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11 - Duality: maps versus states

Published online by Cambridge University Press:  27 August 2009

Ingemar Bengtsson
Affiliation:
Stockholms Universitet
Karol Zyczkowski
Affiliation:
Jagiellonian University, Krakow
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Summary

Good mathematicians see analogies. Great mathematicians see analogies between analogies.

Stefan Banach

We have already discussed the static structure of our ‘Quantum Town’ – the set of density matrices – on the one hand, and the set of all physically realizable processes which may occur in it on the other hand. Now we are going to reveal a quite remarkable property: the set of all possible ways to travel in the ‘Quantum Town’ is equivalent to a ‘Quantum Country’ – an appropriately magnified copy of the initial ‘Quantum Town’! More precisely, the set of all transformations which map the set of density matrices of size N into itself (dynamics) is identical to a subset of the set of density matrices of size N2 (kinematics). From a mathematical point of view this relation is based on the Jamiołkowski isomorphism, analysed later in this chapter. Before discussing this intriguing duality, let us leave the friendly set of quantum operations and pay a short visit to a neighbouring land of maps, as yet unexplored, which are positive but not completely positive.

Positive and decomposable maps

Quantum transformations which describe physical processes are represented by completely positive (CP) maps. Why should we care about maps which are not CP? On the one hand it is instructive to realize that seemingly innocent transformations are not CP, and thus do not correspond to any physical process. On the other hand, as discussed in Chapter 15, positive but not completely positive maps provide a crucial tool in the investigation of quantum entanglement.

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Geometry of Quantum States
An Introduction to Quantum Entanglement
, pp. 281 - 296
Publisher: Cambridge University Press
Print publication year: 2006

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