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Future sensitivity to new physics in Bd, Bs, and K mixings

Jérôme Charles1,2,*, Sébastien Descotes-Genon3,*, Zoltan Ligeti4, Stéphane Monteil5,*, Michele Papucci6, and Karim Trabelsi7,*

  • 1Aix-Marseille Université, CNRS, CPT, UMR 7332, 13288 Marseille, France
  • 2Université de Toulon, CNRS, CPT, UMR 7332, 83957 La Garde, France
  • 3Laboratoire de Physique Théorique, CNRS/Univ. Paris-Sud 11 (UMR 8627) 91405 Orsay Cedex, France
  • 4Ernest Orlando Lawrence Berkeley National Laboratory, University of California, Berkeley, California 94720, USA
  • 5Laboratoire de Physique Corpusculaire de Clermont-Ferrand Université Blaise Pascal, 24 Avenue des Landais F-63177 Aubiere Cedex, France
  • 6Michigan Center for Theoretical Physics, University of Michigan, Ann Arbor, Michigan 48109, USA
  • 7High Energy Accelerator Research Organization, KEK 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan

  • *For the CKMfitter group.

Phys. Rev. D 89, 033016 – Published 27 February, 2014

DOI: https://doi.org/10.1103/PhysRevD.89.033016

Abstract

We estimate, in a large class of scenarios, the sensitivity to new physics in Bd and Bs mixings achievable with 50ab1 of Belle II and 50fb1 of LHCb data. We find that current limits on new physics contributions in both Bd,s systems can be improved by a factor of 5 for all values of the CP-violating phases, corresponding to over a factor of 2 increase in the scale of new physics probed. Assuming the same suppressions by Cabbibo-Kobayashi-Maskawa matrix elements as those of the standard model box diagrams, the scale probed will be about 20 TeV for tree-level new physics contributions, and about 2 TeV for new physics arising at one loop. We also explore the future sensitivity to new physics in K mixing. Implications for generic new physics and for various specific scenarios, such as minimal flavor violation, light third-generation dominated flavor violation, or U(2) flavor models are studied.

Article Text

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