Universal C*-algebra
In mathematics, the Cuntz algebra
, named after Joachim Cuntz, is the universal C*-algebra generated by
isometries of an infinite-dimensional Hilbert space
satisfying certain relations.[1] These algebras were introduced as the first concrete examples of a separable infinite simple C*-algebra, meaning as a Hilbert space,
is isometric to the sequence space
![{\displaystyle l^{2}(\mathbb {N} )}](https://wikimedia.org/api/rest_v1/media/math/render/svg/be62598dfdf4ee93a4c8b4e332f6f235f8f21add)
and it has no nontrivial closed ideals. These algebras are fundamental to the study of simple infinite C*-algebras since any such algebra contains, for any given n, a subalgebra that has
as quotient.
Definitions
Let n ≥ 2 and
be a separable Hilbert space. Consider the C*-algebra
generated by a set
![{\displaystyle \{S_{i}\}_{i=1}^{n}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/acd595d039dea6794910f76a82dcb5be11b8a343)
of isometries (i.e.
) acting on
satisfying
![{\displaystyle \sum _{i=1}^{n}S_{i}S_{i}^{*}=1.}](https://wikimedia.org/api/rest_v1/media/math/render/svg/dc8cbaf8715654ddb54d7669d850ccce7f771fef)
This universal C*-algebra is called the Cuntz algebra, denoted by
.
A
of it is infinite.
![{\displaystyle {\mathcal {O}}_{n}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/23c1482aadf309ab3fe04327732c45c8fb8b30c7)
is a separable, simple, purely infinite C*-algebra. Any simple infinite C*-algebra contains a subalgebra that has
![{\displaystyle {\mathcal {O}}_{n}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/23c1482aadf309ab3fe04327732c45c8fb8b30c7)
as a quotient.
Properties
Classification
The Cuntz algebras are pairwise non-
isomorphic
, i.e.
![{\displaystyle {\mathcal {O}}_{n}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/23c1482aadf309ab3fe04327732c45c8fb8b30c7)
and
![{\displaystyle {\mathcal {O}}_{m}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/23c152e895fbdb7467badbf1bc050e87b7a2f722)
are non-isomorphic for
n ≠
m. The
K0 group of
![{\displaystyle {\mathcal {O}}_{n}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/23c1482aadf309ab3fe04327732c45c8fb8b30c7)
is
![{\displaystyle \mathbb {Z} /(n-1)\mathbb {Z} }](https://wikimedia.org/api/rest_v1/media/math/render/svg/c8f78b67b648a18f573a47e76b0365b24803a88b)
, the
,
![{\displaystyle {\mathcal {O}}_{n}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/23c1482aadf309ab3fe04327732c45c8fb8b30c7)
and
![{\displaystyle {\mathcal {O}}_{m}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/23c152e895fbdb7467badbf1bc050e87b7a2f722)
are non-isomorphic.
Relation between concrete C*-algebras and the universal C*-algebra
Theorem. The concrete C*-algebra
is isomorphic to the universal C*-algebra
generated by n generators s1... sn subject to relations si*si = 1 for all i and ∑ sisi* = 1.
The proof of the theorem hinges on the following fact: any C*-algebra generated by n isometries s1... sn with orthogonal ranges contains a copy of the
UHF algebra
![{\displaystyle {\mathcal {F}}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/205d4b91000d9dcf1a5bbabdfa6a8395fa60b676)
type
n∞. Namely
![{\displaystyle {\mathcal {F}}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/205d4b91000d9dcf1a5bbabdfa6a8395fa60b676)
is spanned by words of the form
![{\displaystyle s_{i_{1}}\cdots s_{i_{k}}s_{j_{1}}^{*}\cdots s_{j_{k}}^{*},k\geq 0.}](https://wikimedia.org/api/rest_v1/media/math/render/svg/b5adc7f3897a9316b293a204fe914f1f12a745a8)
The *-subalgebra
, being approximately finite-dimensional, has a unique C*-norm. The subalgebra
plays role of the space of Fourier coefficients for elements of the algebra. A key technical lemma, due to Cuntz, is that an element in the algebra is zero
if and only if all its Fourier coefficients vanish. Using this, one can show that the quotient map from
to
is injective, which proves the theorem.
The UHF algebra
has a non-unital subalgebra
that is canonically isomorphic to
itself: In the Mn stage of the direct system defining
, consider the rank-1 projection e11, the matrix that is 1 in the upper left corner and zero elsewhere. Propagate this projection through the direct system. At the Mnk stage of the direct system, one has a rank nk − 1 projection. In the direct limit, this gives a projection P in
. The corner
![{\displaystyle P{\mathcal {F}}P={\mathcal {F'}}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/3d697d70fad953af0a83ac97b99bf4d27389cc8a)
is isomorphic to
. The *-endomorphism Φ that maps
onto
is implemented by the isometry s1, i.e. Φ(·) = s1(·)s1*.
is in fact the crossed product of
with the endomorphism Φ.
Cuntz algebras to represent direct sums
The relations defining the Cuntz algebras align with the definition of the biproduct for preadditive categories. This similarity is made precise in the C*-category of unital *-endomorphisms over C*-algebras. The objects of this category are unital *-endomorphisms, and morphisms are the elements
, where
if
for every
. A unital *-endomorphism
is the direct sum of endomorphisms
if there are isometries
satisfying the
relations and
![{\displaystyle \rho (x)=\sum _{k=1}^{n}S_{k}\sigma _{k}(x)S_{k}^{*},\forall x\in A.}](https://wikimedia.org/api/rest_v1/media/math/render/svg/14554d24a2ce530a292507606f3deb1e9c517cd4)
In this direct sum, the inclusion morphisms are
, and the projection morphisms are
.
Generalisations
Cuntz algebras have been generalised in many ways. Notable amongst which are the Cuntz–Krieger algebras, graph C*-algebras and k-graph C*-algebras.
Applied mathematics
In
subband filter with exact reconstruction give rise to representations of a Cuntz algebra. The same filter also comes from the
multiresolution analysis construction in
wavelet theory.
[2]
See also
References