Abstract
Rather than sticking to the full U(3)3 approximate symmetry normally invoked in Minimal Flavour Violation, we analyze the consequences on the current flavour data of a suitably broken U(2)3 symmetry acting on the first two generations of quarks and squarks. A definite correlation emerges between the ΔF=2 amplitudes \(\mathcal{M}( K^{0} \to \bar{K}^{0} )\), \(\mathcal{M}( B_{d} \to \bar{B}_{d} )\) and \(\mathcal{M}( B_{s} \to \bar{B}_{s} )\), which can resolve the current tension between \(\mathcal{M}( K^{0} \to \bar{K}^{0} )\) and \(\mathcal{M}( B_{d} \to \bar{B}_{d} )\), while predicting \(\mathcal{M}( B_{s}\to \bar{B}_{s} )\). In particular, the CP violating asymmetry in B s →ψφ is predicted to be positive S ψφ =0.12±0.05 and above its Standard Model value (S ψφ =0.041±0.002). The preferred region for the gluino and the left-handed sbottom masses is below about 1÷1.5 TeV. An existence proof of a dynamical model realizing the U(2)3 picture is outlined.
Similar content being viewed by others
References
R.S. Chivukula, H. Georgi, Phys. Lett. B 188, 99 (1987)
L.J. Hall, L. Randall, Phys. Rev. Lett. 65, 2939–2942 (1990)
G. D’Ambrosio, G.F. Giudice, G. Isidori, A. Strumia, Nucl. Phys. B 645, 155–187 (2002). arXiv:hep-ph/0207036
A. Pomarol, D. Tommasini, Nucl. Phys. B 466, 3–24 (1996). arXiv:hep-ph/9507462
R. Barbieri, G.R. Dvali, L.J. Hall, Phys. Lett. B 377, 76–82 (1996). arXiv:hep-ph/9512388
R. Barbieri, L.J. Hall, A. Romanino, Phys. Lett. B 401, 47–53 (1997). arXiv:hep-ph/9702315
E. Lunghi, A. Soni, Phys. Lett. B 666, 162–165 (2008). arXiv:0803.4340 [hep-ph]
A.J. Buras, D. Guadagnoli, Phys. Rev. D 78, 033005 (2008). arXiv:0805.3887 [hep-ph]
W. Altmannshofer, A.J. Buras, S. Gori, P. Paradisi, D.M. Straub, Nucl. Phys. B 830, 17–94 (2010). arXiv:0909.1333 [hep-ph]
E. Lunghi, A. Soni, Phys. Lett. B 697, 323–328 (2011). arXiv:1010.6069 [hep-ph]
A.J. Bevan et al. (UTfit Collaboration), arXiv:1010.5089 [hep-ph]. And updates at http://www.utfit.org
V.M. Abazov et al. (D0 Collaboration), Phys. Rev. D 82, 032001 (2010). arXiv:1005.2757 [hep-ex]
A. Lenz et al., Phys. Rev. D 83, 036004 (2011). arXiv:1008.1593 [hep-ph]
J.C. Hardy, I.S. Towner, Phys. Rev. C 79, 055502 (2009). arXiv:0812.1202 [nucl-ex]
J. Laiho, E. Lunghi, R.S. Van de Water, Phys. Rev. D 81, 034503 (2010). arXiv:0910.2928 [hep-ph]. And updates at http://www.latticeaverages.org
M. Antonelli et al., Eur. Phys. J. C 69, 399–424 (2010). arXiv:1005.2323 [hep-ph]
G. Colangelo et al., arXiv:1011.4408 [hep-lat]
A.J. Buras, D. Guadagnoli, G. Isidori, Phys. Lett. B 688, 309–313 (2010). arXiv:1002.3612 [hep-ph]
B. Kowalewski, Talk at BEAUTY 2011, Amsterdam
E. Lunghi, A. Soni, arXiv:1104.2117 [hep-ph]
K. Nakamura et al. (Particle Data Group Collaboration), J. Phys. G 37, 075021 (2010)
D. Asner et al. (Heavy Flavor Averaging Group Collaboration), arXiv:1010.1589 [hep-ex]. And updates at http://www.slac.stanford.edu/xorg/hfag/
A. Abulencia et al. (CDF Collaboration), Phys. Rev. Lett. 97, 242003 (2006). arXiv:hep-ex/0609040
R. Barbieri, L.J. Hall, A. Romanino, Nucl. Phys. B 551, 93–101 (1999). arXiv:hep-ph/9812384
Z. Ligeti, M. Papucci, G. Perez, J. Zupan, Phys. Rev. Lett. 105, 131601 (2010). arXiv:1006.0432 [hep-ph]
M. Blanke, A.J. Buras, D. Guadagnoli, C. Tarantino, J. High Energy Phys. 10, 003 (2006). arXiv:hep-ph/0604057
N. Craig, D. Green, A. Katz, arXiv:1103.3708 [hep-ph]
A.L. Kagan, G. Perez, T. Volansky, J. Zupan, Phys. Rev. D 80, 076002 (2009). arXiv:0903.1794 [hep-ph]
R. Barbieri, P. Lodone, D.M. Straub, arXiv:1102.0726 [hep-ph]
Author information
Authors and Affiliations
Corresponding author
Rights and permissions
About this article
Cite this article
Barbieri, R., Isidori, G., Jones-Pérez, J. et al. U(2) and minimal flavour violation in supersymmetry. Eur. Phys. J. C 71, 1725 (2011). https://doi.org/10.1140/epjc/s10052-011-1725-z
Received:
Revised:
Published:
DOI: https://doi.org/10.1140/epjc/s10052-011-1725-z