**algebraic quantum field theory** (perturbative, on curved spacetimes, homotopical)

**quantum mechanical system**, **quantum probability**

**interacting field quantization**

(geometry $\leftarrow$ Isbell duality $\to$ algebra)

The generalization of the process of one-point compactification of possibly non-compact topological spaces from topology to non-commutative topology is the process of adding units to possibly non-unital C*-algebras, thought of as formal duals of non-commutative spaces in noncommutative topology.

For $(A, {\Vert \cdot \Vert_{A}})$ a non-unital C*-algebra, its **unitisation** is the $C^{\ast}$-algebra whose underlying vector space is the direct sum

$A^{+} \coloneqq A \oplus \mathbb{C}$

of $A$ with the field of complex numbers, equipped with the multiplication law

$(a_{1} \oplus z_{1}) \cdot (a_{2} \oplus z_{2})
\coloneqq (a_{1} a_{2} + z_{2} a_{1} + z_{1} a_{2}) \oplus z_{1} z_{2},$

and the involution

$(a \oplus z)^\ast \coloneqq a^{\ast} \oplus \overline{z}$

(complex conjugation is taking place on the right). This really is a $C^\ast$-algebra. The norm can be characterised as

${\Vert a \oplus z \Vert}_{A^{+}}
= {\Vert L_{a} + z \cdot \operatorname{Id}_{A} \Vert}_{\mathcal{B}(A)}
\coloneqq \sup_{b \in A, \Vert b \Vert_{A} \leq 1} \Vert a b + z b \Vert_{A}.$

if $A$ does not have a multiplicative unit. (Note that the operatornorm vanishes on $1_A\oplus -1_{\mathbb{C}}$ if $A$ does have a multiplicative unit). For $C^\ast$-algebras with a multiplicative unit one can show that the norm equals

$\Vert a\oplus z \Vert_{A^+} = \max\{\|a+z1_A\|,|z|\}$

For $X$ a locally compact Hausdorff topological space and $C(X)$ its possibly non-unital C*-algebra of functions, then

$(C_0(X))^+ \simeq C_0(X) \oplus \mathbb{C} \simeq C(X^+)$

this is equivalently the unital $C^\ast$-algebra of functions on the one-point compactification of $X$.

There is hence a canonical projection

$i^\ast \colon C(X^+) \to \mathbb{C}$

The topological K-theory of $X$ is the kernel of the induced map in operator K-theory

$K(X) \simeq ker(i^\ast) \simeq K(C_0(X))
\,.$

The unitisation of $A$ comes with a canonical projection homomorphism of C*-algebras

$i^\ast_A \colon A^+ \to \mathbb{C}$

given by

$(a + z) \mapsto z
\,.$

Dually this corresponds to the inclusion of the “point at infinity”.

The map $i^\ast_A \colon A^+ \to \mathbb{C}$ of remark induces a homomorphism of operator K-theory groups of the form

$K(i^\ast_A) \colon K(A^+) \to K(\mathbb{C}) \simeq \mathbb{Z}
\,.$

The kernel of this map is the operator K-theory of the original possibly non-unital $C^\ast$-algebra $A$:

$K(A) \coloneqq ker(K(i^\ast_A))
\,.$

Heuristically it is clear that this is the “compactly suppported” K-theory of the possibly non-compact non-commutative space given by the algebra $A$. This statement has been made precise for instance in (Emerson 07, theorem 3.8)):

For $X$ a locally compact Hausdorff topological space, there is a natural isomorphism

$K(X) \simeq [X,Fred]_{cs}
\,,$

where on the right we homotopy classes of maps of compact support into the classifying space for K-theory (space of Fredholm operators).

- Heath Emerson,
*Equivariant representable K-theory*(arXiv:0710.1410)

Last revised on November 25, 2017 at 18:50:55. See the history of this page for a list of all contributions to it.