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Modified Weyl theory and extended elementary objects
Authors:W Drechsler
Institution:(1) Max-Planck-Institut für Physik und Astrophysik, Werner-Heisenberg-Institut für Physik, P.O. Box 40 12 12, Munich, Federal Republic of Germany
Abstract:To represent extension of objects in particle physics, a modified Weyl theory is used by gauging the curvature radius of the local fibers in a soldered bundle over space-time possessing a homogeneous space G/H of the (4, 1)-de Sitter group G as fiber. Objects with extension determined by a fundamental length parameter R0 appear as islands D(i) in space-time characterized by a geometry of the Cartan-Weyl type (i.e., involving torsion and modified Weyl degrees of freedom). Farther away from the domains D(i), space-time is identified with the pseudo-Riemannian space of general relativity. Extension and symmetry breaking are described by a set of additional fields ( 
$$(\tilde \xi ^a (x),R(x)) \in {G \mathord{\left/ {\vphantom {G H}} \right. \kern-\nulldelimiterspace} H}x R^ +$$
, given as a section on an associated bundle 
$$\tilde E(B,{G \mathord{\left/ {\vphantom {G H}} \right. \kern-\nulldelimiterspace} H}x R^ +  ,\tilde G)$$
over space-time B with structural group 
$$\tilde G$$
= G otimes D(1), where D(1) is the dilation group. Field equations for the quantities defining the underlying bundle geometry and for the fields 
$$\tilde \xi ^a (x)$$
are established involving matter source currents derived from a generalized spinor wave function. Einstein's equations for the metric are regarded as the part of the 
$$\tilde G$$
-gauge theory related to the Lorentz subgroup H of G exhibiting thereby the broken nature of the 
$$\tilde G$$
-symmetry for regions outside the domains D(i).Talk presented at the International Conference on Field Theory and General Relativity held at Utah State University, Logan, Utah, June 26–July 2, 1988.
Keywords:
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