Definition

Let AA and BB be . A bounded Φ:AB\Phi:A\to B is completely positive if it is for every integer n1n\geq1. Explicitly, for each nn, the entrywise amplification

Φ(n):Mn(A)Mn(B),[aij][Φ(aij)],\Phi^{(n)}:M_n(A)\longrightarrow M_n(B),\qquad [a_{ij}]\longmapsto[\Phi(a_{ij})],

must carry positive elements to positive elements. Complete positivity therefore controls positivity simultaneously at every matrix level, not only on AA itself. The definition does not require Φ\Phi to preserve the identity, be multiplicative, or be normal when the algebras are von Neumann algebras.

Stinespring characterization

When B=B(H)B=B(H), Stinespring's theorem characterizes complete positivity by a factorization

Φ(a)=Vπ(a)V,\Phi(a)=V^*\pi(a)V,

where π\pi is a of AA on a KK and V:HKV:H\to K is bounded. With the usual minimality condition the factorization is unique up to unitary equivalence Paulsen, Chapter 4.

Closure properties and examples

Every is completely positive. Compositions and nonnegative of completely positive maps are completely positive, as are maps aVπ(a)Va\mapsto V^*\pi(a)V. A ACA\to\mathbb C is automatically completely positive. These facts make CP maps stable under the constructions used for representations and quantum operations.

Positivity is not enough
References
  1. Vern Paulsen, Completely Bounded Maps and Operator Algebras, Cambridge University Press, 2002. DOI record. Relevant: Chapters 2–4 on matrix positivity, completely positive maps, and Stinespring dilation.
  2. Masamichi Takesaki, Theory of Operator Algebras I, Springer, 1979. DOI record. Relevant: Chapter IV on completely positive maps.