Definition

Let AA be a unital complex CC^*-algebra, let (H+H,π,F)(H^+\oplus H^-,\pi,F) be a normalized , and write F+:H+HF^+:H^+\to H^- for its positive-to-negative part. For a pMn(A)p\in M_n(A) representing a , put p±=πn±(p)p^\pm=\pi_n^\pm(p). The compression

pFn+p+:p+H+npHnp^-F_n^+p^+:p^+H^{+n}\longrightarrow p^-H^{-n}

is , and the even index pairing is

[p],[H,π,F]=ind(pFn+p+).\langle[p],[H,\pi,F]\rangle=\operatorname{ind}(p^-F_n^+p^+).

It extends additively to differences of projections, giving a bilinear pairing K0(A)×K0(A)ZK_0(A)\times K^0(A)\to\mathbb Z.

Why the compression is Fredholm

Because [F,π(a)][F,\pi(a)] is compact, pFn+p+p^-F_n^+p^+ has p+Fnpp^+F_n^-p^- as an inverse modulo . The compressed operator is therefore Fredholm by Atkinson's characterization. Its index is unchanged under stabilization of pp, homotopy of the projection, compact perturbation of FF, and stable homotopy of the . These facts make the formula descend to and . Connes, Chapter IV, Section 1, Proposition 2(a).

For a class [p][q][p]-[q], the value is

ind(pFn+p+)ind(qFm+q+).\operatorname{ind}(p^-F_n^+p^+)-\operatorname{ind}(q^-F_m^+q^+).

This subtraction is essential: the pairing is defined on the Grothendieck group, not only on individual projections.

Geometric example

Let MM be a closed even-dimensional spin manifold and take the even Fredholm module obtained from its . A projection pMn(C(M))p\in M_n(C^\infty(M)) determines a EE. The compression represents the Dirac operator twisted by EE, so the pairing is its Fredholm index. This is the operator-theoretic bridge from a K0K_0-class to an integer index. Connes, Chapter IV, Section 1, example and Proposition 2.

For A=CA=\mathbb C, pairing the class of a finite-rank projection with an even cycle scales the cycle's basic index by the rank.

Conventions and scope

For nonunital AA, projections are taken in matrix algebras over the , with the scalar projection subtracted so that the class lies in K0(A)K_0(A). An unnormalized Fredholm module may be normalized or handled directly modulo compact operators before compression.

Switching which grading summand is called positive, or replacing the Fredholm-index convention dimkerTdimkerT\dim\ker T-\dim\ker T^* by its negative, reverses the displayed sign. The convention in the core agrees with Connes's Proposition 2(a).

References