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Article #4537Feynman 27 "at any speed"
From: Jack Sarfatti
Date: Tue, 10 Nov 1992 05:23
Date: Tue, 10 Nov 1992 05:23
132 lines
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8661 bytes
Feynman 27 "at any speed" Gleick's book GENIUS p.229:"It was still possible, barely, to understand spin literally: to view the electron as a little moon. But if the electron was also an infinitesimal point, it could hardly rotate in the classical fasion. And if the electron was also a smear of probabilities and a wave reverberating in a constraining chamber. how could these objects be said to spin? What sort of spin could come only in unit amounts or half-unit amounts (as quantum mechanical spin did)? ... (Feynman) reduced the problem to a skeleton, a universe with just one dimensions (or two: one space and one time). This universe was merely a line, and in it a particle could take just one kind of path, back and forth [at the speed of light! JS], reversing direction like a crazed insect. Feynman's ... method .... the summing of all possible paths a particle could take .... he could derive ... a one dimensional Dirac equation .... he added something new - a diagram ... for keeping track of the zigs and zags. The horizontal dimensions represented his one spatial dimension, and the vertical dimension represented time.... Phase was crucial to the mathematics of summing the paths, because paths would either cancel or reinforce one another, depending on how their phases overlapped." p.231 [In this 1D Feynman picture a massive particle is a massless particle trapped in a string of length equal to the Compton wavelength h/mc. JS] ... p.246 "In mid-1947 friends of Feynman persuaded him - threats and cajoling were required - to write for publication ... He said he had developed an alternative formulation of quantum mechanics to add to the pair of formulations produced two decades before by Schrodinger and Heisenberg. He defined the notion of a probability amplitude for a space- time path. In the classical world one could merely add probabilities ... In the quantum world probabilities were expressed as complex numbers, numbers with a quantity and a phase, and these so-called amplitudes were squared to produce a probability." [Sarfatti comments: The square is the "absolute square" or product of the "retarded" complex number with its "advanced" complex conjugate number. The conjugate corresponds to running the path backward in time. Therefore, if two different paths are indistinguishable, the interference terms correspond to "loops in time" going forward in time on one path and returning backwards in time on the other path. Thus, the purely quantum distortions of the classical probabilities are due to loops in time that span a finite spacetime area. The reason for the i in quantum mechanics is the time loop. It's interesting the classical Wheeler-Feynman electrodynamics also has advanced backward in time effects. Similar loops of parallel transport (curvature) in the limit of shrinking area also determine the Newtonian limit of general relativity.] p.247 "Feynman described .... the canonical thought experiment of quantum mechanics, the so-cqalled two-slit experiment.... A beam of electrons (for example) passes through two slits in a screen, A detector on the far side records their arrival. If the detector is sensitive enough, it wil record individual events, like bullets striking; it might be designed to click as a Geiger counter clicks. But a peculiar spatial pattern emerges: the probabilities of electrons arriving at different places vary in the distinct manner of diffraction, precisely as though waves were passing the slit and interfering with one another. Particles or waves? Sealing the paradox, quantum mechanically, ... each electron 'sees' or 'knows about,' or somehow goes through both slits. Classically a particle would have to go through one slit or the other. .... If one tries to glimpse the particle as it passes through one slit or the other.... again one finds that the mere presence of the detector destroys the pattern." [Sarfatti comments: Bohm has still a fourth interpretation, the nonlocal quantum potential acts at a distance with a new kind of force on a real particle. In the Dirac ket notation, destruction of the interference pattern on the screen is caused by tracing over orthogonal kets of the measuring device that is 1-1 correlated (entangled) to the alternative paths of the electron from the two slits to a region on the screen. My quantum connection communicatio gedankenexperiment is a variation on "the canonical thought experiment of quantum mechanics". Instead of a single photon we have an entangled photon pair. Instead of the paths through the two slits we have the ordinary and extraordinary paths of the transmitter photon exiting the transmitter calcite crystal. A half-wave plate disentangles the photon pair in polarization space but not in physical space so that both paths of the transmitter photon have the same polarization. There is no contradiction with unitarity here as some critics falsely claim because the spatial distinction keeps the two parallel polarization states of the transmitter photon in different vector spaces until they collapse on the same photo-sensitive surface of a counter. The "screen" where "fringes" are observed corresponds to the two receiver counters behind the receiver calcite which is misaligned to the transmitter calcite by angle theta. The two reciever counters see complementary fringes. For example if one is bright, the other is dark. The fringe formula is essentially sin(2theta)cos(phi) where phi is the mean phase difference of the two alternative transmitter photon paths. There are no unitarity-violating fringes at the transmitter counter. The fringe shift quantum leaps to the two receiver counters where they obey local unitarity! It's a very pretty picture that is globally self consistent. The first nonlocal fringe shift was predicted by Bohm and Aharonov. *The amazing prediction is that one can cause a fringe shift at the receiver by making a "delayed choice" decision after the fringe shift has already happened. In this way useful "precognitive information" can be transmitted backward in time. It is posible to know the future and to act on that knowledge within certain limits. Your actions cannot prevent the future events that caused your knowledge. No wonder the orthodox scream "Crackpot!" - Sarfatti] "Probability amplitudes were normally associated with the liklihood of a particle's arrving at a certain place at a certain time. Feynman said he would associate the probability amplitude 'with an entire motion of a particle' - with a path. He stated the central principle of his quantum mechanics: The probability of an event which can happen in several different [indistinguishable or un-entangled - JS] ways is the absolute square of a sum of complex contributions, one from each alternative way. These complex numbers, these amplitudes, were written in terms of the classical action ..[ i.e., quantum amplitude for a single path = e^i2pi classical action for that path/Planck's constant h is the fundamental Feynman formula as important as Einstein's formula E = mc^2 - JS] p.249 His readers ... found no fancy mathematics, just this shift of vision, a bit of physical intuition laid atop a foundation of clean, classical mechanics. Few immediately recognized the power of Feynman's vision. One who did was the Polish mathematician Mark Kac, who heard Feynman describe his path integrals at Cornell and immediately recognized a kinship with ... the work of Norbert Weiner on Brownian motion, the herky-jerky random motion in the diffusion process [I took a math physics course with Kac at Cornell. - JS] ... Feynman's summing of paths - path integrals seemed bizzarre. They conjured a universe where no potential goes uncounted; where nothing is latent, everything alive; where every possibility makes itself felt in the outcome. He had expressed his conception to Dyson: 'The electron does anything it likes. It just goes in any direction at any speed, forward or backward in time, however it likes, and then you add up the amplitudes and it gives you the wave function.' Dyson gleefully retorted that he was crazy." p.250 to be continued - don't miss the next episode at your computer coming soon!
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Newsgroups: sci.physics Path: arc1-ca.pugleaf.net!sparky!uunet!well!sarfatti From: sarfatti@well.sf.ca.us (Jack Sarfatti) Subject: Feynman 27 "at any speed" Message-ID: <BxHIzs.HAD@well.sf.ca.us> Sender: news@well.sf.ca.us Organization: Whole Earth 'Lectronic Link Date: Tue, 10 Nov 1992 05:23:51 GMT Lines: 133