Quantum Mechanics Versus Local Realism 1988
DOI: 10.1007/978-1-4684-8774-9_11
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Quantum Action-at-a-Distance: The Mystery of Einstein-Podolsky-Rosen Correlations

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“…6 we can deduce [9,12] different joint and conditional probabilities for detecting particles + and -in separated regions of space-time. First, we have at time t ′′ out > t ′′ the joint probability P (D + , D − ) = 1 12 (7) meaning that the probability of a joint outcome in wavepackets D + and D − is not vanishing (this formula doesn't require the simultaneity of D + and D − measurements). We have also the conditional probabilities…”
Section: Reviewing the No-go Theoremsmentioning
confidence: 99%
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“…6 we can deduce [9,12] different joint and conditional probabilities for detecting particles + and -in separated regions of space-time. First, we have at time t ′′ out > t ′′ the joint probability P (D + , D − ) = 1 12 (7) meaning that the probability of a joint outcome in wavepackets D + and D − is not vanishing (this formula doesn't require the simultaneity of D + and D − measurements). We have also the conditional probabilities…”
Section: Reviewing the No-go Theoremsmentioning
confidence: 99%
“…However, as stated by Hardy [12], Bohm [3,6,27], and Bell [1,3] there is no experiment that can be performed to determine what this preferred frame is (even if the absolute reference frame associated with the 2.7 K microwave cosmological background is often recalled [3,8] as a good candidate in this context). Vigier and coworkers [7] also proposed to use the center of mass of the full particle ensemble to define a preferred frame in BM. Similarly, Durr, Struyve et all.…”
Section: Reviewing the No-go Theoremsmentioning
confidence: 99%
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