.
(An element of a C*-algebra
is said to be
positive if it is
self-adjoint with non-negative
spectrum.)
[8] [9] Hilbert C*-modules
An analogue to the Cauchy–Schwarz inequality holds for an inner-product
-module
:
[10] \langlex,y\rangleA\langley,x\rangleA\leq\Vert\langley,y\rangleA\Vert\langlex,x\rangleA
for
,
in
.
On the pre-Hilbert module
, define a norm by
\Vertx\Vert=\Vert\langlex,x\rangleA
.
The norm-completion of
, still denoted by
, is said to be a
Hilbert
-module or a
Hilbert C*-module over the C*-algebra
.The Cauchy–Schwarz inequality implies the inner product is jointly continuous in norm and can therefore be extended to the completion.
The action of
on
is continuous: for all
in
Similarly, if
is an
approximate unit for
(a
net of self-adjoint elements of
for which
and
tend to
for each
in
), then for
in
Whence it follows that
is
dense in
, and
when
is unital. Let
\langleE,E\rangleA=\operatorname{span}\{\langlex,y\rangleA\midx,y\inE\},
then the closure of
is a two-sided ideal in
. Two-sided ideals are C*-subalgebras and therefore possess approximate units. One can verify that
is dense in
. In the case when
is dense in
,
is said to be
full. This does not generally hold.
Examples
Hilbert spaces
Since the complex numbers
are a C*-algebra with an involution given by complex conjugation, a complex Hilbert space
is a Hilbert
-module under scalar multipliation by complex numbers and its inner product.
Vector bundles
If
is a locally compact Hausdorff space and
a
vector bundle over
with projection
a Hermitian metric
, then the space of continuous sections of
is a Hilbert
-module. Given sections
of
and
the right action is defined by
\sigmaf(x)=\sigma(x)f(\pi(x)),
and the inner product is given by
\langle\sigma,\rho\rangleC(X)(x):=g(\sigma(x),\rho(x)).
The converse holds as well: Every countably generated Hilbert C*-module over a commutative unital C*-algebra
is isomorphic to the space of sections vanishing at infinity of a continuous field of Hilbert spaces over
.
C*-algebras
Any C*-algebra
is a Hilbert
-module with the action given by right multiplication in
and the inner product
. By the C*-identity, the Hilbert module norm coincides with C*-norm on
.
The (algebraic) direct sum of
copies of
can be made into a Hilbert
-module by defining
\langle(ai),(bi)\rangleA=
bi.
If
is a projection in the C*-algebra
, then
is also a Hilbert
-module with the same inner product as the direct sum.
The standard Hilbert module
One may also consider the following subspace of elements in the countable direct product of
\ell2(A)=l{H}A=\{(ai)|
aiconvergesinA\}.
Endowed with the obvious inner product (analogous to that of
), the resulting Hilbert
-module is called the
standard Hilbert module over
.
The standard Hilbert module plays an important role in the proof of the Kasparov stabilization theorem which states that for any countably generated Hilbert
-module
there is an isometric isomorphism
E ⊕ \ell2(A)\cong\ell2(A).
[11] Maps between Hilbert modules
Let
and
be two Hilbert modules over the same C*-algebra
. These are then Banach spaces, so it is possible to speak of the Banach space of bounded linear maps
, normed by the operator norm.
The adjointable and compact adjointable operators are subspaces of this Banach space defined using the inner product structures on
and
.
In the special case where
is
these reduce to bounded and
compact operators on Hilbert spaces respectively.
Adjointable maps
A map (not necessarily linear)
is defined to be adjointable if there is another map
, known as the adjoint of
, such that for every
and
,
\langlef,Te\rangle=\langleT*f,e\rangle.
Both
and
are then automatically linearand also
-module maps. The closed graph theorem can be used to show that they are also bounded.
Analogously to the adjoint of operators on Hilbert spaces,
is unique (if it exists) and itself adjointable with adjoint
. If
is a second adjointable map,
is adjointable with adjoint
.
The adjointable operators
form a subspace
of
, which is complete in the operator norm.
In the case
, the space
of adjointable operators from
to itself is denoted
, and is a C*-algebra.
[12] Compact adjointable maps
Given
and
, the map
|f\rangle\langlee|\colonE\toF
is defined, analogously to the
rank one operators of Hilbert spaces, to be
g\mapstof\langlee,g\rangle.
This is adjointable with adjoint
.
The compact adjointable operators
are defined to be the closed span of
\{|f\rangle\langlee|\mide\inE, f\inF\}
in
.
As with the bounded operators,
is denoted
. This is a (closed, two-sided) ideal of
.
[13] C*-correspondences
If
and
are C*-algebras, an
C*-correspondenceis a Hilbert
-module equipped with a left action of
by adjointable maps that is faithful. (NB: Some authors require the left action to be non-degenerate instead.) These objects are used in the formulation of Morita equivalence for C*-algebras, see applications in the construction of Toeplitz and Cuntz-Pimsner algebras,
[14] and can be employed to put the structure of a bicategory on the collection of C*-algebras.
[15] Tensor products and the bicategory of correspondences
If
is an
and
a
correspondence,the algebraic tensor product
of
and
as vector spaces inherits left and right
- and
-module structures respectively.
It can also be endowed with the
-valued sesquilinear form defined on pure tensors by
\langlee\odotf,e'\odotf'\rangleC:=\langlef,\langlee,e'\rangleBf\rangleC.
This is positive semidefinite, and the Hausdorff completion of
in the resulting seminorm is denoted
. The left- and right-actions of
and
extend to make this an
correspondence.
[16] The collection of C*-algebras can then be endowed with the structure of a bicategory, with C*-algebras as objects,
correspondences as arrows
, and isomorphisms of correspondences (bijective module maps that preserve inner products) as 2-arrows.
[17] Toeplitz algebra of a correspondence
Given a C*-algebra
, and an
correspondence
,its Toeplitz algebra
is defined as the universal algebrafor Toeplitz representations (defined below).
The classical Toeplitz algebra can be recovered as a special case, and the Cuntz-Pimsner algebrasare defined as particular quotients of Toeplitz algebras.[18]
In particular, graph algebras, crossed products by
, and the Cuntz algebras are all quotients of specific Toeplitz algebras.
Toeplitz representations
A Toeplitz representation[19] of
in a C*-algebra
is a pair
of a linear map
and a homomorphism
such that
is "isometric":
S(e)*S(f)=\phi(\langlee,f\rangle)
for all
,
resembles a bimodule map:
and
for
and
.
Toeplitz algebra
The Toeplitz algebra
is the universal Toeplitz representation.That is, there is a Toeplitz representation
of
in
such that if
is any Toeplitz representationof
(in an arbitrary algebra
) there is a unique *-homomorphism
such that
and
.
[20] Examples
If
is taken to be the algebra of complex numbers, and
the vector space
, endowed with the natural
-bimodule structure, the corresponding Toeplitz algebrais the universal algebra generated by
isometries with mutually orthogonal range projections.
[21] In particular,
is the universal algebra generated by a single isometry, which is the classical Toeplitz algebra.
See also
References
- Book: Lance, E. Christopher. Hilbert C*-modules: A toolkit for operator algebraists . London Mathematical Society Lecture Note Series. 1995 . Cambridge University Press . Cambridge, England.
- Book: Wegge-Olsen, N. E.. K-Theory and C*-Algebras . Oxford University Press . 1993.
- Book: Brown . Nathanial P. . Ozawa . Narutaka . 2008 . C*-Algebras and Finite-Dimensional Approximations . American Mathematical Society.
- Buss . Alcides . Meyer . Ralf . Zhu . Chenchang . 2013 . A higher category approach to twisted actions on c* -algebras . Proceedings of the Edinburgh Mathematical Society . 56 . 2 . 387–426 . 10.1017/S0013091512000259. 0908.0455 .
- Fowler . Neal J. . Raeburn . Iain . 1999 . The Toeplitz algebra of a Hilbert bimodule . Indiana University Mathematics Journal . 48 . 1 . 155–181. 10.1512/iumj.1999.48.1639 . 24900141 . math/9806093 .
External links
Notes and References
- Kaplansky. I.. Irving Kaplansky . Modules over operator algebras. American Journal of Mathematics. 75. 4. 839–853. 1953. 10.2307/2372552. 2372552.
- Paschke. W. L.. Inner product modules over B*-algebras. Transactions of the American Mathematical Society. 182. 443–468. 1973. 10.2307/1996542. 1996542.
- Rieffel. M. A.. Induced representations of C*-algebras. Advances in Mathematics. 13. 176–257. 1974. 10.1016/0001-8708(74)90068-1. free . 2.
- Kasparov. G. G.. Hilbert C*-modules: Theorems of Stinespring and Voiculescu. Journal of Operator Theory. 4. 133–150. Theta Foundation. 1980.
- Rieffel. M. A.. Morita equivalence for operator algebras. Proceedings of Symposia in Pure Mathematics. 38. 176–257. American Mathematical Society. 1982.
- Baaj. S.. Skandalis, G.. Unitaires multiplicatifs et dualité pour les produits croisés de C*-algèbres. Annales Scientifiques de l'École Normale Supérieure. 26. 4. 425–488. 1993. 10.24033/asens.1677. free.
- Woronowicz. S. L.. S. L. Woronowicz. Unbounded elements affiliated with C*-algebras and non-compact quantum groups. Communications in Mathematical Physics. 136. 399–432. 1991. 10.1007/BF02100032. 1991CMaPh.136..399W. 2 . 118184597.
- Book: Arveson, William. William Arveson
. William Arveson. An Invitation to C*-Algebras. Springer-Verlag. 1976. 35.
- In the case when
is non-unital, the spectrum of an element is calculated in the C*-algebra generated by adjoining a unit to
.
- This result in fact holds for semi-inner-product
-modules, which may have non-zero elements
such that
, as the proof does not rely on the nondegeneracy property.
- Kasparov. G. G.. Hilbert C*-modules: Theorems of Stinespring and Voiculescu. Journal of Operator Theory. 4. 133–150. ThetaFoundation. 1980.
- Wegge-Olsen 1993, pp. 240-241.
- Wegge-Olsen 1993, pp. 242-243.
- Brown, Ozawa 2008, section 4.6.
- Buss, Meyer, Zhu, 2013, section 2.2.
- Brown, Ozawa 2008, pp. 138-139.
- Buss, Meyer, Zhu 2013, section 2.2.
- Brown, Ozawa, 2008, section 4.6.
- Fowler, Raeburn, 1999, section 1.
- Fowler, Raeburn, 1999, Proposition 1.3.
- Brown, Ozawa, 2008, Example 4.6.10.