Definition

Let AA and BB be . A completely positive contraction, often abbreviated CPC map, is a ϕ:AB\phi:A\to B satisfying

ϕ1.\|\phi\|\leq 1.

Thus every matrix amplification ϕ(n):Mn(A)Mn(B)\phi^{(n)}:M_n(A)\to M_n(B) is positive, while the contraction condition is imposed on the ordinary . Complete positivity then implies ϕcb=ϕ\|\phi\|_{\mathrm{cb}}=\|\phi\|, in the sense of the , so every CPC map is completely contractive. Neither multiplicativity nor unitality is required. In particular, a unital CPC map need not preserve products.

Norm tests

If AA is unital and ϕ\phi is completely positive, then

ϕ=ϕcb=ϕ(1A).\|\phi\|=\|\phi\|_{\mathrm{cb}}=\|\phi(1_A)\|.

Consequently such a map is CPC exactly when ϕ(1A)1B\phi(1_A)\leq 1_B, provided BB is unital. A unital completely positive map is automatically contractive. For a nonunital domain, the definition still uses ϕ1\|\phi\|\leq1; one may test it after passing to an appropriate unitization Brown–Ozawa, §1.5.

Examples and boundary cases

Every contractive is CPC. If V:KHV:K\to H is a contraction, the compression ϕ(T)=VTV\phi(T)=V^*TV from B(H)B(H) to B(K)B(K) is CPC; it is unital exactly when VV is an isometry. Multiplying the identity map by a scalar λ>1\lambda>1 preserves complete positivity but fails the contraction condition, so it is not CPC.

Role in approximation

Finite-dimensional approximation properties are commonly formulated using CPC maps because positivity controls order at every matrix level while contractivity prevents norms from growing during composition. Nuclearity, for example, can be expressed through point-norm approximations of the identity by CPC maps factoring through matrix algebras Brown–Ozawa, §2.3.

References
  1. Nathanial P. Brown and Narutaka Ozawa, C-Algebras and Finite-Dimensional Approximations*, Graduate Studies in Mathematics 88, American Mathematical Society, 2008. AMS DOI record. Relevant: §1.5 on completely positive maps and §2.3 on nuclear approximation.