Applying positive maps to $K$-theory This question is about mapping finitely generated projective modules over $C^*$ algebras (or K-theory classes - I don't mind much) under maps between algebras. If we have an idempotent matrix $P\in M_n(A)$ and a star algebra map $\phi:A\to B$ then taking $\phi(P)$ (applying to each entry) will give another idempotent. However suppose that we only have a completely positive map $\psi:A\to B$ -- what do we do then?
One possible way would be to use the KSGNS theorem to say that $\psi$ is given by a Hilbert bimodule structure on some $M$ together with an element $m\in M$. The module given by the applying the map to an $A$-module $E$ might be taken as $M\otimes_A E$ (or rather the conjugate of $M$ to get the sides right...). However this seems to be a very non-unique construction, and likely far too big. 
The reason I am interested in this is the problem of calculating characteristic classes (a la Connes) for algebras which simply do not have any nicely calculable $n$-cycles. It may be simplest to transfer the bundle to an easier to deal with algebra. (Just as classically we can define a cycle on a manifold by using an embedded submanifold). However then we run into the problem that we often only have CP maps, not algebra maps... I would be grateful for any assistance. 
 A: This is not really an answer, but an idea. I am not sure if it works, plus you need an extra assumption on the completely positive map. 
Definition: We call a completely positive map $\psi \colon A \to B$ of order zero if it is orthogonality preserving, i.e. if $ab = 0$ implies that $\psi(a)\,\psi(b) = 0$ for any two self-adjoint elements $a,b \in A$. 
Let $A$ and $B$ be unital $C^*$-algebras and let $\psi \colon A \to B$ be a completely positive order zero map. There is a powerful structure theorem for these maps, which can be found in Section 3.3 of the paper "Completely positive maps of order zero" by Wilhelm Winter and Joachim Zacharias: Let $C = C^*(\psi(A))$ be the $C^*$-algebra generated by the image of $\psi$, then $h = \psi(1_A) \in C$ commutes with $C$ and there is a $*$-homomorphism $\pi_{\psi} \colon A \to M(C) \cap \{h\}'$ such that 
$$
 h^{1/2}\,\pi_{\psi}(a)\,h^{1/2} = h\,\pi_{\psi}(a) = \pi_{\psi}(a)h = \psi(a)
$$
for all $a \in A$. This says that completely positive order zero maps can always be written as compressions of a $*$-homomorphism into a bigger algebra by a positive element. 
If you now start with a projection $p \in A$ (or in a matrix algebra over $A$), then you can consider the sequence 
$$
q_n = \left(h +\frac{1}{n}\right)^{-1}\psi(p) .
$$ 
This should get arbitrarily close to a projection in $B$ and hence can be cut down to an honest projection for $n$ big enough.
