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Measurement of the $B^0 \to \pi^{-} \ell^{+} \nu$ and $B^{+} \to \pi^0 \ell^{+} \nu$ branching fractions and determination of $|V_{ub}|$ in $\upsilon_{4S} \to B \bar{B}$ events tagged by a fully reconstructed $B$ meson

B. Aubert,P. Tan,G. Simi,S. Playfer,T. Latham,G. Marchiori,A.M. Boyarski,R. Prepost,T. Held,A. V. Gritsan,R. H. Schindler,V. Eschenburg,E. Won,D. Monorchio,Y. Xie,M. Datta,F. Couderc,E. Torrence,C. C. Young,D. Best,T. Schalk,R. N. Cahn,M. C. Simani,P. Patterí,R. Godang,H. Nicholson,A. D. Bukin,R. Faccini,L. Del Buono,K. A. George,M. C. Hodgkinson,F. Ferroni,D. Lange,F. C. Porter,F. Muheim,David Norvil Brown,P. Roudeau,T. J. Harrison,C. Buchanan,W. S. Lockman,A. Lusiani,S. Rodier,M. Haire,S. Dasu,J. Reidy,D. Judd,A. Palano,A. K. Yarritu,S. Banerjee,N. Chevalier,G. Grosdidier,K. Goetzen,M. Weaver,C. Gatto,V. Poireau,K. Peters,M. Piccolo,M. Carpinelli,I. Ofte,J. P. Coleman,N. Arnaud,A. Gaidot,J. Biesiada,X. Chen,V. Lombardo,J. Strube,N.D. Qi,L. Roos,V. Lüth,H. Neal,J. C. Williams,G. Hamel de Monchenault,S. Pacetti,W. F. Mader,G. Wagner,S.R. Wagner,J. Olsen,S.L. Wu,A. Hauke,D. Boutigny,T. J. Orimoto,F. Forti,A. Rýd,J. H. von Wimmersperg-Toeller,C. Yéche,K.S. Chaisanguanthum,G. Lynch,K. R. Schubert,B. C. Shen,J. W. Berryhill,E. Paoloni,R. Kroeger,B. Viaud,T.B. Moore,X. Li,T. Vazquez Schroeder,S. Prell,Y. Karyotakis,R. Ter-Antonyan,C. Angelini,S. D. Foulkes,A. Chen,A. Mihályi,G. Cowan,E. Gabathuler,A. Satpathy,A. J. Hart,M. Gaspero,D. Bernard,J. R. Johnson,D. Kovalskyi,C. Hast,D. E. Hutchcroft,S. Ye,M. Battaglia,M. Rotondo,M. Wittgen,F. Galeazzi,M. L. Kocian,M. Pripstein,E. Graugés,G. Rizzo,A. Snyder,L. Lanceri,M. Pierini,J. Marks,W. Panduro Vazquez,M. Zito,R. Covarelli,M. John,J. E. Sundermann,A. Cunha,N. S. Knecht,J. Zhang,A. J. Edwards,M. Barrett,G. Rong,D. Bettoni,W.A. Wenzel,B. Bhuyan,H. M. Lacker,A. V. Telnov,Yu. I. Skovpen,S. J. Sekula,A. Calcaterra,J. Chauveau,S. Chen,G. Mancinelli,Q. K. Wong,J. P. Burke,E. Robutti,Y. P. Lau,C. Voena,U. Langenegger,A. D’Orazio,J. Kroseberg,C.K. Lae,R. Capra,N. Berger,D. D. Altenburg,M. Davier,J. E. Brau,W. Kozanecki,T. Adye,W. T. Meyer,G.W. London,P. David,B. Spaan,H. U. Flaecher,M. Negrini,P. E. Kutter,A. B. Breon,V. E. Özcan,C. J. Flacco,G. B. Mohanty,V. Sharma,G. Vasseur,J. Kadyk,B. Dahmes,A. M. Eisner,E. Chen,S. Curry,В. П. Дружинин,M. Bomben,D. E. Wagoner,J. Ocariz,L. Lista,G. Brandenburg,E.O. Olaiya,G. Cavoto,M. Krishnamurthy,G. De Nardo,F. X. Yumiceva,M. Rama,R. Cowan,J. J. Hollar,A. Zallo,R. Waldi,H. Kim,M. Morganti,R. Contri,S.E. Morgan,T. Çuhadar-Dönszelmann,S. Luitz,G. Vasileiadis,F. Gallo,F. Bucci,M. T. Graham,C.T. Potter,R.W. Kadel,W. D. Hulsbergen,P. S. Jackson,C. Bozzi,C. M. Brown,D. Del Re,A. M. Eichenbaum,U. Nauenberg,Ph Leruste,G. Schott,A. Salnikov,A. E. Blinov,N. R. Barlow,M. Chao,J. M. Izen,A. Santroni,A. J. Bevan,D. J. Bard,J. Wu,S. Fan,M. Bóna,E. P. Solodov,S. F. Ganzhur,F. Martínez-Vidal,R.G. Jacobsen,A. Buzzo,M. Lo Vetere, Saeed,M. P. Kelly,J. M. Bauer,A.M. Lutz,M. Perl,S. Schrenk,D. A. Roberts,E. Luppi,S. Jayatilleke,L. T. Kerth,Tetiana Berger-Hryn'ova,J. L. Harton,J. W. Gary,C. Cartaro,G. Wormser,S. Emery,S. Ricciardi,A. Jawahery,J.C. Chen,B. A. Schumm,C. M. Hawkes,M. Posocco,M. 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Azzolini,P. Wang,G. Graziani,J. Libby,S. Saremi,J. Cochran,A. Pompili,F. Safai Tehrani,G. S. Abrams,H. L. Lynch,W. Verkerke,S. Brunet,H. Koch, Мазур,K. Yi,J. Albert,I. J. Forster,P. J. Clark,S. Morganti,T. Glanzman,J. D. Richman,E. A. Kravchenko,В. Б. Голубев,F. Fabozzi,J. R. Fry,M. Bondioli,H. K. Hadavand,D. Su,L. Gladney,M. G. Wilson,G. P. Taylor,W. Bugg,G. Blaylock,R. J. Parry,D. Côté,C. H. Cheng,D. N. Brown,Yu. G. Kolomensky, Giorgi,M. Pioppí,D.C. Williams,R. Sacco,S. Rahatlou,A. Roodman,B. Cheng,R.S. Panvini,G. Kukartsev,A. W. Weidemann,H. L. Snoek, L. Zhang,P. F. Harrison,G. R. Bonneaud,A. E. Rubin,A. Kreisel,C.A. Heusch,D. Fortin,N. De Groot,Niels Anton van Bakel,J. Walsh,C. Dallapiccola,T. M. Hong,A. Lazzaro,A. Petzold,R. Bartoldus,C. Campagnari,Karsten Koeneke,M. Saleem,M. A. Baak,Ch De La Vaissière,L. Wilden,P. Elmer,M. Pappagallo,A. M. Rahimi,F. R. Wappler,E. J. Hill,T. Brandt,M. T. Ronan,U. Uwer,F. Palombo,D.H. Wright,J. R. Wilson,M.T. Naisbit,C. Touramanis,X. C. Lou,T. C. Petersen,S. Passaggio,D. Aston,J. Schubert,M. R. Monge,R. L. Flack,C. Roat,P. M. Patel,D. J. Payne,R. Eckmann,G. Piredda,N. Danielson,S. Schenk,Eric W. Gill,G. Nesom,U. Mallik,M. Lu,J. Hirschauer,S. Grancagnolo,H. B. Crawley,H. P. Paar,Y. Groysman,R. C. Field,C. Hearty,R. Kofler,G. Benelli,C. L. Davis,P. C. Bloom,O. Igonkina,K.E. Ford,L. Li Gioi,A. Soffer,K. K. Gan,V. Tisserand,M. Fritsch,M. Morii,J. Stelzer,T. Piatenko,H. Bulten,J. T. Boyd,M. R. Convery,D. Hufnagel,F. Blanc

Presented at(2005)

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摘要
The authors report preliminary measurements of the charmless exclusive semileptonic branching fractions of the B{sup 0} {yields} {pi}{sup -}{ell}{sup +}{nu} and B{sup +} {yields} {pi}{sup 0}{ell}{sup +}{nu} decays, based on 211 fb{sup -1} of data collected at the {Upsilon}(4S) resonance by the BABAR detector. In events in which the decay of one B meson to a hadronic final state is fully reconstructed, the semileptonic decay of the second B meson is identified by the detection of a charged lepton and a pion. They measure the partial branching fractions for B{sup 0} {yields} {pi}{sup -}{ell}{sup +}{nu} and B{sup +} {yields} {pi}{sup 0}{ell}{sup +}{nu} in three regions of the invariant mass squared of the lepton pair, and they obtain the total branching fractions {Beta}(B{sup 0} {yields} {pi}{sup -}{ell}{sup +}{nu}) = (1.14 {+-} 0.27{sub stat} {+-} 0.17{sub syst}) x 10{sup -4} and {Beta}(B{sup +} {yields} {pi}{sup 0}{ell}{sup +}{nu}) = (0.86 {+-} 0.22{sub stat} {+-} 0.11{sub syst}) x 10{sup -4}. Using isospin symmetry, they measure the combined total branching fraction {Beta}(B{sup 0} {yields} {pi}{sup -}{ell}{sup +}{nu}) = (1.28 {+-} 0.23{sub stat} {+-} 0.16{sub syst}) x 10{sup -4}. Theoretical predictions of the form-factor are used to determine the magnitude of the Cabibbo-Kobayashi-Maskawa matrix element |V{submore » ub}| = (3.7 {+-} 0.3{sub stat} {+-} 0.2{sub syst{sub -0.5FF}{sup +0.8}}) x 10{sup -3}, where the last uncertainty is due to the form-factor normalization.« less
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