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- Path: sparky!uunet!mtnmath!paul
- From: paul@mtnmath.UUCP (Paul Budnik)
- Newsgroups: sci.physics
- Subject: Re: The instantaneous transfer of information in QM calculations
- Message-ID: <485@mtnmath.UUCP>
- Date: 11 Jan 93 16:24:04 GMT
- References: <481@mtnmath.UUCP> <1993Jan10.164016.16419@cs.wayne.edu> <1993Jan11.031132.1521@cs.wayne.edu>
- Organization: Mountain Math Software, P. O. Box 2124, Saratoga. CA 95070
- Lines: 58
-
- In article <1993Jan11.031132.1521@cs.wayne.edu>, atems@igor.physics.wayne.edu (Dale Atems) writes:
- [...]
- > Consider an experimental setup designed to test the version of Bell's
- > inequality that applies to spin-half particles in the singlet state. [...]
- >
- > Bell's inequality for this situation takes the form of a relationship
- > between correlation functions < (S(1,a) S(2,b) > where S(i,a) is the
- > component of particle i's spin along a, and similarly for b. To determine
- > such a correlation function experimentally, *in principle* all you need
- > to do is repeat the experiment a sufficient number of times, measuring
- > the spins of both particles and forming the product S(1,a) S(2,b) for
- > each pair, sum the products and divide by the number of pairs detected.
- > I don't see where you need to assume anything about what happens to the
- > wave function of one particle after the other is detected. One simply
- > measures spin components and computes a statistical average.
-
- Of course you do not need to make any such assumption to analyze the
- statistics of the experimental results. You do need to use the
- collapse postulate in some from to prove what quantum mechanics *predicts*
- in such an experiment. What is crucial about Bell's inequality is that
- the observation at one site was *affected* by the *measurement* made
- at the other site. If it were simply a matter of the two particles having
- parameters that were correlated at the time they split apart you *cannot*
- get a violation of Bell's inequality. To get the QM prediction you have
- to use more then the assumption that the two particles are in a singlet
- state. If you just used this assumption then the probability density of
- a detection at one site would be independent of the observations at the
- other site because those observations cannot influence the distant probability
- density. You have to assume that when you make an observation at one site
- this *changes* the probability density you use in your *calculations* at
- the other site to be in accord with information you obtained from that
- distant measurement. This may not sound like quantum collapse. You may
- just think about it as using all the information you have, but it terms
- of the mathematical theory you are forced to use the collapse postulate to
- get the correct probability density.
-
- > Of course, a finding that the observed correlations violate Bell's
- > inequality says nothing about locality if they could have been produced
- > by an exchange of information. As I understand it, the basic
- > premise behind Bell's proof is that all components of each particle's
- > spin are fixed when the singlet state is prepared and do not change
- > afterward. [...]
-
- This is dead wrong. If it were true you would not get a violation of
- Bell's inequality. There is a real instantaneous information transfer
- whenever there is a violation of Bell's inequality. In quantum
- mechanics it is not a form of information transfer that can be used for
- communication, but a distant experimental setting instantaneously influences
- the observational results at a local site. This comes from the central
- assumption of quantum mechanics that a state *does not exist* until it
- is observed. All that is *determined* from the assumption that the two
- photons are in a singlet state is that observations of them will have a
- certain correlation. The actual orientation of the spins *is not determined*
- until an observation is made. If you assume it is predetermined you
- have a hidden variables theory and will get results in contradiction with
- the predictions of QM.
-
- Paul Budnik
-