PMEM and Unification

PMEM and Unification

Pre-metric electromagnetism as a path to unification. DAVID DELPHENICH Independent researcher Spring Valley, OH 45370, USA [email protected] It is shown that the pre-metric approach to Maxwell’s equations provides an alternative to the traditional Einstein- Maxwell unification problem, namely, that electromagnetism and gravitation are unified in a different way that makes the gravitational field a consequence of the electromagnetic constitutive properties of spacetime, by way of the dispersion law for the propagation of electromagnetic waves. Keyw ords: Pre-metric electromagnetism, Einstein-Maxwell unification problem, line geometry, electromagnetic constitutive laws 1. The Einstein-Maxwell unification problem. fundamental distinctions between them, as well. In particular, the analogy between mass and Ever since Einstein succeeded in accounting for charge was not complete, since at the time (and the presence of gravitation in the universe by to this point in time, as well), no one had ever showing how it was a natural consequence of the observed what one might call “negative” mass or curvature of the Levi-Civita connection that one “anti-gravitation.” Of course, the possibility that derived from the Lorentzian metric on the such a unification of gravitation and spacetime manifold, he naturally wondered if the electromagnetism might lead to such tantalizing other fundamental force of nature that was consequences has been an ongoing source of known at the time – namely, electromagnetism – impetus for the search for that theory. could also be explained in a similar way. Since Several attempts followed by Einstein and the best-accepted theory of electromagnetism at others (cf., e.g., [1] and part II of [2]) at the time (as well as the best-accepted “classical” achieving such a unification. They seemed to theory to this day) was Maxwell’s theory, that fall into two basic categories: Extensions of g gave rise to what one might called the Einstein- with a four-dimensional spacetime and Maxwell unification problem: Find some extensions of spacetime to something higher- intrinsic (presumably geometric) structure on dimensional. The former models included spacetime (suitably extended) that will teleparallelism 1 and the Einstein-Schrödinger decompose into (or at least lead to) the theory [2], while the latter include the Kaluza- Lorentzian metric tensor g and the Klein models [1, 2, 4, 5], and some of the electromagnetic field strength 2-form F, along attempts to extend the tangent bundle of the four- with a set of field equations for that extended dimensional spacetime manifold to an geometric structure that would imply the anholonomic (i.e., non-integrable) rank-4 sub- Einstein field equations for g and the Maxwell bundle of the tangent bundle to a five- equations for F (at least, in some dimensional manifold (cf., e.g., [6-8]). approximation). All of the attempts were regarded as failures The suspicion that such a “unified field for one reason or another. One problem with theory” might actually exist was perhaps based upon the fact that Maxwell’s theory itself represented a “unified field theory” of the 1 The author has compiled an anthology [3] of electric and magnetic fields, and that there English translations of many of the early papers existed a well-known analogy between on teleparallelism that is available as a free PDF Coulomb’s law of electrostatics and Newton’s download at his website (neo-classical- law of universal gravitation, although there were physics.info) 2 Pre-metric electromagnetism as a path to unification teleparallelism was that it included unphysical passed over that “classical” problem 1 and started solutions, such as a static distribution of with the exchange-particle concept, combined gravitating, uncharged masses. The main with the scattering approximation for the field problem with the other theories was that they dynamics. That means: Rather than speculate on implied no new consequences of that unification; what might constitute the “field equations of i.e., they were “concatenations” of the field QED” or the nature of the electromagnetic theories, not unifications. What was missing “force” that acts between elementary charges at were any sort of “gravito-electromagnetic the quantum level, quantum physics was going to inductions,” that would suggest an analogue to replace the force of interaction with the exchange the electromagnetic induction in Maxwell’s of an elementary particle that would mediate the theory. Indeed, it is important to note that the interaction; for QED, that particle would be the latter inductions had been established photon. Then, rather than posing “classical” experimentally by Faraday before Maxwell problems, such as boundary-value problems in formulated his theory, while to date, no such statics and the Cauchy problem in dynamics, couplings of electromagnetic and gravitational QED would simply pass to the approximation in fields seem to have materialized in the which the initial time was − ∞ and the final time laboratory. (“Gravitomagnetism” is a different was + ∞, which is equivalent to assuming that matter, and we shall discuss it below.) the interaction of particles takes place inside a However, as quantum physics evolved, the very small “black box” time interval in which the nature of the Einstein-Maxwell unification nonlinear nature of the interaction can be problem changed, as well. Increasingly, Einstein enclosed in such a way that the time evolution suspected that gravitation could only be unified operator that takes incoming fields to outgoing with electromagnetism when one went to ones becomes a linear operator that takes quantum electromagnetism. That possibility incoming scattering states (which are asymptotic seems more reasonable nowadays, since the free fields) to outgoing ones. That allows one to phenomenon of “gravitomagnetism” had not use the methods of Fourier analysis and discuss been observed experimentally until relatively the scattering operator in momentum space recently [9]. The essence of that phenomenon is without having to worry that the perturbation that the analogy between Coulomb’s law and series that one defines (i.e., Feynman diagrams Newton’s law goes beyond the scope of statics, or loop expansions) is unphysical. since there is, in fact, a field that is induced by Of course, it is precisely the fundamental the relative motion of a mass that is analogous to distinction between Einstein’s theory of the magnetic field that is induced by the relative gravitation as a “classical” field theory (i.e., one motion of an electric charge, and which is in which one can pose boundary-value problems commonly called the gravitomagnetic field . As a in statics and the Cauchy problem in dynamics), result, one sees that Maxwell’s equations are while QED is a “quantum” field theory (i.e., one closely analogous to the weak-field equations of that begins in the scattering approximation to gravitation, which suggests that perhaps that Cauchy problem) that is the greatest Einstein’s equations of gravitation, which are the obstruction to the unification of those theories, strong-field equations, should be somehow although that fact is rarely addressed in quantum analogous to some hitherto-unknown “strong- gravity, which takes more of a “play it where it field” equations of electromagnetism. lays” approach. The physical realm in which one would Another common critique of the Einstein- expect to find the strongest electromagnetic Maxwell unification problem is that it is fields is in the atomic to subatomic domain, currently a partial unification problem, in the where one approaches the Schwinger critical sense that since the time of Einstein’s early work field strengths at which photons resolve into on gravitation, two other “quantum” interactions electron-positron field-pairs. However, since the time of Heisenberg and Pauli [10], quantum 1 One might suspect that the quantum use of the electrodynamics has not started with a set of word “classical” in a pejorative way is probably “strong-field equations of electromagnetism” an imitation of the pure-mathematical usage of that might perhaps be analogous to Einstein’s the word “trivial,” which often represents little equations of gravitation. Rather, it has simply more than a lack of personal curiosity about the subject, combined with an acceptance of the fact that the problem in question is hard to pose and even harder to solve. David Delphenich 3 have been added to the fundamental interactions, makes perfect sense in the context of the “pre- namely, the weak and strong interactions. metric” approach to electromagnetism. That Furthermore, once Yang and Mills had revisited approach is based upon the observation that the the gauge-field approach to elementary only place in which the Lorentzian metric on interactions that Weyl, Fock, and Ivanenko had spacetime enters into Maxwell’s equations is in studied in the context of electromagnetism at the Hodge * operator. In order to see that, we about the same time that Einstein was pondering express those equations in terms of the unified field theory and the Copenhagen school Minkowski electromagnetic field-strength 2- was defining their foundations for quantum form F as 1: physics, the unification of electromagnetism with the weak interactions as gauge field theories dF = 0, δF = 4 πJ, δJ = 0, (1) defined an entirely different approach to unification that usually took the form of looking in which d represents the exterior derivative for higher-dimensional

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