A Model of Strong Flavor Dynamics for the Top Quark
| dc.creator | Malkawi, Ehab | |
| dc.creator | Tait, Tim | |
| dc.creator | Yuan, C. --P. | |
| dc.date | 1996-03-19 | |
| dc.date.accessioned | 2026-07-07T12:03:16Z | |
| dc.date.available | 2026-07-07T12:03:16Z | |
| dc.description | We discuss a model in which the third generation fermions undergo a different $SU(2)$ weak interaction from the first two generation fermions. In general, a flavor changing neutral current interaction is expected. Constrained by the precision low energy data, the mass ($M_{Z'}=M_{W'}$) of the heavy gauge bosons is bounded from below to be about $1.1$ TeV for $α_s=0.125$ and about $1.3$ TeV for $α_s=0.115$, at the $3σ$ level. This model favors a larger $R_b$ and a smaller $R_c$ as compared with the Standard Model, but it does not explain the $R_c$ data. If one takes the $R_b$ data seriously, then $M_{Z'}$ is bounded, at the $3σ$ level, to be $462$ GeV $< M_{Z^{\prime}} \cosϕ< 1481\,\, {\rm{GeV}}$, where $\cosϕ$ is the mixing angle between the two $SU(2)$'s in the model. Effects predicted for high energy experiments at the Tevatron, LEP140, LEP-II, LHC, and future linear colliders are also discussed. | |
| dc.description | 12 pages LaTeX; 2 figures included as separate files in postscript format | |
| dc.identifier | https://arxiv.org/abs/hep-ph/9603349 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/9603349 | |
| dc.identifier | Phys.Lett.B385:304-310,1996 | |
| dc.identifier | doi:10.1016/0370-2693(96)00859-3 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/207726 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | A Model of Strong Flavor Dynamics for the Top Quark | |
| dc.type | text |