2017
DOI: 10.1364/oe.25.031462
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Enhanced violations of Leggett-Garg inequalities in an experimental three-level system

Abstract: Leggett-Garg inequalities are tests of macroscopic realism that can be violated by quantum mechanics. In this letter, we realise photonic Leggett-Garg tests on a three-level system and implement measurements that admit three distinct measurement outcomes, rather than the usual two. In this way we obtain violations of three- and four-time Leggett-Garg inequalities that are significantly in excess of those obtainable in standard Leggett-Garg tests. We also report violations the quantum-witness equality up to the… Show more

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Cited by 31 publications
(20 citation statements)
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References 54 publications
(81 reference statements)
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“…(1.2) is −1/2. This is the Lüders bound [40][41][42][43][44] and is the maximal violation possible for projective measurements of a dichotomic variable Q (Lüders measurements) and coincides numerically with the Tsirelson bound [11] in Bell experiments. However, for systems with three or more levels, there are different macrorealistically equivalent methods of measuring the correlators which permit violations of the Lüders bound.…”
Section: B Two-time Nsit Conditions In the Triple Slit Experimentssupporting
confidence: 67%
“…(1.2) is −1/2. This is the Lüders bound [40][41][42][43][44] and is the maximal violation possible for projective measurements of a dichotomic variable Q (Lüders measurements) and coincides numerically with the Tsirelson bound [11] in Bell experiments. However, for systems with three or more levels, there are different macrorealistically equivalent methods of measuring the correlators which permit violations of the Lüders bound.…”
Section: B Two-time Nsit Conditions In the Triple Slit Experimentssupporting
confidence: 67%
“…The two and three-time LG inequalities given above have a lower bound of −1/2 in quantum theory. This is the so-called Lüders bound [35,[37][38][39][40] and is readily derived as follows. Suppose for example we consider the LG2 for times t 2 , t 3 , we have…”
Section: Discussionmentioning
confidence: 99%
“…However, what an experimentalist will measure in a lab is independent of this choice. For measurements of a dichotomic operators, the LGIs, in quantum theory, have a lower bound of − 1 2 , the socalled Lüders bound [35,[37][38][39][40]. Similarly, the 3rd-order…”
Section: 2)mentioning
confidence: 99%
“…However, MPD utilizes photon-counting intensity detection with a significantly low experimental complexity. It is also simpler compared with the LGI violating architectures utilizing single-photon sources and Mach-Zehnder interferometers [11,20,21]. Besides that, light sources not fully coherent in terms of spatial and temporal dimensions are theoretically modeled while the violation of LGI and QPI are numerically analyzed for specific MPD setup geometry satisfying coherence of light under Gaussian source beam assumptions.…”
Section: Introductionmentioning
confidence: 99%