Three fermion generations with two unbroken gauge symmetries from the complex sedenions
Abstract We show that three generations of leptons and quarks with unbroken Standard Model gauge symmetry $$SU(3)_c\times U(1)_{em}$$ SU(3)c×U(1)em can be described using the algebra of complexified sedenions $${\mathbb {C}}\otimes {\mathbb {S}}$$ C⊗S . A primitive idempotent is constructed by selec...
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Series: | European Physical Journal C: Particles and Fields |
Online Access: | http://link.springer.com/article/10.1140/epjc/s10052-019-6967-1 |
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doaj-51071cdfa4d64285afdee7a0c80cbbb12020-11-25T03:18:27ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-05-0179511110.1140/epjc/s10052-019-6967-1Three fermion generations with two unbroken gauge symmetries from the complex sedenionsAdam B. Gillard0Niels G. Gresnigt1Department of Mathematical Sciences, Xi’an Jiaotong-Liverpool UniversityDepartment of Mathematical Sciences, Xi’an Jiaotong-Liverpool UniversityAbstract We show that three generations of leptons and quarks with unbroken Standard Model gauge symmetry $$SU(3)_c\times U(1)_{em}$$ SU(3)c×U(1)em can be described using the algebra of complexified sedenions $${\mathbb {C}}\otimes {\mathbb {S}}$$ C⊗S . A primitive idempotent is constructed by selecting a special direction, and the action of this projector on the basis of $${\mathbb {C}}\otimes {\mathbb {S}}$$ C⊗S can be used to uniquely split the algebra into three complex octonion subalgebras $${\mathbb {C}}\otimes {\mathbb {O}}$$ C⊗O . These subalgebras all share a common quaternionic subalgebra. The left adjoint actions of the 8 $${\mathbb {C}}$$ C -dimensional $${\mathbb {C}}\otimes {\mathbb {O}}$$ C⊗O subalgebras on themselves generates three copies of the Clifford algebra $${\mathbb {C}}\ell (6)$$ Cℓ(6) . It was previously shown that the minimal left ideals of $${\mathbb {C}}\ell (6)$$ Cℓ(6) describe a single generation of fermions with unbroken $$SU(3)_c\times U(1)_{em}$$ SU(3)c×U(1)em gauge symmetry. Extending this construction from $${\mathbb {C}}\otimes {\mathbb {O}}$$ C⊗O to $${\mathbb {C}}\otimes {\mathbb {S}}$$ C⊗S naturally leads to a description of exactly three generations.http://link.springer.com/article/10.1140/epjc/s10052-019-6967-1 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Adam B. Gillard Niels G. Gresnigt |
spellingShingle |
Adam B. Gillard Niels G. Gresnigt Three fermion generations with two unbroken gauge symmetries from the complex sedenions European Physical Journal C: Particles and Fields |
author_facet |
Adam B. Gillard Niels G. Gresnigt |
author_sort |
Adam B. Gillard |
title |
Three fermion generations with two unbroken gauge symmetries from the complex sedenions |
title_short |
Three fermion generations with two unbroken gauge symmetries from the complex sedenions |
title_full |
Three fermion generations with two unbroken gauge symmetries from the complex sedenions |
title_fullStr |
Three fermion generations with two unbroken gauge symmetries from the complex sedenions |
title_full_unstemmed |
Three fermion generations with two unbroken gauge symmetries from the complex sedenions |
title_sort |
three fermion generations with two unbroken gauge symmetries from the complex sedenions |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2019-05-01 |
description |
Abstract We show that three generations of leptons and quarks with unbroken Standard Model gauge symmetry $$SU(3)_c\times U(1)_{em}$$ SU(3)c×U(1)em can be described using the algebra of complexified sedenions $${\mathbb {C}}\otimes {\mathbb {S}}$$ C⊗S . A primitive idempotent is constructed by selecting a special direction, and the action of this projector on the basis of $${\mathbb {C}}\otimes {\mathbb {S}}$$ C⊗S can be used to uniquely split the algebra into three complex octonion subalgebras $${\mathbb {C}}\otimes {\mathbb {O}}$$ C⊗O . These subalgebras all share a common quaternionic subalgebra. The left adjoint actions of the 8 $${\mathbb {C}}$$ C -dimensional $${\mathbb {C}}\otimes {\mathbb {O}}$$ C⊗O subalgebras on themselves generates three copies of the Clifford algebra $${\mathbb {C}}\ell (6)$$ Cℓ(6) . It was previously shown that the minimal left ideals of $${\mathbb {C}}\ell (6)$$ Cℓ(6) describe a single generation of fermions with unbroken $$SU(3)_c\times U(1)_{em}$$ SU(3)c×U(1)em gauge symmetry. Extending this construction from $${\mathbb {C}}\otimes {\mathbb {O}}$$ C⊗O to $${\mathbb {C}}\otimes {\mathbb {S}}$$ C⊗S naturally leads to a description of exactly three generations. |
url |
http://link.springer.com/article/10.1140/epjc/s10052-019-6967-1 |
work_keys_str_mv |
AT adambgillard threefermiongenerationswithtwounbrokengaugesymmetriesfromthecomplexsedenions AT nielsggresnigt threefermiongenerationswithtwounbrokengaugesymmetriesfromthecomplexsedenions |
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1724626695089029120 |