Evidence for the B(0)-> p(p)over-barK*(0) and B(+)->eta(c)K*(+) decays and study of the decay dynamics of B meson decays into p(p)over-barh final states RID C-5223-2009 RID C-5719-2008 RID D-1055-2009

With a sample of 232x10(6) Upsilon(4S)-> B (B) over bar events collected with the BABAR detector, we study the decays of B mesons to p (p) over barh final states, where h=pi(+), K(S)(0), K*(0), or K*(+). We report evidence for the B(0)-> p (p) over barK(*0) decay, with a branching fraction (1.47 +/- 0.45(stat)+/- 0.40(syst))x10(-6), and for the B(+)->eta(c)K*(+) decay, with the branching fraction of B(B(+)->eta(c)K*(+))xB(eta(c)-> p (p) over bar)=(1.57(-0.45)(+0.56)(stat)(-0.36)(+0.46)(syst))x10(-6), and provide improved measurements of the branching fractions of the other modes of this type. We also report the measurements of the charge asymmetry consistent with zero in the B(+)-> p (p) over bar pi(+), B(0)-> p (p) over barK*(0), and B(+)-> p (p) over barK*(+) modes. No evidence is found for the pentaquark candidate Theta(+) in the mass range 1.52 to 1.55 GeV/c(2), decaying into pK(S)(0), or the glueball candidate f(J)(2220) in the mass range 2.2 < m(p (p) over bar)< 2.4 GeV/c(2), and branching fraction limits are established for both at the 10(-7) level.

Titolo:	Evidence for the B(0)-> p(p)over-barK(0) and B(+)->eta(c)K(+) decays and study of the decay dynamics of B meson decays into p(p)over-barh final states RID C-5223-2009 RID C-5719-2008 RID D-1055-2009
Autori:	Aubert B Bona M Boutigny D Karyotakis Y Lees JP Poireau V Prudent X Tisserand V Zghiche A Tico JG Grauges E Lopez L Palano A Eigen G Stugu B Sun L Abrams GS Battaglia M Brown DN Button Shafer J Cahn RN Groysman Y Jacobsen RG Kadyk JA Kerth LT Kolomensky YG Kukartsev G Pegna DL Lynch G Mir LM Orimoto TJ Ronan MT Tackmann K Wenzel WA Sanchez PD Hawkes CM Soni N Watson AT Held T Koch H Lewandowski B Pelizaeus M Schroeder T Steinke M Walker D Asgeirsson DJ Cuhadar Donszelmann T Fulsom BG Hearty C Mattison TS McKenna JA Khan A Saleem M Teodorescu L Blinov VE Bukin AD Druzhinin VP Golubev VB Onuchin AP Serednyakov SI Skovpen YI Solodov EP Todyshev KY Bondioli M Curry S Eschrich I Kirkby D Lankford AJ Lund P Mandelkern M Martin EC Stoker DP Abachi S Buchanan C Foulkes SD Gary JW Liu F Long O Shen BC Zhang L Paar HP Rahatlou S Sharma V Berryhill JW Campagnari C Cunha A Dahmes B Hong TM Kovalskyi D Richman JD Beck TW Eisner AM Flacco CJ Heusch CA Kroseberg J Lockman WS Schalk T Schumm BA Seiden A Wilson MG Winstrom LO Chen E Cheng CH Fang F Hitlin DG Narsky I Piatenko T Porter FC Andreassen R Mancinelli G Meadows BT Mishra K Sokoloff MD Blanc F Bloom PC Chen S Ford WT Hirschauer JF Kreisel A Nagel M Nauenberg U Olivas A Smith JG Ulmer KA Wagner SR Zhang J Gabareen AM Soffer A Toki WH Wilson RJ Winklmeier F Altenburg DD Feltresi E Hauke A Jasper H Merkel J Petzold A Spaan B Wacker K Klose V Kobel MJ Lacker HM Mader WF Nogowski R Schubert J Schubert KR Schwierz R Sundermann JE Volk A Bernard D Bonneaud GR Latour E Lombardo V Thiebaux C Verderi M Clark PJ Gradl W Muheim F Playfer S Robertson AI Xie Y Andreotti M Bettoni D Bozzi C Calabrese R Cecchi A Cibinetto G Franchini P Luppi E Negrini M Petrella A Piemontese L Prencipe E Santoro V Anulli F Baldini Ferroli R Calcaterra A de Sangro R Finocchiaro G Pacetti S Patteri P Peruzzi IM Piccolo M Rama M Zallo A Buzzo A Contri R Lo Vetere M Macri MM Monge MR Passaggio S Patrignani C Robutti E Santroni A Tosi S Chaisanguanthum KS Morii M Wu J Dubitzky RS Marks J Schenk S Uwer U Bard DJ Dauncey PD Flack RL Nash JA Vazquez WP Tibbetts M Behera PK Chai X Charles MJ Mallik U Ziegler V Cochran J Crawley HB Dong L Eyges V Meyer WT Prell S Rosenberg EI Rubin AE Gao YY Gritsan AV Guo ZJ Lae CK Denig AG Fritsch M Schott G Arnaud N Bequilleux J Davier M Grosdidier G Hocker A Lepeltier V Le Diberder F Lutz AM Pruvot S Rodier S Roudeau P Schune MH Serrano J Sordini V Stocchi A Wang WF Wormser G Lange DJ Wright DM Bingham I Chavez CA Forster IJ Fry JR Gabathuler E Gamet R Hutchcroft DE Payne DJ Schofield KC Touramanis C Bevan AJ George KA Di Lodovico F Menges W Sacco R Cowan G Flaecher HU Hopkins DA Paramesvaran S Salvatore F Wren AC Brown DN Davis CL Allison J Barlow NR Barlow RJ Chia YM Edgar CL Lafferty GD West TJ Yi JI Anderson J Chen C Jawahery A Roberts DA Simi G Tuggle JM Blaylock G Dallapiccola C Hertzbach SS Li X Moore TB Salvati E Saremi S Cowan R Dujmic D Fisher PH Koeneke K Sciolla G Sekula SJ Spitznagel M Taylor F Yamamoto RK Zhao M Zheng Y Mclachlin SE Patel PM Robertson SH Lazzaro A Palombo F Bauer JM Cremaldi L Eschenburg V Godang R Kroeger R Sanders DA Summers DJ Zhao HW Brunet S Cote D Simard M Taras P Viaud FB Nicholson H De Nardo G Fabozzi F Lista L Monorchio D Sciacca C Baak MA Raven G Snoek HL Jessop CP LoSecco JM Benelli G Corwin LA Honscheid K Kagan H Kass R Morris JP Rahimi AM Regensburger JJ Wong QK Blount NL Brau J Frey R Igonkina O Kolb JA Lu M Rahmat R Sinev NB Strom D Strube J Torrence E Gagliardi N Gaz A Margoni M Morandin M Pompili A Posocco M Rotondo M Simonetto F Stroili R Voci C Ben Haim E Briand H Calderini G Chauveau J David P Del Buono L de la Vaissiere C Hamon O Leruste P Malcles J Ocariz J Perez A Gladney L Biasini M Cervelli A Forti F Giorgi MA LUSIANI, Alberto Marchiori G Mazur MA Morganti M Neri N Paoloni E Rizzo G Walsh JJ Haire M Biesiada J Elmer P Lau YP Lu C Olsen J Smith AJS Telnov AV Baracchini E Bellini F Cavoto G D'Orazio A del Re D Di Marco E Faccini R Ferrarotto F Ferroni F Gaspero M Jackson PD Gioi LL Mazzoni MA Morganti S Piredda G Polci F Renga F Voena C Ebert M Hartmann T Schroder H Waldi R Adye T Castelli G Franek B Olaiya EO Ricciardi S Roethel W Wilson FF Aleksan R Emery S Escalier M Gaidot A Ganzhur SF de Monchenault GH Kozanecki W Vasseur G Yeche C Zito M Chen XR Liu H Park W Purohit MV Wilson JR Allen MT Aston D Bartoldus R Bechtle P Berger N Claus R Coleman JP Convery MR Dingfelder JC Dorfan J Dubois Felsmann GP Dunwoodie W Field RC Glanzman T Gowdy SJ Graham MT Grenier P Hast C Hryn'ova T Innes WR Kaminski J Kelsey MH Kim H Kim P Kocian ML Leith DWGS Li S Luitz S Luth V Lynch HL MacFarlane DB Marsiske H Messner R Muller DR O'Grady CP Ofte I Perazzo A Perl M Pulliam T Ratcliff BN Roodman A Salnikov AA Schindler RH Schwiening J Snyder A Stelzer J Su D Sullivan MK Suzuki K Swain SK Thompson JM Va'vra J van Bakel N Wagner AP Weaver M Wisniewski WJ Wittgen M Wright DH Yarritu AK Yi K Young CC Burchat PR Edwards AJ Majewski SA Petersen BA Wilden L Ahmed S Alam MS Bula R Ernst JA Jain V Pan B Saeed MA Wappler FR Zain SB Bugg W Krishnamurthy M Spanier SM Eckmann R Ritchie JL Ruland AM Schilling CJ Schwitters RF Izen JM Lou XC Ye S Bianchi F Gallo F Gamba D Pelliccioni M Bomben M Bosisio L Cartaro C Cossutti F Della Ricca G Lanceri L Vitale L Azzolini V Lopez March N Martinez Vidal F Milanes DA Oyanguren A Albert J Banerjee S Bhuyan B Hamano K Kowalewski R Nugent IM Roney JM Sobie RJ Harrison PF Ilic J Latham TE Mohanty GB Pappagallo M Band HR Chen X Dasu S Flood KT Hollar JJ Kutter PE Pan Y Pierini M Prepost R Wu SL Neal H. mostra contributor esterni nascondi contributor esterni
Data di pubblicazione:	2007
Rivista:	PHYSICAL REVIEW D, PARTICLES, FIELDS, GRAVITATION, AND COSMOLOGY
Abstract:	With a sample of 232x10(6) Upsilon(4S)-> B (B) over bar events collected with the BABAR detector, we study the decays of B mesons to p (p) over barh final states, where h=pi(+), K(S)(0), K(0), or K(+). We report evidence for the B(0)-> p (p) over barK(0) decay, with a branching fraction (1.47 +/- 0.45(stat)+/- 0.40(syst))x10(-6), and for the B(+)->eta(c)K(+) decay, with the branching fraction of B(B(+)->eta(c)K(+))xB(eta(c)-> p (p) over bar)=(1.57(-0.45)(+0.56)(stat)(-0.36)(+0.46)(syst))x10(-6), and provide improved measurements of the branching fractions of the other modes of this type. We also report the measurements of the charge asymmetry consistent with zero in the B(+)-> p (p) over bar pi(+), B(0)-> p (p) over barK(0), and B(+)-> p (p) over barK*(+) modes. No evidence is found for the pentaquark candidate Theta(+) in the mass range 1.52 to 1.55 GeV/c(2), decaying into pK(S)(0), or the glueball candidate f(J)(2220) in the mass range 2.2 < m(p (p) over bar)< 2.4 GeV/c(2), and branching fraction limits are established for both at the 10(-7) level.
Handle:	http://hdl.handle.net/11384/5273
Appare nelle tipologie:	1.1 Articolo in rivista

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