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Strong and electroweak interactions and their unification with non-commutative space-time
Quantum field theories based on non-commutative space-time (NCQFT) have been extensively studied recently. However no NCQFT model which can uniquely describe the strong and electroweak interactions has been constructed. This prevents one to make a consistent and systematic study of non-commutative s...
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Published in: | The European physical journal. C, Particles and fields Particles and fields, 2003-06, Vol.28 (4), p.557-560 |
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Main Author: | |
Format: | Article |
Language: | English |
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Citations: | Items that cite this one |
Online Access: | Get full text |
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Summary: | Quantum field theories based on non-commutative space-time (NCQFT) have been extensively studied recently. However no NCQFT model which can uniquely describe the strong and electroweak interactions has been constructed. This prevents one to make a consistent and systematic study of non-commutative space-time. In this work we construct a NCQFT model based on the trinification gauge group \(SU(3)_C\times SU(3)_{{L}}\times SU(3)_{R}\). A unique feature of this model, that all matter fields (fermions and Higgs bosons) are assigned to (anti-) fundamental representations of the factor SU(3) groups, allows us to construct a NCQFT model for strong and electroweak interactions and their unification without ambiguities. This model provides an example which allows one to make a consistent and systematic study of non-commutative space-time phenomenology. We also comment on some related issues regarding extensions to E6 and \(U(3)_C\times U(3)_{L}\times U(3)_{R}\) models. |
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ISSN: | 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s2003-01185-5 |