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14344276064
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note
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We can develop similar GHZ-like arguments starting from one-particle maximal operators with different eigenvalues other than those chosen in this paper, or even starting from nonmaximal operators. However, the choice in this paper (maximal operators with eigenvalues from -s to s) leads to a natural generalization of the original GHZ proof with spin-1/2 systems. It was recently proved that, for three spin-s particles, any one-particle operator can always be reduced to a direct sum of two two-level anticommuting one-particle operators (J. Savinien, J. Taron, and R. Tarrach, e-print quant-ph/0007069).
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16
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0000153017
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N. D. Mermin, Phys. Rev. Lett. 65, 3373 (1990); Rev. Mod. Phys. 65, 803 (1993).
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Mermin, N.D.1
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34250618244
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N. D. Mermin, Phys. Rev. Lett. 65, 3373 (1990); Rev. Mod. Phys. 65, 803 (1993).
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18
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14344279197
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note
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A similar set of requirements for a GHZ-like contradiction in the case of n spin-1/2 particles is proposed in Ref. [7].
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