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MODELLING THE ELECTRON WITH COSSERAT ELASTICITY

Published online by Cambridge University Press:  12 April 2012

James Burnett
Affiliation:
Department of Mathematics and Institute of Origins, University College London, Gower Street, London WC1E 6BT, U.K. (email: [email protected])
Dmitri Vassiliev
Affiliation:
Department of Mathematics and Institute of Origins, University College London, Gower Street, London WC1E 6BT, U.K. (email: [email protected])
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Abstract

We suggest an alternative mathematical model for the electron in dimension 1+2. We think of our (1+2)-dimensional spacetime as an elastic continuum whose material points can experience no displacements, only rotations. This framework is a special case of the Cosserat theory of elasticity. Rotations of material points are described mathematically by attaching to each geometric point an orthonormal basis which gives a field of orthonormal bases called the coframe. As the dynamical variables (unknowns) of our theory we choose a coframe and a density. We then add an extra (third) spatial dimension, extend our coframe and density into dimension 1+3, choose a conformally invariant Lagrangian proportional to axial torsion squared, roll up the extra dimension into a circle so as to incorporate mass and return to our original (1+2)-dimensional spacetime by separating out the extra coordinate. The main result of our paper is the theorem stating that our model is equivalent to the Dirac equation in dimension 1+2. In the process of analysing our model we also establish an abstract result, identifying a class of nonlinear second order partial differential equations which reduce to pairs of linear first order equations.

Type
Research Article
Copyright
Copyright © University College London 2012

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References

[1]Ball, J. M. and Zarnescu, A., Orientable and non-orientable director fields for liquid crystals. Proc. Appl. Math. Mech. 7(1) (2007), 10507011050704.CrossRefGoogle Scholar
[2]Berestetskii, V. B., Lifshitz, E. M. and Pitaevskii, L. P., Quantum Electrodynamics, 2nd edn. (Course of theoretical physics 4), Butterworth–Heinemann (Oxford, 1982), translated from the Russian by J. B. Sykes and J. S. Bell.Google Scholar
[3]Böhmer, C. G., Downes, R. J. and Vassiliev, D., Rotational elasticity. Quart. J. Mech. Appl. Math. 64(4) (2011), 415439.CrossRefGoogle Scholar
[4]Burnett, J. and Vassiliev, D., Weyl’s Lagrangian in teleparallel form. J. Math. Phys. 50(10) (2009), 102501, 17pp.CrossRefGoogle Scholar
[5]Cartan, É., Sur une généralisation de la notion de courbure de riemann et les espaces à torsion. C. R. Acad. Sci. Paris 174 (1922), 593595.Google Scholar
[6]Cartan, É. and Einstein, A., Letters on Absolute Parallelism, 1929–1932, Princeton University Press (Princeton, NJ, 1979), original text with English translation by Jules Leroy and Jim Ritter, edited by Robert Debever.Google Scholar
[7]Chervova, O. and Vassiliev, D., The stationary Weyl equation and Cosserat elasticity. J. Phys. A 43(33) (2010), 335203, 14pp.CrossRefGoogle Scholar
[8]Cosserat, E. and Cosserat, F., Théorie des corps déformables, Librairie Scientifique A. Hermann et Fils (Paris, 1909), reprinted by Cornell University Library.Google Scholar
[9]Elton, D. and Vassiliev, D., The Dirac equation without spinors. In The Maz’ya Anniversary Collection, Vol. 2 (Rostock, 1998) (Operator Theory: Advances and Applications 110), Birkhäuser (Basel, 1999), 133152.CrossRefGoogle Scholar
[10]Griffiths, J. B. and Newing, R. A., Tetrad equations for the two-component neutrino field in general relativity. J. Phys. A 3 (1970), 269273.CrossRefGoogle Scholar
[11]Hehl, F. W. and Obukhov, Y. N., Élie Cartan’s torsion in geometry and in field theory, an essay. Ann. Fond. Louis de Broglie 32(2,3) (2007), 157194.Google Scholar
[12]Nester, J. M., Special orthonormal frames. J. Math. Phys. 33(3) (1992), 910913.CrossRefGoogle Scholar
[13]Obukhov, Y. N., Conformal invariance and space-time torsion. Phys. Lett. A 90(1,2) (1982), 1316.CrossRefGoogle Scholar
[14]Sauer, T., Field equations in teleparallel space-time: Einstein’s fernparallelismus approach toward unified field theory. Historia Math. 33(4) (2006), 399439.CrossRefGoogle Scholar
[15]Unzicker, A. and Case, T., Translation of Einstein’s attempt of a unified field theory with teleparallelism. Preprint, 2005, arXiv:physics/0503046v1.Google Scholar
[16]Vassiliev, D., Teleparallel model for the neutrino. Phys. Rev. D 75(2) (2007), 025006, 6pp.CrossRefGoogle Scholar