科研之友
微信
新浪微博
Facebook
分享链接
摘要
We introduce a toy model implementing the proposal of using a custodial symmetry to protect the Zb(L)b(L) coupling from large corrections. This "doublet-extended standard model" adds a weak doublet of fermions (including a heavy partner of the top quark) to the particle content of the standard model in order to implement an O(4)xU(1)(X)similar to SU(2)(L)xSU(2)(R)xP(LR)xU(1)(X) symmetry in the top-quark mass generating sector. This symmetry is softly broken to the gauged SU(2)(L)xU(1)(Y) electroweak symmetry by a Dirac mass M for the new doublet; adjusting the value of M allows us to explore the range of possibilities between the O(4)-symmetric (M -> 0) and standard-model-like (M ->infinity) limits. In this simple model, we find that the experimental limits on the Zb(L)b(L) coupling favor smaller M while the presence of a potentially sizable negative contribution to alpha T strongly favors large M. Comparison with precision electroweak data shows that the heavy partner of the top quark must be heavier than about 3.4 TeV, making it difficult to search for at LHC. This result demonstrates that electroweak data strongly limit the amount by which the custodial symmetry of the top-quark mass generating sector can be enhanced relative to the standard model. Using an effective field theory calculation, we illustrate how the leading contributions to alpha T, alpha S, and the Zb(L)b(L) coupling in this model arise from an effective operator coupling right-handed top quarks to the Z boson, and how the effects on these observables are correlated. We contrast this toy model with extradimensional models in which the extended custodial symmetry is invoked to control the size of additional contributions to alpha T and the Zb(L)b(L) coupling, while leaving the standard model contributions essentially unchanged.
- 出版日期2009-11
