An Approach to Classical Quantum Field Theory Based on the Geometry of Locally Conformally Flat Space-Time

This paper gives an introduction to certain classical physical theories described in the context of locally Minkowskian causal structures (LMCSs). For simplicity of exposition we consider LMCSs which have locally Euclidean topology (i.e., are manifolds) and hence are Möbius structures. We describe n...

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Main Author: John Mashford
Format: Article
Language:English
Published: Hindawi Limited 2017-01-01
Series:Advances in Mathematical Physics
Online Access:http://dx.doi.org/10.1155/2017/8070462
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spelling doaj-7fab2d7980454c7e87f19762e834e3752021-07-02T09:53:52ZengHindawi LimitedAdvances in Mathematical Physics1687-91201687-91392017-01-01201710.1155/2017/80704628070462An Approach to Classical Quantum Field Theory Based on the Geometry of Locally Conformally Flat Space-TimeJohn Mashford0School of Mathematics and Statistics, University of Melbourne, Parkville, VIC 3010, AustraliaThis paper gives an introduction to certain classical physical theories described in the context of locally Minkowskian causal structures (LMCSs). For simplicity of exposition we consider LMCSs which have locally Euclidean topology (i.e., are manifolds) and hence are Möbius structures. We describe natural principal bundle structures associated with Möbius structures. Fermion fields are associated with sections of vector bundles associated with the principal bundles while interaction fields (bosons) are associated with endomorphisms of the space of fermion fields. Classical quantum field theory (the Dirac equation and Maxwell’s equations) is obtained by considering representations of the structure group K⊂SU(2,2) of a principal bundle associated with a given Möbius structure where K, while being a subset of SU(2,2), is also isomorphic to SL2,C×U(1). The analysis requires the use of an intertwining operator between the action of K on R4 and the adjoint action of K on su⁡(2,2) and it is shown that the Feynman slash operator, in the chiral representation for the Dirac gamma matrices, has this intertwining property.http://dx.doi.org/10.1155/2017/8070462
collection DOAJ
language English
format Article
sources DOAJ
author John Mashford
spellingShingle John Mashford
An Approach to Classical Quantum Field Theory Based on the Geometry of Locally Conformally Flat Space-Time
Advances in Mathematical Physics
author_facet John Mashford
author_sort John Mashford
title An Approach to Classical Quantum Field Theory Based on the Geometry of Locally Conformally Flat Space-Time
title_short An Approach to Classical Quantum Field Theory Based on the Geometry of Locally Conformally Flat Space-Time
title_full An Approach to Classical Quantum Field Theory Based on the Geometry of Locally Conformally Flat Space-Time
title_fullStr An Approach to Classical Quantum Field Theory Based on the Geometry of Locally Conformally Flat Space-Time
title_full_unstemmed An Approach to Classical Quantum Field Theory Based on the Geometry of Locally Conformally Flat Space-Time
title_sort approach to classical quantum field theory based on the geometry of locally conformally flat space-time
publisher Hindawi Limited
series Advances in Mathematical Physics
issn 1687-9120
1687-9139
publishDate 2017-01-01
description This paper gives an introduction to certain classical physical theories described in the context of locally Minkowskian causal structures (LMCSs). For simplicity of exposition we consider LMCSs which have locally Euclidean topology (i.e., are manifolds) and hence are Möbius structures. We describe natural principal bundle structures associated with Möbius structures. Fermion fields are associated with sections of vector bundles associated with the principal bundles while interaction fields (bosons) are associated with endomorphisms of the space of fermion fields. Classical quantum field theory (the Dirac equation and Maxwell’s equations) is obtained by considering representations of the structure group K⊂SU(2,2) of a principal bundle associated with a given Möbius structure where K, while being a subset of SU(2,2), is also isomorphic to SL2,C×U(1). The analysis requires the use of an intertwining operator between the action of K on R4 and the adjoint action of K on su⁡(2,2) and it is shown that the Feynman slash operator, in the chiral representation for the Dirac gamma matrices, has this intertwining property.
url http://dx.doi.org/10.1155/2017/8070462
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