Bounds of the mass of Z' and the neutral mixing angles in general SU(2)_L x SU(2)_R x U(1) models

dc.creatorChay, Junegone
dc.creatorLee, Kang Young
dc.creatorNam, Soo-hyeon
dc.date1998-09-08
dc.date.accessioned2026-07-07T10:33:44Z
dc.date.available2026-07-07T10:33:44Z
dc.descriptionWe consider phenomenological constraints on the mass $M_{Z^{\prime}}$ and the two mixing angles $θ_R$ and $ξ$ of the neutral sector in a very general class of $SU(2)_L \times SU(2)_R \times U(1)$ models using electroweak data. We do not make any specific assumptions such as left-right symmetry or the Higgs structure. The analysis of the neutral sector has the advantage that it has relatively fewer parameters compared to the charged sector since the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements in the right-handed sector do not enter into the analysis, hence the number of various possibilities from a big parameter space is reduced. We utilize theoretical considerations on the masses of the gauge particles and the mixing angles. We combine the precision electroweak data from LEP I and the low-energy neutral-current experimental data to constrain the parameters introduced in the model. It turns out that $M_{Z^{\prime}}> 400$ GeV, $-0.0028 <ξ<0.0065$ with little constraint on $θ_R$. In the left-right symmetric theory, $M_{Z^{\prime}}$ should be larger than 900 GeV. With these constraints, we compare the values for $σ(e^+ e^- \to μ^+ μ^-)$, $σ(e^+ e^- \to b\bar{b})$ and $A_{FB}^{\ell}$ at LEP II with experimental values.
dc.description34 pages, a LaTeX file with macros elsart and pictex. 4 Figures
dc.identifierhttps://arxiv.org/abs/hep-ph/9809298
dc.identifierhttp://arxiv.org/abs/hep-ph/9809298
dc.identifierPhys.Rev.D61:035002,2000
dc.identifierdoi:10.1103/PhysRevD.61.035002
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/179220
dc.subjectHigh Energy Physics - Phenomenology
dc.titleBounds of the mass of Z' and the neutral mixing angles in general SU(2)_L x SU(2)_R x U(1) models
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