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Volumn 17, Issue 14, 2009, Pages 11440-11449

Efficient entanglement distribution over 200 kilometers

Author keywords

(060.5565) Quantum communications; (270.5565) Quantum communications; (270.5568) Quantum cryptography; (270.5585) Quantum Information and processing

Indexed keywords

PARTICLE BEAMS; QUANTUM CRYPTOGRAPHY; QUANTUM OPTICS;

EID: 67650541713     PISSN: None     EISSN: 10944087     Source Type: Journal    
DOI: 10.1364/OE.17.011440     Document Type: Article
Times cited : (108)

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    • The observed correlation in the experiment, C is connected to the visibility V thus: C=V cos2 (f) where f is a function of signal and idler phases, f (θs, θi, We use the Clauser-Horne-Shimony-Holt Bell inequality [34] with associated Bell parameter S=|C (θs, θi, C (θs, θi, C (θ's, θ'i, C θ's, θi, ≤ 2. Quantum-mechanically, this inequality can be violated with maximum violation of S=2√2. The violation of the Bell CHSH inequality in terms of visibility is hence V > 1 /√2
    • i)| ≤ 2. Quantum-mechanically, this inequality can be violated with maximum violation of S=2√2. The violation of the Bell CHSH inequality in terms of visibility is hence V > 1 /√2.
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    • The factor of two variation in error bar values between the two basis measurements arises from statistical variations from one experimental run to another
    • The factor of two variation in error bar values between the two basis measurements arises from statistical variations from one experimental run to another.


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