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数学学报

Strongly Separable Operators on Finite Dimensional Tensor Product Spaces

Zhang Ye, Cao Huaixin, Zhihua Guo

Published Jan 1, 2011• 0 citations
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Separable operators and PPT operators on a finite dimensional tensor product space are introduced.Then,general forms of separable self-adjoint operators,separable projective operators and separable positive operators are obtained.The relationship between separable operators and PPT operators are proved,and some examples which are PPT operators but not separable operators are given.Lastly,separable maps and PPT maps are introduced and discussed,and it is proved that every separable map maps a PPT operator as a PPT operator.
Tensor product operators on finite dimensional Hilbert spaces are studied. The focus is on bilinear tensor product operators. A tensor product operator on a pair of Hilbert spaces is a maximally general bilinear operator into a target Hilbert space. By 'maximally general' is meant every bilinear operator from the same pair of spaces to any Hilbert space factors into the composition of the tensor product operator with a uniquely determined linear mapping on the target space. There are multiple distinct tensor product operators of the same type; there is no "the" tensor product. Distinctly different tensor product operators can be associated with different parts of a multipartite system without difficulty. Separability of states, and locality of operators and observables is tensor product operator dependent. The same state in the target state space can be inseparable with respect to one tensor product operator but separable with respect to another, and no tensor product operator is distinguished relative to the others; the unitary operator used to construct a Bell state from a pair of |0>'s being highly tensor product operator-dependent is a prime example. The relationship between two tensor product operators of the same type is given by composition with a unitary operator. There is an equivalence between change of tensor product operator and change of basis in the target space. Among the gains from change of tensor product operator is the localization of some nonlocal operators as well as separability of inseparable states. Examples are given.