4.6 Article

Geometry of the set of quantum correlations

期刊

PHYSICAL REVIEW A
卷 97, 期 2, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevA.97.022104

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资金

  1. Singapore Ministry of Education [MOE2012-T3-1-009]
  2. National Research Fund
  3. Ministry of Education, Singapore, under the Research Centres of Excellence programme
  4. John Templeton Foundation [60607]
  5. European Union's Horizon research and innovation programme under Marie Sklodowska-Curie Action ROSETTA [749316]
  6. European Research Council [337603]
  7. Danish Council for Independent Research (SapereAude)
  8. VILLUM FONDEN via the QMATH Centre of Excellence [10059]
  9. National Research, Development, and Innovation Office NKFIH [K111734, KH125096]
  10. Ministry of Education of Taiwan, R.O.C.
  11. Ministry of Science and Technology of Taiwan, R.O.C. [104-2112-M-006-021-MY3]
  12. Perimeter Institute for Theoretical Physics
  13. Government of Canada through the Department of Innovation, Science, and Economic Development Canada
  14. Province of Ontario through the Ministry of Research, Innovation, and Science
  15. Marie Curie Actions (MSCA) [749316] Funding Source: Marie Curie Actions (MSCA)

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It is well known that correlations predicted by quantum mechanics cannot be explained by any classical (local-realistic) theory. The relative strength of quantum and classical correlations is usually studied in the context of Bell inequalities, but this tells us little about the geometry of the quantum set of correlations. In other words, we do not have a good intuition about what the quantum set actually looks like. In this paper we study the geometry of the quantum set using standard tools from convex geometry. We find explicit examples of rather counterintuitive features in the simplest nontrivial Bell scenario (two parties, two inputs, and two outputs) and illustrate them using two-dimensional slice plots. We also show that even more complex features appear in Bell scenarios with more inputs or more parties. Finally, we discuss the limitations that the geometry of the quantum set imposes on the task of self-testing.

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