6,240 research outputs found
Proposal for revealing quantum nonlocality via local contextuality
Two distant systems can exhibit quantum nonlocality even though the
correlations between them admit a local model. This nonlocality can be revealed
by testing extra correlations between successive measurements on one of the
systems which do not admit a noncontextual model whatever the reduced state of
this system is. This shows that quantum contextuality plays a fundamental role
in quantum nonlocality, and allows an experimental test of the Kochen-Specker
with locality theorem.Comment: REVTeX4-1, 4 pages, 1 figur
Quantum correlations are not contained in the initial state
Two proofs are presented which show that quantum mechanics is incompatible
with the following assumption: all possible correlations between subsystems of
an individual isolated composite quantum system are contained in the initial
quantum state of the whole system, although just a subset of them is revealed
by the actual experiment.Comment: REVTeX, 4 pages, 1 figur
Bosonic bunching does not reveal stronger quantum contextuality
In a recent paper, Kurzynski et al. present a gedanken experiment that, they
claim, violates the Klyachko-Can-Binicioglu-Shumovsky (KCBS) noncontextuality
(NC) inequality beyond its maximum quantum value, and a similar experiment
that, they claim, violates Specker's NC inequality, which is not violated by
quantum mechanics. We argue that these claims are baseless, since these
experiments do not satisfy the conditions required for any observation of
contextuality through the experimental violation of a NC inequality. Moreover,
the physical events in the experiments of Kurzynski et al. do not have the
relationships of exclusivity which the authors assume they have.Comment: REVTeX4, 3 page
Minimal proofs of state-independent contextuality
It has been recently shown that state-independent contextuality (SIC) is a
fundamental resource linked with a type of nonlocality which cannot be improved
by nonsignaling resources. Therefore, it is of fundamental importance to
identify the simplest sets of quantum observables needed to prove SIC. We show
that d+10 rank-1 projectors are sufficient to prove SIC for any physical system
in dimension d>2. This result outperforms both the best Kochen-Specker proofs
and the results presented by Yu and Oh in arXiv:1112.5513v1.Comment: REVTeX4, 2 page
Quantum key distribution in the Holevo limit
A theorem by Shannon and the Holevo theorem impose that the efficiency of any
protocol for quantum key distribution, , defined as the number of
secret (i.e., allowing eavesdropping detection) bits per transmitted bit plus
qubit, is . The problem addressed here is whether the limit
can be achieved. It is showed that it can be done by splitting
the secret bits between several qubits and forcing Eve to have only a
sequential access to the qubits, as proposed by Goldenberg and Vaidman. A
protocol with based on polarized photons and in which Bob's state
discrimination can be implemented with linear optical elements is presented.Comment: REVTeX, 4 pages, 2 figure
Comment on "Non-contextual hidden variables and physical measurements"
Kent's conclusion that ``non-contextual hidden variable theories cannot be
excluded by theoretical arguments of the Kochen-Specker type once the
imprecision in real world experiments is taken into account'' [Phys. Rev. Lett.
83, 3755 (1999)], is criticized. The Kochen-Specker theorem just points out
that it is impossible even conceive a hidden variable model in which the
outcomes of all measurements are pre-determined; it does not matter if these
measurements are performed or not, or even if these measurements can be
achieved only with finite precision.Comment: 2 page
Exclusivity principle and the quantum bound of the Bell inequality
We show that, for general probabilistic theories admitting sharp
measurements, the exclusivity principle together with two assumptions exactly
singles out the Tsirelson bound of the Clauser-Horne-Shimony-Holt Bell
inequality.Comment: REVTeX4, 4 pages, 1 figur
Specker's fundamental principle of quantum mechanics
I draw attention to the fact that three recently proposed physical
principles, namely "local orthogonality", "global exclusive disjunction", and
"compatible orthogonality" are not new principles, but different versions of a
principle that Ernst Specker noticed long ago. I include a video of Specker
stating this principle in 2009 in the following terms: "Do you know what,
according to me, is the fundamental theorem of quantum mechanics? (...) That
is, if you have several questions and you can answer any two of them, then you
can also answer all of them". I overview some results that suggest that
Specker's principle may be of fundamental importance for explaining quantum
contextuality. Specker passed away in December 10, 2011, at the age of 91.Comment: REVTeX4, 4 pages, 1 figure, 1 vide
Proposed experiment to exclude higher-than-quantum violations of the Bell inequality
We show that a recent observation by Yan leads to a method to experimentally
test whether a higher-than-quantum violation of the Clauser-Horne-Shimony-Holt
Bell inequality is possible (assuming that the sum of probabilities of pairwise
exclusive propositions cannot exceed 1). The test requires reaching the maximum
quantum violation of a noncontextuality inequality involving sequences of three
compatible measurements on a five-dimensional quantum system.Comment: REVTeX4, 4 pages, 1 figur
Simple explanation of the quantum violation of a fundamental inequality
We show that the maximum quantum violation of the
Klyachko-Can-Binicioglu-Shumovsky (KCBS) inequality is exactly the maximum
value satisfying the following principle: The sum of probabilities of pairwise
exclusive events cannot exceed 1. We call this principle "global exclusivity,"
since its power shows up when it is applied to global events resulting from
enlarged scenarios in which the events in the inequality are considered jointly
with other events. We identify scenarios in which this principle singles out
quantum contextuality, and show that a recent proof excluding nonlocal boxes
follows from the maximum violation imposed by this principle to the KCBS
inequality.Comment: REVTeX4, 6 pages, 3 figure
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