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Phys. Rev. A 73, 022104 (2006) [7 pages]

Experimenter’s freedom in Bell’s theorem and quantum cryptography

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Johannes Kofler1, Tomasz Paterek2, and Časlav Brukner1,3
1Institut für Experimentalphysik, Universität Wien, Boltzmanngasse 5, 1090 Wien, Austria
2Instytut Fizyki Teoretycznej i Astrofizyki, Uniwersytet Gdański, PL-80-952 Gdańsk, Poland
3Institut für Quantenoptik und Quanteninformation, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, 1090 Wien, Austria

Received 21 October 2005; published 6 February 2006

Bell’s theorem states that no local realistic explanation of quantum mechanical predictions is possible, in which the experimenter has a freedom to choose between different measurement settings. Within a local realistic picture the violation of Bell’s inequalities can only be understood if this freedom is denied. We determine the minimal degree to which the experimenter’s freedom has to be abandoned, if one wants to keep such a picture and be in agreement with the experiment. Furthermore, the freedom in choosing experimental arrangements may be considered as a resource, since its lacking can be used by an eavesdropper to harm the security of quantum communication. We analyze the security of quantum key distribution as a function of the (partial) knowledge the eavesdropper has about the future choices of measurement settings which are made by the authorized parties (e.g., on the basis of some quasi-random generator). We show that the equivalence between the violation of Bell’s inequality and the efficient extraction of a secure key—which exists for the case of complete freedom (no setting knowledge)—is lost unless one adapts the bound of the inequality according to this lack of freedom.

© 2006 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevA.73.022104
DOI:
10.1103/PhysRevA.73.022104
PACS:
03.65.Ud, 03.67.Dd