1997
DOI: 10.1016/s0370-2693(97)01181-7
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String scale unification in an SU(6) × SU(2) GUT

Abstract: We construct and analyze an SU(6)×SU(2) GUT. The model is k=1 string embedable in the sense that we employ only chiral representations allowed at the k=1 level of the associated Kač-Moody Algebra. Both cases SU(6) × SU(2) L and SU(6) × SU(2) R are realized. The model is characterized by the SU(6) × SU(2) → SU(4) × SU(2) × SU(2) breaking scale M X , and theThe spectrum bellow M R includes an extra pair of charge-1/3 colour-triplets of mass M I ≤ M R that does not couple to matter fields and, possibly, an extra … Show more

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Cited by 7 publications
(14 citation statements)
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“…This symmetry breaking chain was proposed in [64]. The decomposition of 27 representation of E 6 in terms of gauge group…”
Section: Brief Review Of Grand Unified Theoriesmentioning
confidence: 99%
“…This symmetry breaking chain was proposed in [64]. The decomposition of 27 representation of E 6 in terms of gauge group…”
Section: Brief Review Of Grand Unified Theoriesmentioning
confidence: 99%
“…One possibility is the SU (6)×SU (2) gauge group, a maximal subgroup of E 6 , which also allows us to implement the "deunification" scenario for proton decay suppression. There are two possible embeddings of the weak isospin in this gauge group, namely SU (6) × SU (2) L and SU (6) × SU (2) R [10]. However, only the SU (6) × SU (2) R gauge symmetry admits an SU (5) × U (1) X subgroup.…”
Section: An Extended Flipped Su (5) Modelmentioning
confidence: 99%
“…where N c H , N c H are the singlets residing in H (10,1) , H (10,−1) of the SU (5) × U (1) subgroup respectively and…”
Section: An Extended Flipped Su (5) Modelmentioning
confidence: 99%
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“…Consider for example, the fermion multiplets of one family in Flipped SU (5). Under the SU( 5) ×U(1) they transform as 10 1 + 5 −3 + 1 5 , where the superscripts denote the U(1) charges.…”
Section: Introductionmentioning
confidence: 99%