We search for a charged partner of the X(3872) in the decay B-->X-K, X--->J/psipi(-)pi(0), using 234x10(6) B (B) over bar events collected at the Y(4S) resonance with the BABAR detector at the PEP-II e(+)e(-) asymmetric-energy storage ring. The resulting product branching fraction upper limits are B(B-0-->X-K+,X--->J/psipi(-)pi(0))<5.4x10(-6) and B(B--->X-(K) over bar (0),X--->J/psipi(-)pi(0))<22x10(-6) at the 90% confidence level.
Search for a charged partner of the X(3872) in the B meson decay B -> X-K, X--> J/psi pi(-)pi(0) / Aubert, B; Barate, R; Boutigny, D; Couderc, F; Karyotakis, Y; Lees, Jp; Poireau, V; Tisserand, V; Zghiche, A; GRAUGES POUS, E; Palano, A; Pompili, A; Chen, Jc; Qi, Nd; Rong, G; Wang, P; Zhu, Ys; Eigen, G; Ofte, I; Stugu, B; Abrams, Gs; Borgland, Aw; Breon, Ab; Brown, Dn; BUTTON SHAFER, J; Cahn, Rn; Charles, E; Day, Ct; Gill, Ms; Gritsan, Av; Groysman, Y; Jacobsen, Rg; Kadel, Rw; Kadyk, J; Kerth, Lt; Kolomensky, Yg; Kukartsev, G; Lynch, G; Mir, Lm; Oddone, Pj; Orimoto, Tj; Pripstein, M; Roe, Na; Ronan, Mt; Wenzel, Wa; Barrett, M; Ford, Ke; Harrison, Tj; Hart, Aj; Hawkes, Cm; Morgan, Se; Watson, At; Fritsch, M; Goetzen, K; Held, T; Koch, H; Lewandowski, B; Pelizaeus, M; Schroeder, T; Steinke, M; Boyd, Jt; Chevalier, N; Cottingham, Wn; Kelly, Mp; Latham, Te; Wilson, Ff; CUHADAR DONSZELMANN, T; Hearty, C; Knecht, Ns; Mattison, Ts; Mckenna, Ja; Thiessen, D; Khan, A; Kyberd, P; Teodorescu, L; Blinov, Ae; 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Lanceri, L; Poropat, P; Vitale, L; Vuagnin, G; MARTINEZ VIDAL, F; Panvini, Rs; Banerjee, S; Bhuyan, B; Brown, Cm; Fortin, D; Jackson, Pd; Kowalewski, R; Roney, Jm; Sobie, Rj; Back, Jj; Harrison, Pf; Mohanty, Gb; Band, Hr; Chen, X; Cheng, B; Dasu, S; Datta, M; Eichenbaum, Am; Flood, Kt; Graham, M; Hollar, Jj; Johnson, Jr; Kutter, Pe; Li, H; Liu, R; Mihalyi, A; Pan, Y; Prepost, R; Tan, P; VON WIMMERSPERG TOELLER, Jh; Wu, J; Wu, Sl; Yu, Z; Greene, Mg; Neal, H.. - In: PHYSICAL REVIEW D, PARTICLES, FIELDS, GRAVITATION, AND COSMOLOGY. - ISSN 1550-7998. - 71:(2005). [10.1103/physrevd.71.031501]
Search for a charged partner of the X(3872) in the B meson decay B -> X-K, X--> J/psi pi(-)pi(0)
AUBERT B; BARATE R; BOUTIGNY D; COUDERC F; KARYOTAKIS Y; LEES JP; POIREAU V; TISSERAND V; ZGHICHE A; GRAUGES POUS E; PALANO A; POMPILI A; CHEN JC; QI ND; RONG G; WANG P; ZHU YS; EIGEN G; OFTE I; STUGU B; ABRAMS GS; BORGLAND AW; BREON AB; BROWN DN; BUTTON SHAFER J; CAHN RN; CHARLES E; DAY CT; GILL MS; GRITSAN AV; GROYSMAN Y; JACOBSEN RG; KADEL RW; KADYK J; KERTH LT; KOLOMENSKY YG; KUKARTSEV G; LYNCH G; MIR LM; ODDONE PJ; ORIMOTO TJ; PRIPSTEIN M; ROE NA; RONAN MT; WENZEL WA; BARRETT M; FORD KE; HARRISON TJ; HART AJ; HAWKES CM; MORGAN SE; WATSON AT; FRITSCH M; GOETZEN K; HELD T; KOCH H; LEWANDOWSKI B; PELIZAEUS M; SCHROEDER T; STEINKE M; BOYD JT; CHEVALIER N; COTTINGHAM WN; KELLY MP; LATHAM TE; WILSON FF; CUHADAR DONSZELMANN T; HEARTY C; KNECHT NS; MATTISON TS; MCKENNA JA; THIESSEN D; KHAN A; KYBERD P; TEODORESCU L; BLINOV AE; BLINOV VE; DRUZHININ VP; GOLUBEV VB; IVANCHENKO VN; KRAVCHENKO EA; ONUCHIN AP; SEREDNYAKOV SI; SKOVPEN YI; SOLODOV EP; YUSHKOV AN; BEST D; BRUINSMA M; CHAO M; ESCHRICH I; KIRKBY D; LANKFORD AJ; MANDELKERN M; MOMMSEN RK; ROETHEL W; STOKER DP; BUCHANAN C; HARTFIEL BL; WEINSTEIN AJR; FOULKES SD; GARY JW; LONG O; SHEN BC; WANG K; DEL RE, Daniele ;HADAVAND HK; HILL EJ; MACFARLANE DB; PAAR HP; RAHATLOU, SHAHRAM ;SHARMA V; CUNHA JA; BERRYHILL JW; CAMPAGNARI C; DAHMES B; HONG TM; LU A; MAZUR MA; RICHMAN JD; VERKERKE W; BECK TW; EISNER AM; HEUSCH CA; KROSEBERG J; LOCKMAN WS; NESOM G; SCHALK T; SCHUMM BA; SEIDEN A; SPRADLIN P; WILLIAMS DC; WILSON MG; ALBERT J; CHEN E; DUBOIS FELSMANN GP; DVORETSKII A; HITLIN DG; NARSKY I; PIATENKO T; PORTER FC; RYD A; SAMUEL A; YANG S; JAYATILLEKE S; MANCINELLI G; MEADOWS BT; SOKOLOFF MD; BLANC F; BLOOM P; CHEN S; FORD WT; NAUENBERG U; OLIVAS A; RANKIN P; RUDDICK WO; SMITH JG; ULMER KA; ZHANG J; ZHANG L; CHEN A; ECKHART EA; HARTON JL; SOFFER A; TOKI WH; WILSON RJ; WINKLMEIER F; ZENG Q; SPAAN B; ALTENBURG D; BRANDT T; BROSE J; DICKOPP M; FELTRESI E; HAUKE A; LACKER HM; NOGOWSKI R; OTTO S; PETZOLD A; SCHUBERT J; SCHUBERT KR; SCHWIERZ R; SUNDERMANN JE; BERNARD D; BONNEAUD GR; GRENIER P; SCHRENK S; THIEBAUX C; VASILEIADIS G; VERDERI M; BARD DJ; CLARK PJ; MUHEIM F; PLAYFER S; XIE Y; ANDREOTTI M; AZZOLINI V; BETTONI D; BOZZI C; CALABRESE R; CIBINETTO G; LUPPI E; NEGRINI M; PIEMONTESE L; SARTI, ALESSIO ;TREADWELL E; ANULLI F; BALDINI FERROLI R; CALCATERRA A; DE SANGRO R; FINOCCHIARO G; PATTERI P; PERUZZI IM; PICCOLO M; ZALLO A; BUZZO A; CAPRA R; CONTRI R; CROSETTI G; LO VETERE M; MACRI M; MONGE MR; PASSAGGIO S; PATRIGNANI C; ROBUTTI E; SANTRONI A; TOSI S; BAILEY S; BRANDENBURG G; CHAISANGUANTHUM KS; MORII M; WON E; DUBITZKY RS; LANGENEGGER U; MARKS J; UWER U; BHIMJI W; BOWERMAN DA; DAUNCEY PD; EGEDE U; GAILLARD JR; MORTON GW; NASH JA; NIKOLICH MB; TAYLOR GP; CHARLES MJ; GRENIER GJ; MALLIK U; COCHRAN J; CRAWLEY HB; LAMSA J; MEYER WT; PRELL S; ROSENBERG EI; RUBIN AE; YI J; BIASINI M; COVARELLI R; PIOPPI M; ARNAUD N; DAVIER M; GIROUX X; GROSDIDIER G; HOCKER A; LE DIBERDER F; LEPELTIER V; LUTZ AM; PETERSEN TC; PLASZCZYNSKI S; SCHUNE MH; WORMSER G; CHENG CH; LANGE DJ; SIMANI MC; WRIGHT DM; BEVAN AJ; CHAVEZ CA; COLEMAN JP; FORSTER IJ; FRY JR; GABATHULER E; GAMET R; HUTCHCROFT DE; PARRY RJ; PAYNE DJ; TOURAMANIS C; CORMACK CM; DI LODOVICO F; BROWN CL; COWAN G; FLACK RL; FLAECHER HU; GREEN MG; JACKSON PS; MCMAHON TR; RICCIARDI S; SALVATORE F; WINTER MA; BROWN D; DAVIS CL; ALLISON J; BARLOW NR; BARLOW RJ; HODGKINSON MC; LAFFERTY GD; WILLIAMS JC; CHEN C; FARBIN A; HULSBERGEN WD; JAWAHERY A; KOVALSKYI D; LAE CK; LILLARD V; ROBERTS DA; BLAYLOCK G; DALLAPICCOLA C; HERTZBACH SS; KOFLER R; KOPTCHEV VB; MOORE TB; SAREMI S; STAENGLE H; WILLOCQ S; COWAN R; KOENEKE K; SCIOLLA G; SEKULA SJ; TAYLOR F; YAMAMOTO RK; PATEL PM; ROBERTSON SH; LAZZARO A; LOMBARDO V; PALOMBO F; BAUER JM; CREMALDI L; ESCHENBURG V; GODANG R; KROEGER R; REIDY J; SANDERS DA; SUMMERS DJ; ZHAO HW; BRUNET S; COTE D; TARAS P; NICHOLSON H; CAVALLO N; FABOZZI F; GATTO C; LISTA L; MONORCHIO D; PAOLUCCI P; PICCOLO D; SCIACCA C; BAAK M; BULTEN H; RAVEN G; SNOEK HL; WILDEN L; JESSOP CP; LOSECCO JM; ALLMENDINGER T; BENELLI G; GAN KK; HONSCHEID K; HUFNAGEL D; KAGAN H; KASS R; PULLIAM T; RAHIMI AM; TER ANTONYAN R; WONG QK; BRAU J; FREY R; IGONKINA O; LU M; POTTER CT; SINEV NB; STROM D; TORRENCE E; COLECCHIA F; DORIGO A; GALEAZZI F; MARGONI M; MORANDIN M; POSOCCO M; ROTONDO M; SIMONETTO F; STROILI R; VOCI C; BENAYOUN M; BRIAND H; CHAUVEAU J; DAVID P; DE LA VAISSIERE C; DEL BUONO L; HAMON O; JOHN MJJ; LERUSTE P; MALCLES J; OCARIZ J; ROOS L; THERIN G; BEHERA PK; GLADNEY L; GUO QH; PANETTA J; ANGELINI C; BATIGNANI G; BETTARINI S; BONDIOLI M; BUCCI F; CALDERINI G; CARPINELLI M; FORTI F; GIORGI MA; LUSIANI A; MARCHIORI G; MORGANTI M; NERI N; PAOLONI E; RAMA M; RIZZO G; SIMI G; WALSH J; HAIRE M; JUDD D; PAICK K; WAGONER DE; DANIELSON N; ELMER P; LAU YP; LU C; MIFTAKOV V; OLSEN J; SMITH AJS; TELNOV AV; BELLINI, Fabio ;CAVOTO, Gianluca ;D'ORAZIO A; DI MARCO E; FACCINI, Riccardo ;FERRAROTTO F; FERRONI, Fernando ;GASPERO, Mario ;GIOI LL; MAZZONI MA; MORGANTI S; PIERINI M; PIREDDA G; POLCI F; TEHRANI FS; VOENA C ;CHRIST S; SCHRODER H; WAGNER G; WALDI R; ADYE T; DE GROOT N; FRANEK B; GOPAL GP; OLAIYA EO; ALEKSAN R; EMERY S; GAIDOT A; GANZHUR SF; GIRAUD PF; DE MONCHENAULT GH; KOZANECKI W; LEGENDRE M; LONDON GW; MAYER B; SCHOTT G; VASSEUR G; YECHE C; ZITO M; PUROHIT MV; WEIDEMANN AW; WILSON JR; YUMICEVA FX; ABE T; ALLEN M; ASTON D; BARTOLDUS R; BERGER N; BOYARSKI AM; BUCHMUELLER OL; CLAUS R; CONVERY MR; CRISTINZIANI M; DE NARDO G; DINGFELDER JC; DONG D; DORFAN J; DUJMIC D; DUNWOODIE W; FAN S; FIELD RC; GLANZMAN T; GOWDY SJ; HADIG T; HALYO V; HAST C; HRYN'OVA T; INNES WR; KELSEY MH; KIM P; KOCIAN ML; LEITH DWGS; LIBBY J; LUITZ S; LUTH V; LYNCH HL; MARSISKE H; MESSNER R; MULLER DR; O'GRADY CP; OZCAN VE; PERAZZO A; PERL M; RATCLIFF BN; ROODMAN A; SALNIKOV AA; SCHINDLER RH; SCHWIENING J; SNYDER A; SOHA A; STELZER J; STRUBE J; SU D; SULLIVAN MK; THOMPSON J; VA'VRA J; WAGNER SR; WEAVER M; WISNIEWSKI WJ; WITTGEN M; WRIGHT DH; YARRITU AK; YOUNG CC; BURCHAT PR; EDWARDS AJ; MAJEWSKI SA; PETERSEN BA; ROAT C; AHMED M; AHMED S; ALAM MS; ERNST JA; SAEED MA; SALEEM M; WAPPLER FR; BUGG W; KRISHNAMURTHY M; SPANIER SM; ECKMANN R; KIM H; RITCHIE JL; SATPATHY A; SCHWITTERS RF; IZEN JM; KITAYAMA I; LOU XC; YE S; BIANCHI F; BONA M; GALLO F; GAMBA D; BOSISIO L; CARTARO C; COSSUTTI F; DELLA RICCA G; DITTONGO S; GRANCAGNOLO S; LANCERI L; POROPAT P; VITALE L; VUAGNIN G; MARTINEZ VIDAL F; PANVINI RS; BANERJEE S; BHUYAN B; BROWN CM; FORTIN D; JACKSON PD; KOWALEWSKI R; RONEY JM; SOBIE RJ; BACK JJ; HARRISON PF; MOHANTY GB; BAND HR; CHEN X; CHENG B; DASU S; DATTA M; EICHENBAUM AM; FLOOD KT; GRAHAM M; HOLLAR JJ; JOHNSON JR; KUTTER PE; LI H; LIU R; MIHALYI A; PAN Y; PREPOST R; TAN P; VON WIMMERSPERG TOELLER JH; WU J; WU SL; YU Z; GREENE MG; NEAL H.
2005
Abstract
We search for a charged partner of the X(3872) in the decay B-->X-K, X--->J/psipi(-)pi(0), using 234x10(6) B (B) over bar events collected at the Y(4S) resonance with the BABAR detector at the PEP-II e(+)e(-) asymmetric-energy storage ring. The resulting product branching fraction upper limits are B(B-0-->X-K+,X--->J/psipi(-)pi(0))<5.4x10(-6) and B(B--->X-(K) over bar (0),X--->J/psipi(-)pi(0))<22x10(-6) at the 90% confidence level.
Citazione
Search for a charged partner of the X(3872) in the B meson decay B -> X-K, X--> J/psi pi(-)pi(0) / Aubert, B; Barate, R; Boutigny, D; Couderc, F; Karyotakis, Y; Lees, Jp; Poireau, V; Tisserand, V; Zghiche, A; GRAUGES POUS, E; Palano, A; Pompili, A; Chen, Jc; Qi, Nd; Rong, G; Wang, P; Zhu, Ys; Eigen, G; Ofte, I; Stugu, B; Abrams, Gs; Borgland, Aw; Breon, Ab; Brown, Dn; BUTTON SHAFER, J; Cahn, Rn; Charles, E; Day, Ct; Gill, Ms; Gritsan, Av; Groysman, Y; Jacobsen, Rg; Kadel, Rw; Kadyk, J; Kerth, Lt; Kolomensky, Yg; Kukartsev, G; Lynch, G; Mir, Lm; Oddone, Pj; Orimoto, Tj; Pripstein, M; Roe, Na; Ronan, Mt; Wenzel, Wa; Barrett, M; Ford, Ke; Harrison, Tj; Hart, Aj; Hawkes, Cm; Morgan, Se; Watson, At; Fritsch, M; Goetzen, K; Held, T; Koch, H; Lewandowski, B; Pelizaeus, M; Schroeder, T; Steinke, M; Boyd, Jt; Chevalier, N; Cottingham, Wn; Kelly, Mp; Latham, Te; Wilson, Ff; CUHADAR DONSZELMANN, T; Hearty, C; Knecht, Ns; Mattison, Ts; Mckenna, Ja; Thiessen, D; Khan, A; Kyberd, P; Teodorescu, L; Blinov, Ae; 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[10.1103/physrevd.71.031501]
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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.