A search for lepton flavour violating decays of the Higgs boson in the µτ and eτ decay modes is presented. The search is based on a data set corresponding to an integrated luminosity of 35.9 fb −1 of proton-proton collisions collected with the CMS detector in 2016, at a centre-of-mass energy of 13 TeV. No significant excess over the standard model expectation is observed. The observed (expected) upper limits on the lepton flavour violating branching fractions of the Higgs boson are B(H → µτ ) < 0.25% (0.25%) and B(H → eτ ) < 0.61% (0.37%), at 95% confidence level. These results are used to derive upper limits on the off-diagonal µτ and eτ Yukawa couplings √ |Y µτ | 2 + |Y τ µ | 2 < 1.43×10 −3 and |Y eτ | 2 + |Y τ e | 2 < 2.26×10 −3 at 95% confidence level. The limits on the lepton flavour violating branching fractions of the Higgs boson and on the associated Yukawa couplings are the most stringent to date. The CMS collaboration 33
IntroductionThe discovery of the Higgs boson (H) at the CERN LHC [1][2][3] has stimulated further precision measurements of the properties of the new particle. A combined study of the 7 and 8 TeV data sets collected by the CMS and ATLAS collaborations shows consistency between the measured couplings of the Higgs boson and the standard model (SM) predictions [4]. However, the constraint on the branching fraction to non-SM decay modes derived from these measurements, B(non-SM) < 34% at 95% confidence level (CL), still allows for a significant contribution from exotic decays [4]. In this paper a search for lepton flavour violating (LFV) decays of the Higgs boson in the µτ and eτ channels is presented. These decays are forbidden in the SM but occur in many new physics scenarios. These include supersymmetric [5][6][7][8][9][10][11][12][13], composite Higgs [14,15], or Randall-Sundrum models [16][17][18], SM extensions with more than one Higgs boson doublet [19,20] or with flavour symmetries [21], and many other scenarios [22][23][24][25][26][27][28][29][30][31][32][33][34][35][36]. The presence of LFV Higgs boson couplings would allow τ → µ and τ → e to proceed via a virtual Higgs boson [37,38]. Consequently the experimental limits on rare τ lepton -1 -
JHEP06(2018)001decays, such as τ → eγ and τ → µγ [39], provide upper limits on B(H → µτ ) and B(H → eτ ) [40,41] of O(10%). Measurements of the electron and muon magnetic moments, and exclusion limits on the electric dipole moment of the electron also provide complementary constraints [42]. The LFV Higgs boson decay to µe is strongly constrained by the µ → eγ limit, B(H → eµ) < O(10 −9 ) [43].The CMS experiment published the first direct search for H → µτ [44], followed by searches for H → eτ and H → eµ decays [45], using proton-proton (pp) collision data corresponding to an integrated luminosity of 19.7 fb −1 at a centre-of-mass energy of 8 TeV.A small excess of data with respect to the SM background-only hypothesis at m H = 125 GeV was observed in the H → µτ channel, with a significance of 2.4 standard deviations (σ), and the bes...