Measurements of the semileptonic decays B¯→Dℓν¯ and B¯→D*ℓν¯ using a global fit to DXℓν¯ final states

Bernard Aubert,M. Bona,Y. Karyotakis,J. P. Lees,V. Poireau,E. Prencipe, X. Prudent,V. Tisserand,J. Garra Tico,E. Grauges,L. Lopezab,A. Palanoab,M. Pappagalloab,G. Eigen, B. Stugu,Lingfen Sun,G. S. Abrams,M. Battaglia, D. N. Brown,R. N. Cahn,R. G. Jacobsen,L. T. Kerth,G. Kolomensky, G. Lynch,I. L. Osipenkov,M. T. Ronan, K. Tackmann, T. Tanabe,C. M. Hawkes,N. Soni,A. T. Watson, H. Koch,T. Schroeder,D. Walker,D. J. Asgeirsson,B. G. Fulsom, C. Hearty,T. S. Mattison,J. McKenna,M. Barrett,A. Khan,V. Blinov,A. Bukin,A. Buzykaev,V. Druzhinin,V. Golubev,A. Onuchin,S. Serednyakov,Yu. Skovpen,E. Solodov,K. Todyshev,M. Bondioli,S. Curry, I. Eschrich,D. Kirkby,A. Lankford,P. Lund,M. Mandelkern,E. Martin,D. Stoker,S. Abachi,C. Buchanan,J. Gary,F. Liu,O. Long,B. Shen,G. Vitug,Z. Yasin, L. Zhang,V. Sharma,C. Campagnari,T. Hong, D. Kovalskyi,M. Mazur,J. Richman,T. Beck,A. Eisner,C. Flacco,C. Heusch, J. Kroseberg,W. Lockman,T. Schalk,B. Schumm, A. Seiden,L. Wang,M. Wilson, L. Winstrom, C. Cheng,D. 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PHYSICAL REVIEW D(2009)

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Abstract
Semileptonic (B) over bar decays to DXl (nu) over bar (l = e or mu) are selected by reconstructing D(0)l and D(+)l combinations from a sample of 230 x 10(6) Y(4S) --> B (B) over bar decays recorded with the BABAR detector at the PEP-II e(+)e(-) collider at SLAC. A global fit to these samples in a three-dimensional space of kinematic variables is used to determine the branching fractions B(B- --> D(0)l (nu) over bar = (2.34 +/- 0.03 +/- 0.13)% and B(B- --> D*(0)l (nu) over bar) = (5.40 +/- 0.02 +/- 0.21)% where the errors are statistical and systematic, respectively. The fit also determines form-factor parameters in a parametrization based on heavy quark effective theory, resulting in rho(2)(D) = 1.20 +/- 0.04 +/- 0.07 for (B) over bar --> Dl (nu) over bar and rho(2)(D*) = 1.22 +/- 0.02 +/- 0.07 for (B) over bar --> D*(0)l (nu) over bar. These values are used to obtain the product of the Cabibbo-Kobayashi-Maskawa matrix element |V-cb| times the form factor at the zero recoil point for both (B) over bar --> Dl (nu) over bar decays, G(1)|V-cb| = (43.1 +/- 0.8 +/- 2.3) x 10(-3), and for (B) over bar --> D*l (nu) over bar decays, F(1)|V-cb| = (35.9) +/- 0.2 +/- 1.2) x 10(-3).
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Key words
elementary particles,form factor,three dimensional
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