We present an investigation of the decays B-0 -> Lambda(+)(c)(p) over bar and B- -> Lambda(+)(c)(p) over bar pi(-) based on 383 X 10(6)Y(4S) -> B (B) over bar decays recorded with the BABAR detector. We measure the branching fractions of these decays; their ratio is B(B- -> Lambda(+)(c)(p) over bar pi(-))/B((B) over bar (0) -> Lambda(+)(c)(p) over bar) = 15.4 +/- 1.8 +/- 0.3. The B- -> Lambda(+)(c)(p) over bar pi(-) process exhibits an enhancement at the Lambda(+)(c)(p) over bar threshold and is a laboratory for searches for excited charm baryon states. We observe the resonant decays B- -> Sigma(c)(2455)(0)(p) over bar and B- -> Sigma(c)(2800)(0)(p) over bar but see no evidence for B- -> Sigma(c)(2520)(0)(p) over bar. This is the first observation of the decay B- -> Sigma(c)(2800)(0)(p) over bar; however, the mass of the observed excited Sigma(0)(c) state is (2846 +/- 8 +/- 10) MeV/c(2), which is somewhat inconsistent with previous measurements. Finally, we examine the angular distribution of the B- -> Sigma(c)(2455)(0)(p) over bar decays and measure the spin of the Sigma(c)(2455)(0) baryon to be 1/2, as predicted by the quark model.
Measurements of B((B)over-bar(0) -> Lambda(+)(c)(p)over-bar and B(B- -> Lambda(+)(c)(p)over-bar pi(-)) and studies of Lambda(+)(c)pi(-) resonances / Aubert, B; Bona, M; Karyotakis, Y; Lees, Jp; Poireau, V; Prencipe, E; Prudent, X; Tisserand, V; Tico, Jg; Grauges, E; Lopez, L; Palano, A; Pappagallo, M; Eigen, G; Stugu, B; Sun, L; Abrams, Gs; Battaglia, M; Brown, Dn; Cahn, Rn; Jacobsen, Rg; Kerth, Lt; Kolomensky, Yg; Kukartsev, G; Lynch, G; Osipenkov, Il; Ronan, Mt; Tackmann, K; Tanabe, T; Hawkes, Cm; Soni, N; Watson, At; Koch, H; Schroeder, T; Walker, D; Asgeirsson, Dj; CUHADAR DONSZELMANN, T; Fulsom, Bg; Hearty, C; Mattison, Ts; Mckenna, Ja; Barrett, M; Khan, A; Teodorescu, L; Blinov, Ve; Bukin, Ad; Buzykaev, Ar; 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; Gary, Jw; Liu, F; Long, O; Shen, Bc; Vitug, Gm; Yasin, Z; Zhang, L; Sharma, V; Campagnari, C; Hong, Tm; Kovalskyi, D; Mazur, Ma; Richman, Jd; Beck, Tw; Eisner, Am; Flacco, Cj; Heusch, Ca; Kroseberg, J; Lockman, Ws; Schalk, T; Schumm, Ba; Seiden, A; Wang, L; Wilson, Mg; Winstrom, Lo; Cheng, Ch; Doll, Da; Echenard, B; Fang, F; Hitlin, Dg; Narsky, I; Piatenko, T; Porter, Fc; Andreassen, R; Mancinelli, G; Meadows, Bt; Mishra, K; Sokoloff, Md; Blanc, F; Bloom, Pc; Ford, Wt; Gaz, A; Hirschauer, Jf; Kreisel, A; Nagel, M; Nauenberg, U; Smith, Jg; Ulmer, Ka; Wagner, Sr; Ayad, R; Soffer, A; Toki, Wh; Wilson, Rj; Altenburg, Dd; Feltresi, E; Hauke, A; Jasper, H; Karbach, M; Merkel, J; Petzold, A; Spaan, B; Wacker, K; Kobel, Mj; Mader, Wf; Nogowski, R; Schubert, Kr; Schwierz, R; Sundermann, Je; Volk, A; Bernard, D; Bonneaud, Gr; Latour, E; Thiebaux, C; Verderi, M; Clark, Pj; Gradl, W; Playfer, S; Watson, Je; Andreotti, M; Bettoni, D; Bozzi, C; Calabrese, R; Cecchi, A; Cibinetto, G; Franchini, P; Luppi, E; Negrini, M; Petrella, A; Piemontese, L; Santoro, V; 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; Dubitzky, Rs; Marks, J; Schenk, S; Uwer, U; Klose, V; Lacker, Hm; Bard, Dj; Dauncey, Pd; Nash, Ja; Vazquez, Wp; Tibbetts, M; Behera, Pk; Chai, X; Charles, Mj; Mallik, U; Cochran, J; Crawley, Hb; Dong, L; 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; D'Orazio, A; Davier, M; FERMINO DA COSTA, J; Grosdidier, G; Hocker, A; Lepeltier, V; LE DIBERDER, F; Lutz, Am; Pruvot, S; Roudeau, P; Schune, Mh; Serrano, J; Sordini, V; Stocchi, A; Wormser, G; Lange, Dj; Wright, Dm; Bingham, I; Burke, Jp; Chavez, Ca; Fry, Jr; Gabathuler, E; Gamet, R; Hutchcroft, De; Payne, Dj; Touramanis, C; Bevan, Aj; George, Ka; DI LODOVICO, F; 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Spanier, Sm; Wogsland, Bj; Eckmann, R; Ritchie, Jl; Ruland, Am; Schilling, Cj; Schwitters, Rf; Drummond, Bw; Izen, Jm; Lou, Xc; Bianchi, F; Gamba, D; Pelliccioni, M; Bomben, M; Bosisio, L; Cartaro, C; 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; Choi, Hhf; Hamano, K; Kowalewski, R; Lewczuk, Mj; Nugent, Im; Roney, Jm; Sobie, Rj; Gershon, Tj; Harrison, Pf; Ilic, J; Latham, Te; Mohanty, Gb; Band, Hr; Chen, X; Dasu, S; Flood, Kt; Pan, Y; Pierini, M; Prepost, R; Vuosalo, Co; Wu, Sl. - In: PHYSICAL REVIEW D, PARTICLES, FIELDS, GRAVITATION, AND COSMOLOGY. - ISSN 1550-7998. - 78:(2008). [10.1103/physrevd.78.112003]
Measurements of B((B)over-bar(0) -> Lambda(+)(c)(p)over-bar and B(B- -> Lambda(+)(c)(p)over-bar pi(-)) and studies of Lambda(+)(c)pi(-) resonances
AUBERT B; BONA M; KARYOTAKIS Y; LEES JP; POIREAU V; PRENCIPE E; PRUDENT X; TISSERAND V; TICO JG; GRAUGES E; LOPEZ L; PALANO A; PAPPAGALLO M; EIGEN G; STUGU B; SUN L; ABRAMS GS; BATTAGLIA M; BROWN DN; CAHN RN; JACOBSEN RG; KERTH LT; KOLOMENSKY YG; KUKARTSEV G; LYNCH G; OSIPENKOV IL; RONAN MT; TACKMANN K; TANABE T; HAWKES CM; SONI N; WATSON AT; KOCH H; SCHROEDER T; WALKER D; ASGEIRSSON DJ; CUHADAR DONSZELMANN T; FULSOM BG; HEARTY C; MATTISON TS; MCKENNA JA; BARRETT M; KHAN A; TEODORESCU L; BLINOV VE; BUKIN AD; BUZYKAEV AR; 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; GARY JW; LIU F; LONG O; SHEN BC; VITUG GM; YASIN Z; ZHANG L; SHARMA V; CAMPAGNARI C; HONG TM; KOVALSKYI D; MAZUR MA; RICHMAN JD; BECK TW; EISNER AM; FLACCO CJ; HEUSCH CA; KROSEBERG J; LOCKMAN WS; SCHALK T; SCHUMM BA; SEIDEN A; WANG L; WILSON MG; WINSTROM LO; CHENG CH; DOLL DA; ECHENARD B; FANG F; HITLIN DG; NARSKY I; PIATENKO T; PORTER FC; ANDREASSEN R; MANCINELLI G; MEADOWS BT; MISHRA K; SOKOLOFF MD; BLANC F; BLOOM PC; FORD WT; GAZ A; HIRSCHAUER JF; KREISEL A; NAGEL M; NAUENBERG U; SMITH JG; ULMER KA; WAGNER SR; AYAD R; SOFFER A; TOKI WH; WILSON RJ; ALTENBURG DD; FELTRESI E; HAUKE A; JASPER H; KARBACH M; MERKEL J; PETZOLD A; SPAAN B; WACKER K; KOBEL MJ; MADER WF; NOGOWSKI R; SCHUBERT KR; SCHWIERZ R; SUNDERMANN JE; VOLK A; BERNARD D; BONNEAUD GR; LATOUR E; THIEBAUX C; VERDERI M; CLARK PJ; GRADL W; PLAYFER S; WATSON JE; ANDREOTTI M; BETTONI D; BOZZI C; CALABRESE R; CECCHI A; CIBINETTO G; FRANCHINI P; LUPPI E; NEGRINI M; PETRELLA A; PIEMONTESE L; SANTORO V; 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; DUBITZKY RS; MARKS J; SCHENK S; UWER U; KLOSE V; LACKER HM; BARD DJ; DAUNCEY PD; NASH JA; VAZQUEZ WP; TIBBETTS M; BEHERA PK; CHAI X; CHARLES MJ; MALLIK U; COCHRAN J; CRAWLEY HB; DONG L; 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; D'ORAZIO A; DAVIER M; FERMINO DA COSTA J; GROSDIDIER G; HOCKER A; LEPELTIER V; LE DIBERDER F; LUTZ AM; PRUVOT S; ROUDEAU P; SCHUNE MH; SERRANO J; SORDINI V; STOCCHI A; WORMSER G; LANGE DJ; WRIGHT DM; BINGHAM I; BURKE JP; CHAVEZ CA; FRY JR; GABATHULER E; GAMET R; HUTCHCROFT DE; PAYNE DJ; TOURAMANIS C; BEVAN AJ; GEORGE KA; DI LODOVICO F; SACCO R; SIGAMANI M; COWAN G; FLAECHER HU; HOPKINS DA; PARAMESVARAN S; SALVATORE F; WREN AC; BROWN DN; DAVIS CL; ALWYN KE; 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; DALLAPICCOLA C; HERTZBACH SS; LI X; SALVATI E; SAREMI S; COWAN R; DUJMIC D; FISHER PH; KOENEKE K; SCIOLLA G; SPITZNAGEL M; TAYLOR F; YAMAMOTO RK; ZHAO M; MCLACHLIN SE; PATEL PM; ROBERTSON SH; LAZZARO A; LOMBARDO V; PALOMBO F; BAUER JM; CREMALDI L; ESCHENBURG V; GODANG R; KROEGER R; SANDERS DA; SUMMERS DJ; ZHAO HW; SIMARD M; TARAS P; VIAUD FB; NICHOLSON H; DE NARDO G; LISTA L; MONORCHIO D; ONORATO G; SCIACCA C; BAAK MA; RAVEN G; SNOEK HL; JESSOP CP; KNOEPFEL KJ; LOSECCO JM; WANG WF; BENELLI G; CORWIN LA; HONSCHEID K; KAGAN H; KASS R; MORRIS JP; RAHIMI AM; REGENSBURGER JJ; SEKULA SJ; WONG QK; BLOUNT NL; BRAU J; FREY R; IGONKINA O; KOLB JA; LU M; RAHMAT R; SINEV NB; STROM D; STRUBE J; TORRENCE E; CASTELLI G; GAGLIARDI N; MARGONI M; MORANDIN M; POSOCCO M; ROTONDO M; SIMONETTO F; STROILI R; VOCI C; SANCHEZ PD; BEN HAIM E; BRIAND H; CALDERINI G; CHAUVEAU J; DAVID P; DEL BUONO L; HAMON O; LERUSTE P; OCARIZ J; PEREZ A; PRENDKI J; GLADNEY L; BIASINI M; COVARELLI R; MANONI E; ANGELINI C; BATIGNANI G; BETTARINI S; CARPINELLI M; CERVELLI A; FORTI F; GIORGI MA; LUSIANI A; MARCHIORI G; MORGANTI M; NERI N; PAOLONI E; RIZZO G; WALSH JJ; BIESIADA J; LOPES PEGNA D; LU C; OLSEN J; SMITH AJS; TELNOV AV; ANULLI F; BARACCHINI E; CAVOTO, Gianluca ;DEL RE, Daniele ;DI MARCO E; FACCINI, Riccardo ;FERRAROTTO F; FERRONI, Fernando ;GASPERO, Mario ;JACKSON PD; LI GIOI L; MAZZONI MA; MORGANTI S; PIREDDA G; POLCI F; RENGA F; VOENA C ;EBERT M; HARTMANN T; SCHRODER H; WALDI R; ADYE T; FRANEK B; OLAIYA EO; ROETHEL W; WILSON FF; EMERY S; ESCALIER M; ESTEVE L; GAIDOT A; GANZHUR SF; HAMEL DE MONCHENAULT G; KOZANECKI W; VASSEUR G; YECHE C; ZITO M; CHEN XR; LIU H; PARK W; PUROHIT MV; WHITE RM; WILSON JR; ALLEN MT; ASTON D; BARTOLDUS R; BECHTLE P; BENITEZ JF; CENCI R; COLEMAN JP; CONVERY MR; DINGFELDER JC; DORFAN J; DUBOIS FELSMANN GP; DUNWOODIE W; FIELD RC; GABAREEN AM; GOWDY SJ; GRAHAM MT; GRENIER P; HAST C; INNES WR; KAMINSKI J; KELSEY MH; KIM H; KIM P; KOCIAN ML; LEITH DWGS; LI S; LINDQUIST B; LUITZ S; LUTH V; LYNCH HL; MACFARLANE DB; MARSISKE H; MESSNER R; MULLER DR; NEAL H; NELSON S; O'GRADY CP; OFTE I; PERAZZO A; PERL M; RATCLIFF BN; ROODMAN A; SALNIKOV AA; SCHINDLER RH; SCHWIENING J; SNYDER A; SU D; SULLIVAN MK; SUZUKI K; SWAIN SK; THOMPSON JM; VA'VRA J; WAGNER AP; WEAVER M; WEST CA; WISNIEWSKI WJ; WITTGEN M; WRIGHT DH; WULSIN HW; YARRITU AK; YI K; YOUNG CC; ZIEGLER V; BURCHAT PR; EDWARDS AJ; MAJEWSKI SA; MIYASHITA TS; PETERSEN BA; WILDEN L; AHMED S; ALAM MS; BULA R; ERNST JA; PAN B; SAEED MA; ZAIN SB; SPANIER SM; WOGSLAND BJ; ECKMANN R; RITCHIE JL; RULAND AM; SCHILLING CJ; SCHWITTERS RF; DRUMMOND BW; IZEN JM; LOU XC; BIANCHI F; GAMBA D; PELLICCIONI M; BOMBEN M; BOSISIO L; CARTARO C; 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; CHOI HHF; HAMANO K; KOWALEWSKI R; LEWCZUK MJ; NUGENT IM; RONEY JM; SOBIE RJ; GERSHON TJ; HARRISON PF; ILIC J; LATHAM TE; MOHANTY GB; BAND HR; CHEN X; DASU S; FLOOD KT; PAN Y; PIERINI M; PREPOST R; VUOSALO CO; WU SL
2008
Abstract
We present an investigation of the decays B-0 -> Lambda(+)(c)(p) over bar and B- -> Lambda(+)(c)(p) over bar pi(-) based on 383 X 10(6)Y(4S) -> B (B) over bar decays recorded with the BABAR detector. We measure the branching fractions of these decays; their ratio is B(B- -> Lambda(+)(c)(p) over bar pi(-))/B((B) over bar (0) -> Lambda(+)(c)(p) over bar) = 15.4 +/- 1.8 +/- 0.3. The B- -> Lambda(+)(c)(p) over bar pi(-) process exhibits an enhancement at the Lambda(+)(c)(p) over bar threshold and is a laboratory for searches for excited charm baryon states. We observe the resonant decays B- -> Sigma(c)(2455)(0)(p) over bar and B- -> Sigma(c)(2800)(0)(p) over bar but see no evidence for B- -> Sigma(c)(2520)(0)(p) over bar. This is the first observation of the decay B- -> Sigma(c)(2800)(0)(p) over bar; however, the mass of the observed excited Sigma(0)(c) state is (2846 +/- 8 +/- 10) MeV/c(2), which is somewhat inconsistent with previous measurements. Finally, we examine the angular distribution of the B- -> Sigma(c)(2455)(0)(p) over bar decays and measure the spin of the Sigma(c)(2455)(0) baryon to be 1/2, as predicted by the quark model.
Citazione
Measurements of B((B)over-bar(0) -> Lambda(+)(c)(p)over-bar and B(B- -> Lambda(+)(c)(p)over-bar pi(-)) and studies of Lambda(+)(c)pi(-) resonances / Aubert, B; Bona, M; Karyotakis, Y; Lees, Jp; Poireau, V; Prencipe, E; Prudent, X; Tisserand, V; Tico, Jg; Grauges, E; Lopez, L; Palano, A; Pappagallo, M; Eigen, G; Stugu, B; Sun, L; Abrams, Gs; Battaglia, M; Brown, Dn; Cahn, Rn; Jacobsen, Rg; Kerth, Lt; Kolomensky, Yg; Kukartsev, G; Lynch, G; Osipenkov, Il; Ronan, Mt; Tackmann, K; Tanabe, T; Hawkes, Cm; Soni, N; Watson, At; Koch, H; Schroeder, T; Walker, D; Asgeirsson, Dj; CUHADAR DONSZELMANN, T; Fulsom, Bg; Hearty, C; Mattison, Ts; Mckenna, Ja; Barrett, M; Khan, A; Teodorescu, L; Blinov, Ve; Bukin, Ad; Buzykaev, Ar; 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; Gary, Jw; Liu, F; Long, O; Shen, Bc; Vitug, Gm; Yasin, Z; Zhang, L; Sharma, V; Campagnari, C; Hong, Tm; Kovalskyi, D; Mazur, Ma; Richman, Jd; Beck, Tw; Eisner, Am; Flacco, Cj; Heusch, Ca; Kroseberg, J; Lockman, Ws; Schalk, T; Schumm, Ba; Seiden, A; Wang, L; Wilson, Mg; Winstrom, Lo; Cheng, Ch; Doll, Da; Echenard, B; Fang, F; Hitlin, Dg; Narsky, I; Piatenko, T; Porter, Fc; Andreassen, R; Mancinelli, G; Meadows, Bt; Mishra, K; Sokoloff, Md; Blanc, F; Bloom, Pc; Ford, Wt; Gaz, A; Hirschauer, Jf; Kreisel, A; Nagel, M; Nauenberg, U; Smith, Jg; Ulmer, Ka; Wagner, Sr; Ayad, R; Soffer, A; Toki, Wh; Wilson, Rj; Altenburg, Dd; Feltresi, E; Hauke, A; Jasper, H; Karbach, M; Merkel, J; Petzold, A; Spaan, B; Wacker, K; Kobel, Mj; Mader, Wf; Nogowski, R; Schubert, Kr; Schwierz, R; Sundermann, Je; Volk, A; Bernard, D; Bonneaud, Gr; Latour, E; Thiebaux, C; Verderi, M; Clark, Pj; Gradl, W; Playfer, S; Watson, Je; Andreotti, M; Bettoni, D; Bozzi, C; Calabrese, R; Cecchi, A; Cibinetto, G; Franchini, P; Luppi, E; Negrini, M; Petrella, A; Piemontese, L; 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[10.1103/physrevd.78.112003]
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Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande. La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.