2020
DOI: 10.1063/1.5115010
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Geometry of the set of synchronous quantum correlations

Abstract: We provide a complete geometric description of the set of synchronous quantum correlations for the three-experiment two-outcome scenario. We show that these correlations form a closed set. Moreover, every correlation in this set can be realized using projection valued measures on a Hilbert space of dimension no more than 16.

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Cited by 4 publications
(3 citation statements)
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“…However, no similar dimension reduction argument is known when the number of measurements or number of measurement outcomes is greater than 2. A result of Russell describes another linear slice, the synchronous correlations, in C q (3, 3, 2, 2), but again this description does not extend to other numbers of measurements and outcomes [Rus20].…”
Section: Introductionmentioning
confidence: 96%
“…However, no similar dimension reduction argument is known when the number of measurements or number of measurement outcomes is greater than 2. A result of Russell describes another linear slice, the synchronous correlations, in C q (3, 3, 2, 2), but again this description does not extend to other numbers of measurements and outcomes [Rus20].…”
Section: Introductionmentioning
confidence: 96%
“…In another paper, Dykema-Paulsen-Parakash [6] provided a negative answer to the strong Tsirelson problem (whether or not C q (n, m) = C qc (n, m)) in the setting of synchronous correlation sets with n = 5 and m = 2. In [16] the author determined the geometry of the synchronous quantum correlation set in the setting of n = 3 and m = 2 but left the solution to Tsirelson's problems in this setting open. In this paper we complete the study of the n = 3, m = 2 case by showing that the strong Tsirelson problem has an affirmative answer in this setting.…”
Section: Introductionmentioning
confidence: 99%
“…Proof. By [12], the set C s q in our (three input, two output) case is closed. Thus, the supremum (11) used to compute ω q (G, π) is achieved.…”
mentioning
confidence: 96%

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