Determination of the form factors for the decay B0→D*-l+νl and of the CKM matrix element |Vcb|

B. Aubert,M. Bona, D. Boutigny,Y. Karyotakis,J. P. Lees,V. Poireau, X. Prudent,V. Tisserand,A. Zghiche,J. Garra Tico,E. Grauges,L. Lopez,A. Palano,G. Eigen,I. Ofte, B. Stugu, L. Sun,G. S. Abrams,M. Battaglia,D. N. Brown,J. Button-Shafer,R. N. Cahn,Y. Groysman,R. G. Jacobsen,J. A. Kadyk,L. T. Kerth,Yu. Kolomensky, G. Kukartsev,D. Lopes Pegna,G. Lynch,L. M. Mir, T. J. Orimoto,M. Pripstein,N. A. Roe,M. T. Ronan, K. Tackmann,W. A. Wenzel,P. del Amo Sanchez,C. M. Hawkes,A. T. Watson,T. Held,H. Koch,B. Lewandowski,M. Pelizaeus,T. Schroeder, M. Steinke,W. N. Cottingham,D. Walker,D. J. Asgeirsson,T. Cuhadar-Donszelmann,B. G. Fulsom,C. Hearty,N. S. Knecht,T. S. Mattison,J. A. McKenna,A. Khan,M. Saleem,L. Teodorescu,V. E. Blinov,A. D. Bukin,V. P. Druzhinin,V. B. Golubev,A. P. Onuchin,S. I. 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,S. Foulkes,J. Gary,F. Liu,O. Long,B. 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Luppi, M. Negrini,A. Petrella,L. Piemontese,E. Prencipe,V. Santoro, F. Anulli,R. Baldini-Ferroli,A. Calcaterra,R. de Sangro,G. Finocchiaro,S. Pacetti,P. Patteri,I. Peruzzi, M. Piccolo,M. Rama, A. Zallo,A. Buzzo,R. Contri,M. Lo Vetere,M. Macri,M. Monge, S. Passaggio, C. Patrignani,E. Robutti,A. Santroni, S. Tosi,K. Chaisanguanthum,M. Morii,J. Wu,R. Dubitzky,J. Marks,S. Schenk,U. Uwer, D. Bard,P. Dauncey,R. Flack, J. Nash,M. Nikolich,W. Vazquez,P. Behera,X. Chai,M. Charles,U. Mallik,N. Meyer,V. Ziegler,J. Cochran,H. Crawley, L. Dong,V. Eyges, W. Meyer, S. Prell,E. Rosenberg,A. Rubin, A. Gritsan,Z. Guo,C. Lae,A. Denig,M. Fritsch, G. Schott,N. Arnaud,J. Béquilleux, M. Davier,G. Grosdidier,A. Höcker,V. Lepeltier,F. Le Diberder,A. Lutz,S. Pruvot,S. Rodier,P. Roudeau,M. Schune,J. Serrano, V. Sordini, A. Stocchi,W. Wang,G. Wormser,D. Lange, D. Wright,C. Chavez,I. Forster,J. Fry, E. Gabathuler,R. Gamet,D. Hutchcroft,D. Payne,K. Schofield, C. Touramanis,A. Bevan,F. Di Lodovico,K. George,W. 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Purohit,J. Wilson,M. Allen,D. Aston, R. Bartoldus, P. Bechtle, N. Berger, R. Claus,J. Coleman,M. Convery, J. Dingfelder, J. Dorfan,G. Dubois-Felsmann, D. Dujmic,W. Dunwoodie, R. Field, T. Glanzman,S. Gowdy,M. Graham, P. Grenier,C. Hast,T. Hryn’ova, W. Innes,M. Kelsey,H. Kim, P. Kim,D. Leith,S. Li,S. Luitz, V. Luth,H. Lynch, D. MacFarlane,H. Marsiske,R. Messner, D. Muller,C. O’Grady,A. Perazzo,M. Perl,T. Pulliam, B. Ratcliff, A. Roodman, A. Salnikov,R. Schindler,J. Schwiening,A. Snyder,J. Stelzer, D. Su,M. Sullivan,K. Suzuki,S. Swain,J. Thompson,J. Va’vra,N. van Bakel, A. Wagner,M. Weaver,W. Wisniewski,M. Wittgen, D. Wright,A. Yarritu, K. Yi,C. Young, P. Burchat,A. Edwards,S. Majewski,B. Petersen,L. Wilden,S. Ahmed,M. Alam,R. Bula,J. Ernst,V. Jain,B. Pan,M. Saeed,F. Wappler,S. Zain,W. Bugg,M. Krishnamurthy, S. Spanier,R. Eckmann,J. Ritchie,A. Ruland,C. Schilling, R. Schwitters,J. Izen,X. Lou, S. Ye,F. Bianchi,F. Gallo,D. Gamba, M. Pelliccioni, M. Bomben,L. Bosisio,C. Cartaro, F. Cossutti,G. Della Ricca,L. Lanceri,L. Vitale, V. Azzolini,N. Lopez-March,F. Martinez-Vidal,D. Milanes, A. Oyanguren,J. Albert,Sw. Banerjee,B. Bhuyan,K. Hamano, R. Kowalewski,I. Nugent,J. Roney, R. Sobie,J. Back,P. Harrison,T. Latham,G. Mohanty,M. Pappagallo,H. Band,X. Chen, S. Dasu,K. Flood, J. Hollar,P. Kutter, Y. Pan,M. Pierini,R. Prepost, S. Wu,Z. Yu,H. Neal

PHYSICAL REVIEW D(2008)

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摘要
We present a combined measurement of the Cabibbo-Kobayashi-Maskawa matrix element vertical bar V-cb vertical bar and of the parameters rho(2), R-1(1), and R-2(1), which fully characterize the form factors for the B-0 -> D*(-)center dot(+)nu(center dot) decay in the framework of heavy-quark effective field theory. The results, based on a selected sample of about 52 800 B-0 -> D*(-)center dot(+)nu(center dot) decays, recorded by the BABAR detector, are rho(2)=1.157 +/- 0.094 +/- 0.027, R-1(1)=1.327 +/- 0.131 +/- 0.043, R-2(1)=0.859 +/- 0.077 +/- 0.021, and F(1)vertical bar V-cb vertical bar=(34.7 +/- 0.4 +/- 1.0)x10(-3). The first error is the statistical and the second is the systematic uncertainty. Combining these measurements with the previous BABAR measurement of the form factors, which employs a different fit technique on a partial sample of the data, we improve the statistical precision of the result, rho(2)=1.191 +/- 0.048 +/- 0.028, R-1(1)=1.429 +/- 0.061 +/- 0.044, R-2(1)=0.827 +/- 0.038 +/- 0.022, and F(1)vertical bar V-cb vertical bar=(34.4 +/- 0.3 +/- 1.1)x10(-3). Using lattice calculations for the axial form factor F(1), we extract vertical bar V-cb vertical bar=(37.4 +/- 0.3 +/- 1.2 +/-(1.2)(1.4))x10(-3), where the third error is due to the uncertainty in F(1). We also present a measurement of the exclusive branching fraction, B=(4.69 +/- 0.04 +/- 0.34)%.
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