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Titolo:
K(0) PRODUCTION IN ONE-PRONG TAU-DECAYS
Autore:
BUSKULIC D; CASPER D; DEBONIS I; DECAMP D; GHEZ P; GOY C; LEES JP; MINARD MN; ODIER P; PIETRZYK B; ARIZTIZABAL F; CHMEISSANI M; CRESPO JM; EFTHYMIOPOULOS I; FERNANDEZ E; FERNANDEZBOSMAN M; GAITAN V; GARRIDO L; MARTINEZ M; MATTISON T; ORTEU S; PACHECO A; PADILLA C; PASCUAL A; TEUBERT F; CREANZA D; DEPALMA M; FARILLA A; IASELLI G; MAGGI G; MARINELLI N; NATALI S; NUZZO S; RANIERI A; RASO G; ROMANO F; RUGGIERI F; SELVAGGI G; SILVESTRIS L; TEMPESTA P; ZITO G; CHAI Y; HUANG D; HUANG X; LIN J; WANG T; XIE Y; XU D; XU R; ZHANG J; ZHANG L; ZHAO W; BLUCHER E; BONVICINI G; BOUDREAU J; COMAS P; COYLE P; DREVERMANN H; FORTY RW; GANIS G; GAY C; GIRONE M; HAGELBERG R; HARVEY J; JACOBSEN R; JOST B; KNOBLOCH J; LEHRAUS I; MAGGI M; MARKOU C; MATO P; MEINHARD H; MINTEN A; MIQUEL R; PALAZZI P; PATER JR; PERLAS JA; PERRODO P; PUSZTASZERI JF; RANJARD F; ROLANDI L; ROTHBERG J; RUAN T; SAICH M; SCHLATTER D; SCHMELLING M; SEFKOW F; TEJESSY W; TOMALIN IR; VEENHOF R; WACHSMUTH H; WASSERBAECH S; WIEDENMANN W; WILDISH T; WITZELING W; WOTSCHACK J; AJALTOUNI Z; BARDADINOTWINOWSKA M; BARRES A; BOYER C; FALVARD A; GAY P; GUICHENEY C; HENRARD P; JOUSSET J; MICHEL B; MONTRET JC; PALLIN D; PERRET P; PODLYSKI F; PRORIOL J; SAADI F; FEARNLEY T; HANSEN JB; HANSEN JD; HANSEN JR; HANSEN PH; JOHNSON SD; MOLLERUD R; NILSSON BS; KYRIAKIS A; SIMOPOULOU E; SIOTIS I; VAYAKI A; ZACHARIADOU K; BADIER J; BLONDEL A; BONNEAUD G; BRIENT JC; BOURDON P; FOUQUE G; PASSALACQUA L; ROUGE A; RUMPF M; TANAKA R; VERDERI M; VIDEAU H; CANDLIN DJ; PARSONS MI; VEITCH E; FOCARDI E; MONETA L; PARRINI G; CORDEN M; DELFINO M; GEORGIOPOULOS C; JAFFE DE; LEVINTHAL D; ANTONELLI A; BENCIVENNI G; BOLOGNA G; BOSSI F; CAMPANA P; CAPON G; CERUTTI F; CHIARELLA V; FELICI G; LAURELLI P; MANNOCCHI G; MURTAS F; MURTAS GP; PEPEALTARELLI M; SALOMONE S; COLRAIN P; TENHAVE I; KNOWLES IG; LYNCH JG; MAITLAND W; MORTON WT; RAINE C; REEVES P; SCARR JM; SMITH K; SMITH MG; THOMPSON AS; THORN S; TURNBULL RM; BECKER U; BRAUN O; GEWENIGER C; HANKE P; HEPP V; KLUGE EE; PUTZER A; RENSCH B; SCHMIDT M; STENZEL H; TITTEL K; WUNSCH M; BEUSELINCK R; BINNIE DM; CAMERON W; CATTANEO M; COLLING DJ; DORNAN PJ; HASSARD JF; KONSTANTINIDIS N; MOUTOUSSI A; NASH J; PAYNE DG; SANMARTIN G; SEDGBEER JK; WRIGHT AG; GIRTLER P; KUHN D; RUDOLPH G; VOGL R; BOWDERY CK; BRODBECK TJ; FINCH AJ; FOSTER F; HUGHES G; JACKSON D; KEEMER NR; NUTTALL M; PATEL A; SLOAN T; SNOW SW; WHELAN EP; GALLA A; GREENE AM; KLEINKNECHT K; RAAB J; RENK B; SANDER HG; SCHMIDT H; WALTHER SM; WANKE R; WOLF B; BENCHEIKH AM; BENCHOUK C; BONISSENT A; CALVET D; CARR J; DIACONU C; ETIENNE F; NICOD D; PAYRE P; ROOS L; ROUSSEAU D; SCHWEMLING P; TALBY M; ADLUNG S; ASSMANN R; BAUER C; BLUM W; BROWN D; CATTANEO P; DEHNING B; DIETL H; DYDAK F; FRANK M; HALLEY AW; JAKOBS K; KROHA H; LAUBER J; LUTJENS G; LUTZ G; MANNER W; MOSER HG; RICHTER R; SCHRODER J; SCHWARZ AS; SETTLES R; SEYWERD H; STIERLIN U; STIEGLER U; STDENIS R; WOLF G; ALEMANY R; BOUCROT J; CALLOT O; CORDIER A; DAVIER M; DUFLOT L; GRIVAZ JF; HEUSSE P; JANOT P; KIM DW; LEDIBERDER F; LEFRANCOIS J; LUTZ AM; MUSOLINO G; PARK HJ; SCHUNE MH; VEILLET JJ; VIDEAU I; ABBANEO D; BAGLIESI G; BATIGNANI G; BOTTIGLI U; BOZZI C; CALDERINI G; CARPINELLI M; CIOCCI MA; CIULLI V; DELLORSO R; FERRANTE I; FIDECARO F; FOA L; FORTI F; GIASSI A; GIORGI MA; GREGORIO A; LIGABUE F; LUSIANI A; MARROCCHESI PS; MARTIN EB; MESSINEO A; PALLA F; RIZZO G; SANGUINETTI G; SPAGNOLO P; STEINBERGER J; TENCHINI R; TONELLI G; TRIGGIANI G; VALASSI A; VANNINI C; VENTURI A; VERDINI PG; WALSH J; BETTERIDGE AP; GAO Y; GREEN MG; JOHNSON DL; MARCH PV; MEDCALF T; MIR LM; QUAZI IS; STRONG JA; BERTIN V; BOTTERILL DR; CLIFFT RW; EDGECOCK TR; HAYWOOD S; EDWARDS M; NORTON PR; THOMPSON JC; BLOCHDEVAUX B; COLAS P; DUARTE H; EMERY S; KOZANECKI W; LANCON E; LEMAIRE MC; LOCCI E; MARX B; PEREZ P; RANDER J; RENARDY JF; ROSOWSKY A; ROUSSARIE A; SCHULLER JP; SCHWINDLING J; MOHAND DS; VALLAGE B; JOHNSON RP; LITKE AM; TAYLOR G; WEAR J; BEDDALL A; BOOTH CN; CARTWRIGHT S; COMBLEY F; DAWSON I; KOKSAL A; RANKIN C; THOMPSON LF; BOHRER A; BRANDT S; COWAN G; FEIGL E; GRUPEN C; LUTTERS G; MINGUETRODRIGUEZ J; RIVERA F; SARAIVA P; SCHAFER U; SMOLIK L; BOSISIO L; DELLAMARINA R; GIANNINI G; GOBBO B; PITIS L; RAGUSA F; BELLANTONI L; CHEN W; CONWAY JS; FENG Z; FERGUSON DPS; GAO YS; GRAHL J; HARTON JL; HAYES OJ; HU H; NACHTMAN JM; PAN YB; SAADI Y; SCHMITT M; SCOTT I; SHARMA V; TURK JD; WALSH AM; WEBER FV; WU SL; WU X; YAMARTINO JM; ZHENG M; ZOBERNIG G;
Indirizzi:
LAB PHYS PARTICULES,CNRS,IN2P3 F-74019 ANNECY LE VIEUX FRANCE UNIV AUTONOMA BARCELONA,INST FIS ALTES ENERGIES E-08193 BARCELONA SPAIN INFN,DIPARTIMENTO FIS I-70126 BARI ITALY CERN,EUROPEAN LAB PARTICLE PHYS CH-1211 GENEVA 23 SWITZERLAND UNIV CLERMONT FERRAND,PHYS CORPUSCULAIRE LAB,CNRS,IN2P3 F-63177 CLERMONT FERRAND FRANCE NIELS BOHR INST DK-2100 COPENHAGEN DENMARK ECOLE POLYTECH,PHYS NUCL & HAUTES ENERGIES LAB,CNRS,IN2P3 F-91128 PALAISEAU FRANCE CHINESE ACAD SCI,INST HIGH ENERGY PHYS BEIJING PEOPLES R CHINA DEMOKRITOS NATL CTR SCI RES ATHENS GREECE UNIV WASHINGTON SEATTLE WA 98195 UNIV TURIN,IST FIS GEN I-10124 TURIN ITALY CNR,IST COSMOGEOFIS TURIN ITALY KANGNUNG NATL UNIV KANGNUNG SOUTH KOREA CERN,DIV PPE CH-1211 GENEVA 23 SWITZERLAND UNIV EDINBURGH,DEPT PHYS EDINBURGH EH8 9JZ MIDLOTHIAN SCOTLAND UNIV FLORENCE,INFN,DIPARTIMENTO FIS I-50125 FLORENCE ITALY FLORIDA STATE UNIV,SUPERCOMP COMPUTAT RES INST TALLAHASSEE FL 32306 INFN,LAB NAZL I-00044 FRASCATI ITALY UNIV HEIDELBERG,INST HOCHENERGIEPHYS D-69120 HEIDELBERG GERMANY UNIV MAINZ,INST PHYS D-55099 MAINZ GERMANY FAC SCI LUMINY,CTR PHYS PARTICULES,CNRS,IN2P3 F-13288 MARSEILLE FRANCE WERNER HEISENBERG INST,MAX PLANCK INST PHYS D-80805 MUNICH GERMANY SCUOLA NORMALE SUPER PISA I-56010 PISA ITALY UNIV LONDON ROYAL HOLLOWAY & BEDFORD NEW COLL,DEPT PHYS EGHAM TW20 0EX SURREY ENGLAND UNIV SIEGEN,FACHBEREICH PHYS D-57068 SIEGEN GERMANY INFN I-34127 TRIESTE ITALY UNIV GLASGOW,DEPT PHYS & ASTRON GLASGOW G12 8QQ SCOTLAND UNIV LONDON IMPERIAL COLL SCI TECHNOL & MED,DEPT PHYS LONDON SW7 2BZ ENGLAND INNSBRUCK UNIV,INST EXPTL PHYS A-6020 INNSBRUCK AUSTRIA UNIV LANCASTER,DEPT PHYS LANCASTER LA1 4YB ENGLAND UNIV PARIS 11,ACCELERATEUR LINEAIRE LAB,CNRS,IN2P3 F-91405 ORSAY FRANCE UNIV PISA,INFN,DIPARTIMENTO FIS I-56010 PISA ITALY CTR ETUD SACLAY,DAPNIA,SERV PHYS PARTICULES F-91191 GIF SUR YVETTE FRANCE RUTHERFORD APPLETON LAB,DEPT PARTICLE PHYS DIDCOT OX11 0QX OXON ENGLAND UNIV CALIF SANTA CRUZ,INST PARTICLE PHYS SANTA CRUZ CA 95064 UNIV SHEFFIELD,DEPT PHYS SHEFFIELD S3 7RH S YORKSHIRE ENGLAND UNIV WISCONSIN,DEPT PHYS MADISON WI 53706 UNIV TRIESTE,DIPARTIMENTO FIS I-34127 TRIESTE ITALY
Titolo Testata:
Physics letters. Section B
fascicolo: 1-2, volume: 332, anno: 1994,
pagine: 219 - 227
SICI:
0370-2693(1994)332:1-2<219:KPIOT>2.0.ZU;2-C
Fonte:
ISI
Lingua:
ENG
Soggetto:
LEPTONS; LEP;
Tipo documento:
Article
Natura:
Periodico
Settore Disciplinare:
Science Citation Index Expanded
Citazioni:
12
Recensione:
Indirizzi per estratti:
Citazione:
D. Buskulic et al., "K(0) PRODUCTION IN ONE-PRONG TAU-DECAYS", Physics letters. Section B, 332(1-2), 1994, pp. 219-227

Abstract

From a sample of about 75000 tau decays identified with the ALEPH detector, K0 production in 1-prong hadronic decays is investigated by tagging the K(L)0 component in a hadronic calorimeter. Results are given for the final states nu(tau)h-K0 and nu(tau)h-pi0K0 where the h- is separated into pi and K contributions by means of the dE/dx measurement in the central detector. The resulting branching ratios are: (B(tau) --> nu(tau)pi-K0) = (0.88 +/- 0.14 +/- 0.09)%, (B(tau) --> nu(tau)K-K0)= (0.29 +/- 0.12 +/- 0.03)%, (Btau --> nu(tau)pi-pi0K0) = (0.33 +/- 0.14 +/- 0.07)% and (B(tau) --> nu(tau)K-pi0K0) = (0.05 +/- 0.05 +/- 0.01)%. The K decay rate in the K0pi channel agrees with that in the Kpi0 mode: the combined value for the branching ratio is (Btau --> nu(tau)K-) = (1.45 +/- 0.13 +/- 0.11)%.

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Documento generato il 02/12/20 alle ore 17:51:35