| | Von Neumann's Fifth Postulate (Site not responding. Last check: 2007-11-07) |
 | | In quantum theory the condition of a physical system is represented by a state vector, which encodes the probabilities of each possible result of whatever measurements we may perform on the system. |
 | | Thus, Bohm's 1952 theory escaped the no hidden variable theorems essentially by allowing the measurements to have an instantaneous effect on the hidden variables, which, of course, made the theory essentially non-local as well as non-relativistic (although Bohm and others later worked to relativize his theory). |
 | | Of course, it can be argued that contextual theories are somewhat contrived and not entirely compatible with the spirit of hidden variable explanations, but, if nothing else, they serve to illustrate how difficult it is to categorically rule out "all possible" hidden variable theories based simply on the structure of the quantum mechanical state space. |
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