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Erschienen in: Quantum Information Processing 1/2016

01.01.2016

A general framework for complete positivity

verfasst von: Jason M. Dominy, Alireza Shabani, Daniel A. Lidar

Erschienen in: Quantum Information Processing | Ausgabe 1/2016

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Abstract

Complete positivity of quantum dynamics is often viewed as a litmus test for physicality; yet, it is well known that correlated initial states need not give rise to completely positive evolutions. This observation spurred numerous investigations over the past two decades attempting to identify necessary and sufficient conditions for complete positivity. Here, we describe a complete and consistent mathematical framework for the discussion and analysis of complete positivity for correlated initial states of open quantum systems. This formalism is built upon a few simple axioms and is sufficiently general to contain all prior methodologies going back to Pechakas (Phys Rev Lett 73:1060–1062, 1994). The key observation is that initial system-bath states with the same reduced state on the system must evolve under all admissible unitary operators to system-bath states with the same reduced state on the system, in order to ensure that the induced dynamical maps on the system are well defined. Once this consistency condition is imposed, related concepts such as the assignment map and the dynamical maps are uniquely defined. In general, the dynamical maps may not be applied to arbitrary system states, but only to those in an appropriately defined physical domain. We show that the constrained nature of the problem gives rise to not one but three inequivalent types of complete positivity. Using this framework, we elucidate the limitations of recent attempts to provide conditions for complete positivity using quantum discord and the quantum data processing inequality. In particular, we correct the claim made by two of us (Shabani and Lidar in Phys Rev Lett 102:100402–100404, 2009) that vanishing discord is necessary for complete positivity, and explain that it is valid only for a particular class of initial states. The problem remains open, and may require fresh perspectives and new mathematical tools. The formalism presented herein may be one step in that direction.

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Fußnoten
1
Not every state in \(D_{\textsc {s}}\) needs to be covered by a state in \({\mathcal {S}}\). Those that are not covered are inadmissible initial system states, lying outside the domain of \(\tau _{U}^{{\mathcal {S}}}\). See also the comments at the end of Sect. 3.4.
 
2
It should be noted that this notion of \(\mathcal {G}\)-consistency is more general than the notion of assignment map consistency described by Alicki [14] and considered in several later works [12, 16, 17]. The typical interpretation of assignment map consistency is equivalent to \(\mathrm {U}(\mathcal {H}_{\textsc {s}}\otimes \mathcal {H}_{\textsc {b}})\)-consistency with the additional requirement that \(\mathrm{Tr}_{\textsc {b}}{\mathcal {S}}= \mathcal {D}_{\textsc {s}}\), i.e., every state of the subsystem must be covered by exactly one system-bath state in \({\mathcal {S}}\).
 
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Metadaten
Titel
A general framework for complete positivity
verfasst von
Jason M. Dominy
Alireza Shabani
Daniel A. Lidar
Publikationsdatum
01.01.2016
Verlag
Springer US
Erschienen in
Quantum Information Processing / Ausgabe 1/2016
Print ISSN: 1570-0755
Elektronische ISSN: 1573-1332
DOI
https://doi.org/10.1007/s11128-015-1148-0

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