2013
DOI: 10.1103/physrevx.3.011012
|View full text |Cite
|
Sign up to set email alerts
|

Experimental Implementation of a Kochen-Specker Set of Quantum Tests

Abstract: The conflict between classical and quantum physics can be identified through a series of yes-no tests on quantum systems, without it being necessary that these systems be in special quantum states. Kochen-Specker (KS) sets of yes-no tests have this property and provide a quantum-versusclassical advantage that is free of the initialization problem that affects some quantum computers. Here, we report the first experimental implementation of a complete KS set that consists of 18 yes-no tests on four-dimensional q… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
115
1

Year Published

2014
2014
2024
2024

Publication Types

Select...
8
1

Relationship

2
7

Authors

Journals

citations
Cited by 86 publications
(116 citation statements)
references
References 59 publications
0
115
1
Order By: Relevance
“…They were implemented for 4-dim systems with photons [13][14][15][16][17][18], neutrons [19][20][21] trapped ions [22], and molecular nuclear spins in the solid states [23], for 6-dim systems via six path possibilities for the photon transmission through a diffractive aperture [24,25], and for 8-dim systems by means of the linear transverse momentum of single photons transmitted by diffractive apertures addressed in spatial light modulators [26].…”
Section: Introductionmentioning
confidence: 99%
“…They were implemented for 4-dim systems with photons [13][14][15][16][17][18], neutrons [19][20][21] trapped ions [22], and molecular nuclear spins in the solid states [23], for 6-dim systems via six path possibilities for the photon transmission through a diffractive aperture [24,25], and for 8-dim systems by means of the linear transverse momentum of single photons transmitted by diffractive apertures addressed in spatial light modulators [26].…”
Section: Introductionmentioning
confidence: 99%
“…(6) and (5), respectively, for all odd numbers of spins from N = 3 to 17. Note that the pair of forbidden projectors Π (5) 0 and Π (13) 0 have the remarkable geometric property that first order errors vanish when Z w = i, explaining the small statistical standard deviation σ observed in the experimental data. The cho- sen witnesses for other N in Fig.…”
Section: Resultsmentioning
confidence: 97%
“…Unlike the implicit global contradictions inherent to existing BKS experiments [11][12][13], our method confines the apparent contradiction to a particular context, where its physical consequences may be explicitly revealed through weak measurements. Notably, unlike existing approaches to demonstrating BKS-contextuality [27], our witness does not require entangled preparations or measurements, or indeed any interaction between the different spins at all.…”
Section: Discussionmentioning
confidence: 99%
“…This degree of freedom is related to the spatial modes of electromagnetic radiation and provides an infinite dimensional Hilbert space that allows us to implement qudits of, in principle, arbitrary d using single photons. OAM is attracting great attention in the last decade for its applications in a va- riety of disciplines such as biophysics [21][22][23], metrology [24], astronomy [25], quantum communication [26,27], and fundamental quantum physics [28,29]. Here we take advantage of the wide alphabet provided by OAM to encode six-dimensional single photon quantum states by choosing as a logical basis the following OAM eigenstates subset:…”
mentioning
confidence: 99%