Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Posting-Version: version B 2.10.2 8/28/84; site lll-crg.ARPA Path: utzoo!linus!decvax!genrad!panda!talcott!harvard!seismo!lll-crg!brooks From: brooks@lll-crg.ARPA (Eugene D. Brooks III) Newsgroups: net.physics Subject: Re: Quantum Field Theory Message-ID: <760@lll-crg.ARPA> Date: Sun, 4-Aug-85 17:59:50 EDT Article-I.D.: lll-crg.760 Posted: Sun Aug 4 17:59:50 1985 Date-Received: Wed, 7-Aug-85 01:40:32 EDT References: <453@sri-arpa.ARPA> Organization: Lawrence Livermore Labs, CRG group Lines: 17 > In ordinary QM a solution of Schodingers equation is a function > of the form psi(c, t) where c is a variable ranging over configurations > of the system. Is the same true in QFT? In QFT each configuration c > is a distribution of the field in THREE-space? Why does time have such > a distinguished status? Why shouldn't solutions of (whatever) physical > equations be functions of the form psi(c') where c' ranges over > configurations of the field in FOUR-space? I'll have to think about > this further. Time does not have distinguished status, the t=0 surface just happens to be the standard space like surface that is used to establish the initial conditions of the field operators. You can pick any space like surface you like to set up the initial field operators and commutation relations. If you pick the t=0 surface the equations of motion only involves the H operator. If you pick some other surface then the equations of motion involves the full (H, Px, Py, Pz) operator and the t variable in the equations of motion are replaced by a variable s, the distance along a normal to the surface.