Definition

Let AA and BB be . A ϕ:AB\phi:A\to B has order zero if it preserves orthogonality of positive elements:

a,bA+,ab=0ϕ(a)ϕ(b)=0.a,b\in A_+,\quad ab=0 \quad\Longrightarrow\quad \phi(a)\phi(b)=0.

Because positive aa and bb with ab=0ab=0 also satisfy ba=0ba=0, the condition is symmetric. Order zero does not mean that ϕ\phi vanishes, has zero algebraic order, or is multiplicative. Contractivity is not included in the convention used here; a map that is both contractive and order zero is called a CPC order-zero map.

Structure theorem

Let C=C(ϕ(A))C=C^*(\phi(A)). The order-zero structure theorem supplies a positive element hh in the center of the M(C)M(C) and a *-homomorphism πϕ:AM(C)\pi_\phi:A\to M(C) such that

ϕ(a)=πϕ(a)h=hπϕ(a).\phi(a)=\pi_\phi(a)h=h\pi_\phi(a).

For unital AA, one can take h=ϕ(1A)h=\phi(1_A). This factorization explains why order-zero maps retain much of the orthogonality behavior of *-homomorphisms without themselves preserving products Winter–Zacharias, Theorem 2.3.

Cone correspondence

Contractive completely positive order-zero maps ABA\to B correspond naturally to *-homomorphisms

C0((0,1])AB,C_0((0,1])\otimes A\longrightarrow B,

with the coordinate function on (0,1](0,1] sent, together with aa, to ϕ(a)\phi(a). This converts a nonlinear-looking orthogonality condition into ordinary multiplicative data Winter–Zacharias, Corollary 3.1.

Examples and near-misses

Every *-homomorphism has order zero, as does a positive scalar multiple of one. A compression aVaVa\mapsto V^*aV is completely positive but generally not order zero: two orthogonal positive operators can acquire overlapping compressions. Thus complete positivity alone does not preserve orthogonality.

References
  1. Wilhelm Winter and Joachim Zacharias, “Completely positive maps of order zero,” Münster Journal of Mathematics 2 (2009), 311–324. Author-institution record. Relevant: Definition 2.1, Theorem 2.3, and Corollary 3.1.