
arXiv: 0906.4760
Barrett, Hardy, and Kent have shown in 2005 that protocols for quantum key agreement exist the security of which can be proven under the assumption that quantum or relativity theory is correct. More precisely, this is based on the non-local behavior of certain quantum systems, combined with the non-signaling postulate from relativity. An advantage is that the resulting security is independent of what (quantum) systems the legitimate parties' devices operate on: they do not have to be trusted. Unfortunately, the protocol proposed by Barrett et al. cannot tolerate any errors caused by noise in the quantum channel. Furthermore, even in the error-free case it is inefficient: its communication complexity is Theta(1/epsilon) when forcing the attacker's information below epsilon, even if only a single key bit is generated. Potentially, the problem can be solved by privacy amplification of relativistic - or non-signaling - secrecy. We show, however, that such privacy amplification is impossible with respect to the most important form of non-local behavior, and application of arbitrary hash functions.
24 pages, 2 figures
Quantum cryptography (quantum-theoretic aspects), Quantum Physics, cryptography, Cryptography, Bell inequalities, FOS: Physical sciences, quantum key agreement, Quantum Physics (quant-ph), device-independent security, non-locality
Quantum cryptography (quantum-theoretic aspects), Quantum Physics, cryptography, Cryptography, Bell inequalities, FOS: Physical sciences, quantum key agreement, Quantum Physics (quant-ph), device-independent security, non-locality
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