Definition

Let AA be a unital , and form

U(A)=n1U(Mn(A))U_\infty(A)=\bigcup_{n\geq1}U(M_n(A))

using the inclusions udiag(u,1)u\mapsto\operatorname{diag}(u,1). The group K1(A)K_1(A) is the set of path components of U(A)U_\infty(A), with addition induced by block sum. Equivalently, its elements are stable homotopy classes of in over AA. For nonunital AA, define

K1(A)=ker(K1(A~)K1(C))K_1(A)=\ker\bigl(K_1(\widetilde A)\to K_1(\mathbb C)\bigr)

using the scalar quotient from the .

Representative calculus

A nonunital class can be represented by a unitary uMn(A~)u\in M_n(\widetilde A) whose scalar image is 1n1_n. Stabilization permits adjoining identity blocks, and homotopy is taken through unitaries after a common stabilization. Although block sum defines the group law, [uv]=[u]+[v][uv]=[u]+[v] for stabilized unitaries. These equivalent models are proved in Blackadar, Chapter IV.

Basic properties and examples

The functor K1K_1 is homotopy invariant, matrix stable, and strongly Morita invariant. One has K1(C)=0K_1(\mathbb C)=0, while the winding number gives

K1(C(S1))Z.K_1(C(S^1))\cong\mathbb Z.

Continuous *-homomorphisms carry unitary representatives to unitary representatives and therefore induce on K1K_1.

Conventions and scope

For a nonunital algebra, a K1K_1-representative generally belongs to a matrix algebra over A~\widetilde A, not to AA itself. Definitions using connected components of stable invertibles instead of stable unitaries give the same group by polar decomposition. The adjective “odd” reflects Bott periodicity and the odd index pairing; it is not an additional grading on AA.

References
  1. Bruce Blackadar, K-Theory for Operator Algebras, 2nd ed., Cambridge University Press, 1998. DOI record. Relevant: Chapter IV on K1K_1, stable unitary groups, and Bott periodicity.
  2. N. E. Wegge-Olsen, K-Theory and C-Algebras: A Friendly Approach*, Oxford University Press, 1993. DOI record. Relevant: Chapter 7 on K1K_1 and suspensions.