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For detection of spin S particles a Stern-Gerlach device can be used, for which a setting corresponds to the choice of the direction of the magnetic field and detection of each of the possible 2S + 1 outputs.
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For example, all bound entangled states with positive partial transposes with respect to all possible groupings of the involved observers into two parties do not violate any Bell inequality involving two dychotomic observables for each of the observers. It has been even conjectured that such states admit a local hidden variable model; A. Peres, Found. Phys. 29, 589 (1999); R.F. Werner and M.M. Wolf, e-print quant-ph/9910063; see also R.F. Werner and M.M. Wolf, e-print quant-ph/0102024; M. Zukowski and C. Brukner, e-print quant-ph/0102039.
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For example, all bound entangled states with positive partial transposes with respect to all possible groupings of the involved observers into two parties do not violate any Bell inequality involving two dychotomic observables for each of the observers. It has been even conjectured that such states admit a local hidden variable model; A. Peres, Found. Phys. 29, 589 (1999); R.F. Werner and M.M. Wolf, e-print quant-ph/9910063; see also R.F. Werner and M.M. Wolf, e-print quant-ph/0102024; M. Zukowski and C. Brukner, e-print quant-ph/0102039.
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Werner, R.F.1
Wolf, M.M.2
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29
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e-print quant-ph/0102024
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For example, all bound entangled states with positive partial transposes with respect to all possible groupings of the involved observers into two parties do not violate any Bell inequality involving two dychotomic observables for each of the observers. It has been even conjectured that such states admit a local hidden variable model; A. Peres, Found. Phys. 29, 589 (1999); R.F. Werner and M.M. Wolf, e-print quant-ph/9910063; see also R.F. Werner and M.M. Wolf, e-print quant-ph/0102024; M. Zukowski and C. Brukner, e-print quant-ph/0102039.
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Werner, R.F.1
Wolf, M.M.2
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30
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e-print quant-ph/0102039
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For example, all bound entangled states with positive partial transposes with respect to all possible groupings of the involved observers into two parties do not violate any Bell inequality involving two dychotomic observables for each of the observers. It has been even conjectured that such states admit a local hidden variable model; A. Peres, Found. Phys. 29, 589 (1999); R.F. Werner and M.M. Wolf, e-print quant-ph/9910063; see also R.F. Werner and M.M. Wolf, e-print quant-ph/0102024; M. Zukowski and C. Brukner, e-print quant-ph/0102039.
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Zukowski, M.1
Brukner, C.2
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