Measurement of the ratio of branching fractions B(B¯¯¯0→D∗+τ−ν¯τ))/B(B¯¯¯0→D∗+μ−ν¯μ)

R Aaij,Y Amhis,S Barsuk,M Borsato, O Kochebina, J Lefrancois,Yan Li,F Machefert, R Quagliani,P Robbe,M H Schune,M Teklishyn,A Vallier,B Viaud,G Wormser, Z Ajaltouni,M Baalouch,E Cogneras,O Deschamps,I El Rifai,G Gazzoni,M Grabalosa Gandara, P Henrard,M Hoballah, M Kozeiha,R Lefevre,J Maratas,S Monteil,V Niess, P Perret, L Beaucourt, M Chefdeville, D Decamp, N Deleage,Ph Ghez,J P Lees, J F Marchand,M N Minard, B Pietrzyk,Wei Qian,S Tjampens,V Tisserand,E Tournefier,S Akar, E Aslanides, John G Cogan,W Kanso, R Legac,O Leroy,G Mancinelli,Milo M K Martin, A Morda,J Serrano, A Tayduganov,A Tsaregorodtsev

PHYSICAL REVIEW LETTERS(2015)

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摘要
The branching fraction ratio R(D-*) = B((B) over bar (0) -> D-*(+)tau(-)(nu) over bar (tau))/B((B) over bar (0) -> D-*(+)mu(-)(nu) over bar (mu)) is measured using a sample of proton-proton collision data corresponding to 3.0 fb(-1) of integrated luminosity recorded by the LHCb experiment during 2011 and 2012. The tau lepton is identified in the decay mode tau(-) -> mu(-)(nu) over bar (mu)nu(tau). The semitauonic decay is sensitive to contributions from non-standard-model particles that preferentially couple to the third generation of fermions, in particular, Higgs-like charged scalars. A multidimensional fit to kinematic distributions of the candidate (B) over bar (0) decays gives R(D-*) = 0.336 +/- 0.027(stat) +/- 0.030(syst). This result, which is the first measurement of this quantity at a hadron collider, is 2.1 standard deviations larger than the value expected from lepton universality in the standard model.
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branching fractions<mmlmath,ratio,fractions<mmlmath xmlnsmml=http//wwww3org/1998/math/mathml
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