Phenomenology of a gauged SU(3) 3 avour model

Andrzej J. Buras, Maria Valentina Carlucci, Luca Merlo, Emmanuel Stamou

Research output: Contribution to journalArticlepeer-review

47 Scopus citations

Abstract

We present an extensive analysis of ΔF = 2 observables and of B → X in the framework of a specific Maximally Gauged Flavour (MGF) model of Grinstein et al. including all relevant contributions, in particular tree-level heavy gauge boson exchanges whose effects are studied in detail in the present paper for the first time. The model allows in principle for significant deviations from the Standard Model predictions for ε K, ΔM Bd,s, mixing induced CP-asymmetries S ψKS and S ψφ and B → X decay. The tension between ε K and S ψKS present in the SM can be removed by enhancing εK without modifying S ψKS. In this case, we find that in this model i) the results for S ψφ and B → X turn out to be SM-like, ii) the exclusive determination of V ub is favoured and most importantly iii) the values of ΔM Bd and Δ MBs being strongly correlated in this model with ε K turn out to be much larger than the data for the central values of input parameters: ΔM Bd ≈ 0:75=ps and ΔM Bs ≈ 27=ps. Therefore, from the present perspective, the model suffers from a serious ε K-ΔM Bd,s tension. However, this tension can be softened considering theoretical and parametric uncertainties and in particular the decrease of the weak decay constants. On the other side, the model can be strongly constrained considering the theoretically cleaner ratios ΔM Bd=ΔM Bs and BR(B+ → τ +V)= ΔM Bd and we find that it is unable to remove simultaneously all the SM tensions on the data. Finally, we compare the pattern of avour violation in MGF with selected extensions of the SM.

Original languageEnglish
Article number088
JournalJournal of High Energy Physics
Volume2012
Issue number3
DOIs
StatePublished - 2012

Keywords

  • B-Physics
  • Beyond Standard Model
  • Gauge Symmetry
  • Quark Masses and SM Parameters

Fingerprint

Dive into the research topics of 'Phenomenology of a gauged SU(3) 3 avour model'. Together they form a unique fingerprint.

Cite this