2007/08/18 by Ilia Gogoladze, Nobuchika Okada, Qaisar Shafi · 1 citation
Mathematics · Physics and Astronomy · #Black Holes and Theoretical Physics #Compactification (mathematics) #Cosmology and Gravitation Theories #Gauge (firearms) #Gauge boson #Gauge theory #Higgs boson #Higgs field #Mathematics #Orbifold #Particle physics #Particle physics theoretical and experimental studies #Physics #Quark #Standard Model (mathematical formulation) #Theoretical physics #Top quark #Yukawa potential #hep-ph #hep-th
paper · pdf · doi:10.1016/j.physletb.2007.11.059
published as Phys.Lett.B659:316-322,2008 · 15 pages, 7 figures
arxiv created 2007/08/18 · openalex publication_date 2007/12/04 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We consider six dimensional gauge models compactified on the orbifold T2/ZN (N=2,3,4,6) such that the Standard Model (SM) Higgs doublet arises from the extra-dimensional components of the gauge field. For Λ≤ 1019 GeV, where Λdenotes the compactification scale, we obtain 114.4 GeV ≤ mH ≤ 164 GeV for the SM Higgs boson mass. We also consider gauge-Higgs-top and gauge-Higgs-bottom Yukawa unification which respectively yield mH = 131+4-5 GeV and mH = 150+2-2 GeV for a top quark pole mass Mt =170.9+1.8-1.8 GeV. As a special case we recover the result mH ≤ 132 GeV previously obtained for five dimensional models.