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Analysis of the D+→K-π+e +νe decay channel

  • P. Del Amo Sanchez
  • , J. P. Lees
  • , V. Poireau
  • , E. Prencipe
  • , V. Tisserand
  • , J. Garra Tico
  • , E. Grauges
  • , M. Martinelli
  • , D. A. Milanes
  • , A. Palano
  • , M. Pappagallo
  • , G. Eigen
  • , B. Stugu
  • , L. Sun
  • , D. N. Brown
  • , L. T. Kerth
  • , Yu G. Kolomensky
  • , G. Lynch
  • , I. L. Osipenkov
  • , H. Koch
  • T. Schroeder, D. J. Asgeirsson, C. Hearty, T. S. Mattison, J. A. McKenna, A. Khan, A. Randle-Conde, V. E. Blinov, A. R. Buzykaev, V. P. Druzhinin, V. B. Golubev, E. A. Kravchenko, A. P. Onuchin, S. I. Serednyakov, Yu I. Skovpen, E. P. Solodov, K. Yu Todyshev, A. N. Yushkov, M. Bondioli, S. Curry, D. Kirkby, A. J. Lankford, M. Mandelkern, E. C. Martin, D. P. Stoker, H. Atmacan, J. W. Gary, F. Liu, O. Long, G. M. Vitug, C. Campagnari, T. M. Hong, D. Kovalskyi, J. D. Richman, C. West, A. M. Eisner, C. A. Heusch, J. Kroseberg, W. S. Lockman, A. J. Martinez, T. Schalk, B. A. Schumm, A. Seiden, L. O. Winstrom, C. H. Cheng, D. A. Doll, B. Echenard, D. G. Hitlin, P. Ongmongkolkul, F. C. Porter, A. Y. Rakitin, R. Andreassen, M. S. Dubrovin, G. Mancinelli, B. T. Meadows, M. D. Sokoloff, P. C. Bloom, W. T. Ford, A. Gaz, M. Nagel, U. Nauenberg, J. G. Smith, S. R. Wagner, R. Ayad, W. H. Toki, H. Jasper, T. M. Karbach, A. Petzold, B. Spaan, M. J. Kobel, K. R. Schubert, R. Schwierz, D. Bernard, M. Verderi, P. J. Clark, S. Playfer, J. E. Watson, M. Andreotti, D. Bettoni, C. Bozzi, R. Calabrese, A. Cecchi, G. Cibinetto, E. Fioravanti, P. Franchini, I. Garzia, E. Luppi, M. Munerato, M. Negrini, A. Petrella, L. Piemontese, R. Baldini-Ferroli, A. Calcaterra, R. De Sangro, G. Finocchiaro, M. Nicolaci, S. Pacetti, P. Patteri, I. M. Peruzzi, M. Piccolo, M. Rama, A. Zallo, R. Contri, E. Guido, M. Lo Vetere, M. R. Monge, S. Passaggio, C. Patrignani, E. Robutti, S. Tosi, B. Bhuyan, V. Prasad, C. L. Lee, M. Morii, A. Adametz, J. Marks, U. Uwer, F. U. Bernlochner, M. Ebert, H. M. Lacker, T. Lueck, A. Volk, P. D. Dauncey, M. Tibbetts, P. K. Behera, U. Mallik, C. Chen, J. Cochran, H. B. Crawley, L. Dong, W. T. Meyer, S. Prell, E. I. Rosenberg, A. E. Rubin, A. V. Gritsan, Z. J. Guo, N. Arnaud, M. Davier, D. Derkach, J. Firmino Da Costa, G. Grosdidier, F. Le Diberder, A. M. Lutz, B. Malaescu, A. Perez, P. Roudeau, M. H. Schune, J. Serrano, V. Sordini, A. Stocchi, L. Wang, G. Wormser, D. J. Lange, D. M. Wright, I. Bingham, C. A. Chavez, J. P. Coleman, J. R. Fry, E. Gabathuler, R. Gamet, D. E. Hutchcroft, D. J. Payne, C. Touramanis, A. J. Bevan, F. Di Lodovico, R. Sacco, M. Sigamani, G. Cowan, S. Paramesvaran, A. C. Wren, D. N. Brown, C. L. Davis, A. G. Denig, M. Fritsch, W. Gradl, A. Hafner, K. E. Alwyn, D. Bailey, R. J. Barlow, G. Jackson, G. D. Lafferty, J. Anderson, R. Cenci, A. Jawahery, D. A. Roberts, G. Simi, J. M. Tuggle, C. Dallapiccola, E. Salvati, R. Cowan, D. Dujmic, G. Sciolla, M. Zhao, D. Lindemann, P. M. Patel, S. H. Robertson, M. Schram, P. Biassoni, A. Lazzaro, V. Lombardo, F. Palombo, S. Stracka, L. Cremaldi, R. Godang, R. Kroeger, P. Sonnek, D. J. Summers, X. Nguyen, M. Simard, P. Taras, G. De Nardo, D. Monorchio, G. Onorato, C. Sciacca, G. Raven, H. L. Snoek, C. P. Jessop, K. J. Knoepfel, J. M. Losecco, W. F. Wang, L. A. Corwin, K. Honscheid, R. Kass, J. P. Morris, N. L. Blount, J. Brau, R. Frey, O. Igonkina, J. A. Kolb, R. Rahmat, N. B. Sinev, D. Strom, J. Strube, E. Torrence, G. Castelli, E. Feltresi, N. Gagliardi, M. Margoni, M. Morandin, M. Posocco, M. Rotondo, F. Simonetto, R. Stroili, E. Ben-Haim, G. R. Bonneaud, H. Briand, G. Calderini, J. Chauveau, O. Hamon, Ph Leruste, G. Marchiori, J. Ocariz, J. Prendki, S. Sitt, M. Biasini, E. Manoni, A. Rossi, C. Angelini, G. Batignani, S. Bettarini, M. Carpinelli, G. Casarosa, A. Cervelli, F. Forti, M. A. Giorgi, A. Lusiani, N. Neri, E. Paoloni, G. Rizzo, J. J. Walsh, D. Lopes Pegna, C. Lu, J. Olsen, A. J.S. Smith, A. V. Telnov, F. Anulli, E. Baracchini, G. Cavoto, R. Faccini, F. Ferrarotto, F. Ferroni, M. Gaspero, L. Li Gioi, M. A. Mazzoni, G. Piredda, F. Renga, T. Hartmann, T. Leddig, H. Schröder, R. Waldi, T. Adye, B. Franek, E. O. Olaiya, F. F. Wilson, S. Emery, G. Hamel De Monchenault, G. Vasseur, Ch Yèche, M. Zito, M. T. Allen, D. Aston, D. J. Bard, R. Bartoldus, J. F. Benitez, C. Cartaro, M. R. Convery, J. Dorfan, G. P. Dubois-Felsmann, W. Dunwoodie, R. C. Field, M. Franco Sevilla, B. G. Fulsom, A. M. Gabareen, M. T. Graham, P. Grenier, C. Hast, W. R. Innes, M. H. Kelsey, H. Kim, P. Kim, M. L. Kocian, D. W.G.S. Leith, S. Li, B. Lindquist, S. Luitz, V. Luth, H. L. Lynch, D. B. MacFarlane, H. Marsiske, D. R. Muller, H. Neal, S. Nelson, C. P. Grady, I. Ofte, M. Perl, T. Pulliam, B. N. Ratcliff, A. Roodman, A. A. Salnikov, V. Santoro, R. H. Schindler, J. Schwiening, A. Snyder, D. Su, M. K. Sullivan, S. Sun, K. Suzuki, J. M. Thompson, J. Va'Vra, A. P. Wagner, M. Weaver, W. J. Wisniewski, M. Wittgen, D. H. Wright, H. W. Wulsin, A. K. Yarritu, C. C. Young, V. Ziegler, X. R. Chen, W. Park, M. V. Purohit, R. M. White, J. R. Wilson, S. J. Sekula, M. Bellis, P. R. Burchat, A. J. Edwards, T. S. Miyashita, S. Ahmed, M. S. Alam, J. A. Ernst, B. Pan, M. A. Saeed, S. B. Zain, N. Guttman, A. Soffer, P. Lund, S. M. Spanier, R. Eckmann, J. L. Ritchie, A. M. Ruland, C. J. Schilling, R. F. Schwitters, B. C. Wray, J. M. Izen, X. C. Lou, F. Bianchi, D. Gamba, M. Pelliccioni, M. Bomben, L. Lanceri, L. Vitale, N. Lopez-March, F. Martinez-Vidal, A. Oyanguren, J. Albert, Sw Banerjee, H. H.F. Choi, K. Hamano, G. J. King, R. Kowalewski, M. J. Lewczuk, C. Lindsay, I. M. Nugent, J. M. Roney, R. J. Sobie, T. J. Gershon, P. F. Harrison, T. E. Latham, E. M.T. Puccio, H. R. Band, S. Dasu, K. T. Flood, Y. Pan, R. Prepost, C. O. Vuosalo, S. L. Wu
  • Université Savoie Mont Blanc
  • Facultat de Fisica
  • University of Barcelona
  • INFN Sezione di Bari
  • Dipartimento di Fisica
  • Università degli studi di Bari Aldo Moro
  • Institute of Physics
  • University of Bergen
  • University of California, Berkeley
  • Ruhr-University Bochum
  • University of British Columbia
  • Brunel University London
  • Budker Institute of Nuclear Physics of the Siberian Branch of the RAS
  • Long Beach VA and University of California
  • University of California, Riverside
  • University of California, Santa Barbara
  • University of California at Santa Cruz
  • California Institute of Technology
  • University of Cincinnati
  • University of Colorado Boulder
  • Cooperative Institute for Research in the Atmosphere
  • Temple University
  • Fakultät Physik
  • University of Dortmund
  • Institut für Kern- und Teilchenphysik
  • Technical University Dresden
  • University of Edinburgh
  • Sezione INFN di Ferrara
  • Dipartimento di Fisica
  • University of Ferrara
  • LNF-INFN
  • INFM CRS-SOFT
  • University of Perugia
  • Sezione di Genova
  • University of Genoa
  • Department of Biosciences and Bioengineering
  • Harvard University
  • University of Heidelberg
  • Institut für Physik
  • Humboldt-Universität zu Berlin
  • Imperial College London
  • University of Iowa
  • Iowa State University
  • Johns Hopkins University
  • Laboratoire de l'Accélérateur Linéaire
  • University of Rome
  • Lawrence Livermore National Laboratory
  • University of Liverpool
  • Queen Mary University of London
  • Royal Holloway University of London
  • University of Louisville
  • Institut für Kernphysik
  • Johannes Gutenberg University
  • University of Manchester
  • University of Maryland, College Park
  • UMass Amherst
  • Massachusetts Institute of Technology
  • McGill University
  • Sezione INFN di Milano
  • Dipartimento di Fisica
  • University of Milano
  • University of Mississippi
  • Universety of South Alabama
  • Universite de Montreal
  • INFN Sezione di Napoli
  • Dipartimento di Scienze Fisiche
  • University of Naples Federico II
  • Science Park 105
  • University of Notre Dame
  • The Ohio State University
  • University of Oregon
  • INFN
  • Dipartimento di Fisica
  • University of Padova
  • Universités Paris VI and VII
  • INFN Sezione di Perugia
  • Istituto Nazionale di Fisica Nucleare, Sezione di Pisa
  • Department of Physics
  • University of Pisa
  • Dipartimento di Scienze Biomediche
  • Scuola Normale Superiore di Pisa
  • Princeton University
  • Sezione di Roma
  • Dipartimento di Fisica
  • Universität Rostock
  • CCLRC Rutherford Appleton Laboratory
  • Universite Paris-Saclay
  • Stanford Linear Accelerator Center
  • University of South Carolina
  • Southern Methodist University
  • Stanford University
  • State University of New York Albany
  • School of Physics and Astronomy
  • Tel Aviv University
  • University of Tennessee
  • The University of Texas at Austin
  • University of Texas
  • INFN Sezione di Torino
  • University of Turin
  • INFN Sezione di Trieste
  • Dipartimento di Fisica
  • University of Trieste
  • University of Valencia
  • University of Victoria
  • Department of Physics
  • University of Warwick
  • University of Wisconsin-Madison

Research output: Contribution to journalArticlepeer-review

60 Citations (Scopus)

Abstract

Using 347.5fb-1 of data recorded by the BABAR detector at the PEP-II electron-positron collider, 244×103 signal events for the D +→K-π+e+νe decay channel are analyzed. This decay mode is dominated by the K̄(892)0 contribution. We determine the K̄*(892)0 parameters: mK(892)0=(895.4±0.2±0.2)MeV/c2, ΓK *(892)00=(46.5±0.3±0.2)MeV/c2, and the Blatt-Weisskopf parameter rBW=2.1±0.5±0.5(GeV/c) -1, where the first uncertainty comes from statistics and the second from systematic uncertainties. We also measure the parameters defining the corresponding hadronic form factors at q2=0 (rV=V(0)A 1(0)=1.463±0.017±0.031, r2=A 2(0)A1(0)=0.801±0.020±0.020) and the value of the axial-vector pole mass parametrizing the q2 variation of A1 and A2: mA=(2.63±0.10±0.13)GeV/c2. The S-wave fraction is equal to (5.79±0.16±0.15)%. Other signal components correspond to fractions below 1%. Using the D+→K -π+π+ channel as a normalization, we measure the D+ semileptonic branching fraction: B(D +→K-π+e+νe)= (4.00±0.03±0.04±0.09)×10-2, where the third uncertainty comes from external inputs. We then obtain the value of the hadronic form factor A1 at q2=0: A1(0)=0.6200±0. 0056±0.0065±0.0071. Fixing the P-wave parameters, we measure the phase of the S wave for several values of the Kπ mass. These results confirm those obtained with Kπ production at small momentum transfer in fixed target experiments.

Original languageEnglish
Article number072001
JournalPhysical Review D - Particles, Fields, Gravitation and Cosmology
Volume83
Issue number7
DOIs
Publication statusPublished - 1 Apr 2011

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