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406 D. Kucerovsky / Journal of Functional Analysis 236 (2006) 395–408<br />

Definition. Let B be a σ -unital stab<strong>le</strong> C ∗ -algebra, and <strong>le</strong>t A be a separab<strong>le</strong> C ∗ -algebra. A stabilized<br />

ungra<strong>de</strong>d Fredholm cyc<strong>le</strong> in KK 1 (A, B) is a trip<strong>le</strong> (M(B), φ, F ) where φ is a homomorphism<br />

from A to M(B), and F ∈ M(B) is such that:<br />

(i) (F ∗ F − F)φ(a)∈ B;<br />

(ii) [F,φ(a)]∈B; and<br />

(iii) φ(a)(F − F ∗ ) ∈ B.<br />

A cyc<strong>le</strong> is said to be trivial if the above three expressions are actually zero.<br />

We can summarize the above <strong>de</strong>finition by saying that Fredholm trip<strong>le</strong>s are specified by a homomorphism<br />

φ and an operator that is an approximate projection: more specifically, an e<strong>le</strong>ment<br />

of Iφ that becomes a projection in Iφ/Jφ, where<br />

Iφ := m ∈ M(B): φ(a),m ∈ B for all a ∈ A ,<br />

Jφ := m ∈ M(B): φ(a)m∈ B for all a ∈ A .<br />

Sometimes, Fredholm trip<strong>le</strong>s in KK 1 (A, B) are specified by self-adjoint approximate unitaries<br />

instead, but this is equiva<strong>le</strong>nt since self-adjoint unitaries map to projections un<strong>de</strong>r the map<br />

u ↦→ 1 + u/2. For more information on the various pictures of KK-theory, and the interesting<br />

transformations that re<strong>la</strong>te one to the other, see [2].<br />

In some applications, cyc<strong>le</strong>s arise which are not stabilized, meaning that M(B) is rep<strong>la</strong>ced<br />

by the C ∗ -algebra of adjointab<strong>le</strong> operators on some given Hilbert B-mo<strong>du</strong><strong>le</strong>, but it can be shown<br />

that un<strong>de</strong>r an appropriate <strong>de</strong>finition of equiva<strong>le</strong>nce unstabilized cyc<strong>le</strong>s are neverthe<strong>le</strong>ss always<br />

equiva<strong>le</strong>nt to stabilized cyc<strong>le</strong>s.<br />

There are a number of apparently quite different equiva<strong>le</strong>nce re<strong>la</strong>tions on KK 1 -cyc<strong>le</strong>s, and<br />

the one most re<strong>le</strong>vant to our situation is given by “compact” perturbation, addition of <strong>de</strong>generate<br />

cyc<strong>le</strong>s, and unitary equiva<strong>le</strong>nce by multiplier unitaries. (By “compact” perturbation is meant<br />

perturbation of the operator F by e<strong>le</strong>ments of Jφ.)<br />

Definition. We say that a Fredholm trip<strong>le</strong> (M(B), φ, F ) is unital if and only φ(1) = 1 + b and<br />

F = 1 + b ′ for some b,b ′ ∈ B.<br />

C<strong>le</strong>arly this is an extremely strong property. It is, however, of interest in that it p<strong>la</strong>ys a ro<strong>le</strong> in<br />

the <strong>de</strong>finition of the absorption property for a Fredholm trip<strong>le</strong>.<br />

Definition. A unital Fredholm trip<strong>le</strong> F := (M(B), φ, F ) is absorbing if F ⊕ T is unitarily<br />

equiva<strong>le</strong>nt to F for all unital trivial cyc<strong>le</strong>s T . A nonunital Fredholm cyc<strong>le</strong> F is absorbing if it<br />

has this property for all trivial cyc<strong>le</strong>s T .<br />

One observes that there is a natural isomorphism<br />

KK 1 (A, B) → Ext(A, B),<br />

(φ, F ) ↦→ π(FφF ∗ )

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