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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
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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
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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.
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