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In mathematics a positive map is a map between
C*-algebra In mathematics, specifically in functional analysis, a C∗-algebra (pronounced "C-star") is a Banach algebra together with an involution satisfying the properties of the adjoint. A particular case is that of a complex algebra ''A'' of continu ...
s that sends positive elements to positive elements. A completely positive map is one which satisfies a stronger, more robust condition.


Definition

Let A and B be
C*-algebra In mathematics, specifically in functional analysis, a C∗-algebra (pronounced "C-star") is a Banach algebra together with an involution satisfying the properties of the adjoint. A particular case is that of a complex algebra ''A'' of continu ...
s. A linear map \phi: A\to B is called positive map if \phi maps positive elements to positive elements: a\geq 0 \implies \phi(a)\geq 0. Any linear map \phi:A\to B induces another map :\textrm \otimes \phi : \mathbb^ \otimes A \to \mathbb^ \otimes B in a natural way. If \mathbb^\otimes A is identified with the C*-algebra A^ of k\times k-matrices with entries in A, then \textrm\otimes\phi acts as : \begin a_ & \cdots & a_ \\ \vdots & \ddots & \vdots \\ a_ & \cdots & a_ \end \mapsto \begin \phi(a_) & \cdots & \phi(a_) \\ \vdots & \ddots & \vdots \\ \phi(a_) & \cdots & \phi(a_) \end. We say that \phi is k-positive if \textrm_ \otimes \phi is a positive map, and \phi is called completely positive if \phi is k-positive for all k.


Properties

* Positive maps are monotone, i.e. a_1\leq a_2\implies \phi(a_1)\leq\phi(a_2) for all
self-adjoint In mathematics, and more specifically in abstract algebra, an element ''x'' of a *-algebra is self-adjoint if x^*=x. A self-adjoint element is also Hermitian, though the reverse doesn't necessarily hold. A collection ''C'' of elements of a sta ...
elements a_1,a_2\in A_. * Since -\, a\, _A 1_A \leq a \leq \, a\, _A 1_A for all
self-adjoint In mathematics, and more specifically in abstract algebra, an element ''x'' of a *-algebra is self-adjoint if x^*=x. A self-adjoint element is also Hermitian, though the reverse doesn't necessarily hold. A collection ''C'' of elements of a sta ...
elements a\in A_, every positive map is automatically continuous with respect to the C*-norms and its
operator norm In mathematics, the operator norm measures the "size" of certain linear operators by assigning each a real number called its . Formally, it is a norm defined on the space of bounded linear operators between two given normed vector spaces. Intr ...
equals \, \phi(1_A)\, _B. A similar statement with approximate units holds for non-unital algebras. * The set of positive functionals \to\mathbb is the dual cone of the cone of positive elements of A.


Examples

* Every *-
homomorphism In algebra, a homomorphism is a structure-preserving map between two algebraic structures of the same type (such as two groups, two rings, or two vector spaces). The word ''homomorphism'' comes from the Ancient Greek language: () meaning "sa ...
is completely positive. * For every linear operator V:H_1\to H_2 between Hilbert spaces, the map L(H_1)\to L(H_2), \ A \mapsto V A V^\ast is completely positive. Stinespring's theorem says that all completely positive maps are compositions of *-homomorphisms and these special maps. * Every positive functional \phi:A \to \mathbb (in particular every
state State may refer to: Arts, entertainment, and media Literature * ''State Magazine'', a monthly magazine published by the U.S. Department of State * ''The State'' (newspaper), a daily newspaper in Columbia, South Carolina, United States * '' Our ...
) is automatically completely positive. * Every positive map C(X)\to C(Y) is completely positive. * The transposition of matrices is a standard example of a positive map that fails to be 2-positive. Let denote this map on \mathbb^. The following is a positive matrix in \mathbb^ \otimes \mathbb^: \begin \begin1&0\\0&0\end& \begin0&1\\0&0\end\\ \begin0&0\\1&0\end& \begin0&0\\0&1\end \end = \begin 1 & 0 & 0 & 1 \\ 0 & 0 & 0 & 0 \\ 0 & 0 & 0 & 0 \\ 1 & 0 & 0 & 1 \\ \end. The image of this matrix under I_2 \otimes T is \begin \begin1&0\\0&0\end^T& \begin0&1\\0&0\end^T\\ \begin0&0\\1&0\end^T& \begin0&0\\0&1\end^T \end = \begin 1 & 0 & 0 & 0 \\ 0 & 0 & 1 & 0 \\ 0 & 1 & 0 & 0 \\ 0 & 0 & 0 & 1 \\ \end , which is clearly not positive, having determinant −1. Moreover, the
eigenvalues In linear algebra, an eigenvector () or characteristic vector of a linear transformation is a nonzero vector that changes at most by a scalar factor when that linear transformation is applied to it. The corresponding eigenvalue, often denoted b ...
of this matrix are 1,1,1 and −1. (This matrix happens to be the
Choi matrix Choi may refer to: * Choi (Korean surname), a Korean surname * Choi, Macau Cantonese transliteration of the Chinese surname Cui (崔) and Xu (徐) * Choi, Cantonese romanisation of Cai (surname) (蔡), a Chinese surname * CHOI-FM, a radio statio ...
of ''T'', in fact.) {{pb Incidentally, a map Φ is said to be co-positive if the composition Φ \circ ''T'' is positive. The transposition map itself is a co-positive map.


See also

* Choi's theorem on completely positive maps C*-algebras