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...

Full description

Bibliographic Details
Main Authors: Adam B. Gillard, Niels G. Gresnigt
Format: Article
Language:English
Published: SpringerOpen 2019-05-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-019-6967-1
id doaj-51071cdfa4d64285afdee7a0c80cbbb1
record_format Article
spelling 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
_version_ 1724626695089029120