Results 71 to 80 of about 470,444 (191)
Quantum Theory is a Quasi-stochastic Process Theory [PDF]
There is a long history of representing a quantum state using a quasi-probability distribution: a distribution allowing negative values. In this paper we extend such representations to deal with quantum channels. The result is a convex, strongly monoidal,
John van de Wetering
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Local Operations and Completely Positive Maps in Algebraic Quantum Field Theory [PDF]
Einstein introduced the locality principle which states that all physical effect in some finite space-time region does not influence its space-like separated finite region.
Y. Kitajima
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An Asymptotic Property of Factorizable Completely Positive Maps and the Connes Embedding Problem [PDF]
We establish a reformulation of the Connes embedding problem in terms of an asymptotic property of factorizable completely positive maps. We also prove that the Holevo–Werner channels $${W_n^-}$$Wn- are factorizable, for all odd integers $${n\neq 3}$$n≠3.
U. Haagerup, Magdalena Musat
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Covariant Completely Positive Maps and Liftings
zbMATH Open Web Interface contents unavailable due to conflicting licenses.
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Completely Positive Maps of the Cuntz Algebras
The author constructs a covariant functor from the category whose objects are separable Hilbert spaces and whose morphisms are contractions, into the category whose objects are unital \(C^*\)-algebras and whose morphisms are completely positive, identity preserving maps.
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Nuclearity and ${\mathrm {CPC}^*}$ -Systems
We write arbitrary separable nuclear $\mathrm {C}^*$ -algebras as limits of inductive systems of finite-dimensional $\mathrm {C}^*$ -algebras with completely positive connecting maps. The characteristic feature of such ${\mathrm {CPC}^*}$
Kristin Courtney, Wilhelm Winter
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Completely positive maps with memory
The prevailing description for dissipative quantum dynamics is given by the Lindblad form of a Markovian master equation, used under the assumption that memory effects are negligible. However, in certain physical situations, the master equation is essentially of a non-Markovian nature.
Daffer, Sonja +3 more
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Fixed Points Associated to Power of Normal Completely Positive Maps
Let be a normal completely positive map with Kraus operators . An operator X is said to be a fixed point of , if . Let be the fixed points set of . In this paper, fixed points of are considered for , where means j-power of .
Haiyan Zhang, Hongying Si
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Two-qubit causal structures and the geometry of positive qubit-maps
We study quantum causal inference in a setup proposed by Ried et al (2015 Nat. Phys. 11 414) in which a common cause scenario can be mixed with a cause–effect scenario, and for which it was found that quantum mechanics can bring an advantage in ...
Jonas M Kübler, Daniel Braun
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Special classes of positive and completely positive maps
Many authors have studied the problem of characterising the positive and completely positive maps on square complex matrices of size \(n\) under certain invariant conditions. These authors have characterized the above mentioned maps that leave invariant the diagonal or the \(k\)th elementary symmetric functions of the diagonal entries, for \(1 < k \leq
Li, Chi-Kwong, Woerdeman, Hugo J.
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