Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Posting-Version: version B 2.10.2 9/5/84; site umich.UUCP Path: utzoo!watmath!clyde!burl!ulysses!bellcore!petrus!sabre!zeta!epsilon!mb2c!umich!torek From: torek@umich.UUCP (Paul V. Torek ) Newsgroups: net.physics Subject: The Revenge of Probabilism in QM Message-ID: <425@umich.UUCP> Date: Tue, 28-Jan-86 03:00:37 EST Article-I.D.: umich.425 Posted: Tue Jan 28 03:00:37 1986 Date-Received: Thu, 30-Jan-86 04:46:22 EST Distribution: net Organization: University of Michigan, EECS Dept., Ann Arbor, MI Lines: 19 Summary: Or, why we don't have to resort to Many Worlds Quoted without permission from Nicholas Maxwell, "Are Probabilism and Special Relativity Incompatible?" *Philosophy of Science* 52 (1985) 23-43, esp. pp. 36-40 [Answer to title question: yes, and Maxwell favors probabilism]: "... This [Maxwell's] approach requires that precise, microrealistic, quantum conditions be specified for propensities to be `actualised' -- for probabilistic events to occur in quantum systems even in the absence of measurement. My proposed solution to this key problem is that probabilistic `actualizations' occur whenever, as a result of potential particle creation or annihilation, a composite quantum system evolves into a superposition of two states with rest masses that differ by [delta]m. [Sorry folks, I don't have a delta on my keyboard--pt] Reinterpreting the time/energy uncertainty relations, I suggest that such a superposition persists only for a time [delta]t = h / [delta]m c**2, and then jumps to one or the other rest mass state. All quantum measurements can, I argue, be interpreted as special cases of this kind of probabilistic occurrence (see Maxwell 1976a, 1982). :