N. D. Mermin. Hidden variables and the two theorems of John Bell. Reviews of Modern Physics, 65(3):803--815, 1993. Home/Search Document Not in Database Summary Related Articles Check |
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Easy Proofs of Some Consequences of - Gleason's Theorem Mirko (Correct)
....of Am . Another more known proof of nonexistence of two valued states was done by Kochen and Specker [5] the attempts to optimize it lead to a series of Kochen Specker type theorems. In these, one nds a nite sublattice of L(R ) admitting no two valued state; nice overviews can be found in [6, 8, 9]. At this moment, the least construction of this type in L(R ) is due to Conway and Kochen; its arguments use 31 vectors. Another construction due to Peres uses 33 vectors, but these are highly symmetric: They all can be found at a picture of three cubes with a common centre (which appeared in ....
Mermin, N.D.: Hidden variables and the two theorems of John Bell. Rev. Mod. Phys. 65 (1993), 803-815.
Physical versus Computational Complementarity I - Calude, Calude, Svozil, Yu (1996) (1 citation) (Correct)
.... complementarity it might still be possible to pretend that initially the automaton actually is in a single automaton state, which we just do not know (such a state can be seen if the automaton is screwed open ) quantum mechanically this assumption leads to a Kochen Specker contradiction [39, 56, 47, 69]. 11 The terms elements of reality , properties , and observables will be used as synonyms. 12 Note that the automaton in Figure 2 is connected, i.e. every two states are linked by some computation. 7 Only the second type of complementarity deserves more attention. A Moore automaton has ....
Mermin, N. D. Hidden variables and the two theorems of John Bell. Reviews of Modern Physics 65 (1993), 803--815.
Proof of the Impossibility of Non-Contextual Hidden Variables in.. - Fivel (Correct)
.... to each observable one of its eigenvalues, and (2) for any function f(c; d; Delta Delta Delta ) of a commuting subset of observables, the value assigned must be f(v(c) v(d) Delta Delta Delta) A discussion of the physical importance of ruling out such theories is given in Mermin s review[3]. Recently there have been some enormous simplifications in the proofs given by Bell and Kochen Specker, the most elegant being that of Peres[4, 5, 6] In common with the original proofs, however, the improved ones are specific to particular Hilbert space dimensions, and reveal no general ....
1993, Mermin, N. D., "Hidden variables and the two theorems of John Bell," Rev. Mod. Phys. 65, No. 3, 803-815.
Consequences and Limits of Nonlocal Strategies - Richard Cleve Peter (Correct)
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N. D. Mermin. Hidden variables and the two theorems of John Bell. Reviews of Modern Physics, 65(3):803--815, 1993.
Embedding Quantum Universes into Classical Ones - Calude, Hertling, Svozil (1999) (Correct)
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MERMIN, N. D. Hidden variables and the two theorems of John Bell. Reviews of Modern Physics 65 (1993), 803--815.
Density Conditions for Quantum Propositions - Hans Havlicek Institut (1996) (1 citation) (Correct)
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N. D. Mermin. Hidden variables and the two theorems of John Bell. Reviews of Modern Physics, 65:803-815, 1993.
Unknown - (1998) (Correct)
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Mermin, N. D. (1993). Hidden variables and the two theorems of John Bell. Reviews of Modern Physics, 65, 803--815.
Piron's and Bell's Geometrical Lemmas - Mirko Navara Center (Correct)
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Mermin, N.D.: Hidden variables and the two theorems of John Bell. Rev. Mod. Phys. 65 (1993), 803-815.
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