Tez
Graduate Poster
- Joined
- Nov 29, 2001
- Messages
- 1,104
Well the short answer is there is nothing in principle preventing a hidden variable description of QM - Bell provided some simple examples for spin systems, Bohm provided another. Moreover, if all you care about is local predictions (such as your radioactive nucleus decay) then all you have to worry about is the local "hidden variable" physics. This covers almost all the use of QM in practice. (i.e no need to look at the "rest of the universe" etc)
What Bell showed, however, is that if you compare measurements on separated systems, and look for correlations in the data then (for specially prepared systems) you must invoke some sort of nonlocal (i.e. "action at a distance type) effect in order to explain the observed correlations. This is not an objection to all hidden variables, just to the local kind. These nonlocal effects do not allow superluminal signalling (otherwise they'd be incompatible with my assertion above about local predictions etc)
What Bell showed, however, is that if you compare measurements on separated systems, and look for correlations in the data then (for specially prepared systems) you must invoke some sort of nonlocal (i.e. "action at a distance type) effect in order to explain the observed correlations. This is not an objection to all hidden variables, just to the local kind. These nonlocal effects do not allow superluminal signalling (otherwise they'd be incompatible with my assertion above about local predictions etc)