2021
DOI: 10.22331/q-2021-10-27-569
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Quantum Advantage for Shared Randomness Generation

Abstract: Sharing correlated random variables is a resource for a number of information theoretic tasks such as privacy amplification, simultaneous message passing, secret sharing and many more. In this article, we show that to establish such a resource called shared randomness, quantum systems provide an advantage over their classical counterpart. Precisely, we show that appropriate albeit fixed measurements on a shared two-qubit state can generate correlations which cannot be obtained from any possible state on two cl… Show more

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Cited by 14 publications
(5 citation statements)
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“…A similar process will yield H(p)-bit of shared randomness from the state ρ = p |00 00| + (1 − p) |11 11|, with p ∈ [0, 1]. For more elaborative discussions on classical shared randomness from a resource theoretic perspective we refer to the work [32].…”
Section: Definition 3 (Classical Correlated Strategy)mentioning
confidence: 99%
See 1 more Smart Citation
“…A similar process will yield H(p)-bit of shared randomness from the state ρ = p |00 00| + (1 − p) |11 11|, with p ∈ [0, 1]. For more elaborative discussions on classical shared randomness from a resource theoretic perspective we refer to the work [32].…”
Section: Definition 3 (Classical Correlated Strategy)mentioning
confidence: 99%
“…However, it is important to note that to create classical shared randomness between two distant parties, classical communication is a necessary resource, and hence in this work we will consider it to be a costly resource. A number of works in other branches of research [27][28][29] as well as in quantum information theory [30][31][32] already exist where nontrivial utilities of classical shared randomness have been been pointed out.…”
Section: Introductionmentioning
confidence: 99%
“…Such a state generally allows correlation between two coins placed at the left and right compartments of the Box [41]. However, action of the mixing device M c ix on both compartments kills any such correlation and the box state becomes completely mixed, i.e.…”
Section: Appendix A: Physical Theories and Computationmentioning
confidence: 99%
“…It follows from the Gottesman-Knill theorem that it is possible to efficiently simulate any stabilizer circuit on a classical computer, hence rendering stabilizer states and operations useless for universal quantum computation [43,44]. For this reason, this model fits the mold of quantum resource theories where all the states and operations that cannot provide any quantum advantage are treated as free [19,24,[45][46][47][48][49].…”
Section: Introductionmentioning
confidence: 99%