Measurement of the one-prong hadronic tau branching ratios at LEP
Measurement of the one-prong hadronic tau branching ratios at LEP
复制标题
LEP 单管强子 tau 分支比的测量
DOI:
10.1007/s100520050197
复制
发表时间:
1998
期刊:
影响因子:
--
通讯作者:
J. S. White
中科院分区:
文献类型:
--
作者:
K. Ackersta;G. Alexander;J. Allison;N. Altekamp;K. Anderson;S. Anderson;S. Arcelli;S. Asai;S. Ashby;D. Axen;G. Azuelos;A. Ball;E. Barberio;R. Barlow;R. Bartoldus;J. Batley;S. Baumann;J. Bechtluft;C. Beeston;T. Behnke;A. Bell;K. Bell;G. Bella;S. Bentvelsen;S. Bethke;S. Betts;O. Biebel;A. Biguzzi;S. Bird;V. Blobel;I. Bloodworth;J. Bloomer;M. Bobinski;P. Bock;D. Bonacorsi;M. Boutemeur;S. Braibant;L. Brigliadori;R. Brown;H. Burckhart;C. Burgard;R. B. Urgin;P. Capiluppi;R. Carnegie;A. Carter;J. Carter;C. Y. Chang;D. Charlton;D. Chrisman;P. Clarke;I. Cohen;J. Conboy;O. Cooke;C. Couyoumtzelis;R. Coxe;S. Dado;C. Dallapiccola;G. Dallavalle;R. Davis;S. Jong;L. Pozo;K. Desch;B. Dienes;M. Dixit;M. Doucet;E. Duchovni;G. Duckeck;I. Duerdoth;D. Eatough;J. Edwards;P. Estabrooks;H. Evans;M. Evans;F. Fabbri;A. Fanfani;M. Fanti;A. Faust;L. Feld;F. Fiedler;M. Fierro;H. Fischer;I. Fleck;R. Folman;D. Fong;M. Foucher;A. F. Urtjes;D. Futyan;P. Gagnon;J. Gary;J. Gascón;S. Gascon;N. Geddes;C. Geich;T. Geralis;G. Giacomelli;Paolo Giacomelli;R. Giacomelli;V. Gibson;W. Gibson;D. Gingrich;D. Glenzinski;J. Goldberg;M. Goodrick;W. Gorn;C. Grandi;E. Gross;J. Grunhaus;M. Gruw;C. Hajdu;G. Hanson;M. Hansroul;M. Hapke;C. Hargrove;P. Hart;C. Hartmann;M. Hauschild;C. Hawkes;R. Hawkings;R. J. Hemingway;M. Herndon;G. Herten;R. Heuer;M. Hildreth;J. Hill;S. Hillier;P. Hobson;A. Hocker;R. Homer;A. Honma;D. Horv;K. R. Hossain;R. Howard;P. H. Untemeyer;D. Hutchcroft;P. Igo;D. Imrie;M. Ingram;K. Ishii;A. Jawahery;P. Reys;H. Jérémie;M. Jimack;A. Joly;C. Jones;G. Jones;M. Jones;U. Jost;P. Jovanović;T. Junk;J. Kanzaki;D. Karlen;V. Kartvelishvili;K. Kawagoe;T. Kawamoto;P. Kayal;R. Keeler;R. Kellogg;B. Kennedy;J. Kirk;A. Klier;S. Kluth;T. Kobayashi;M. Kobel;D. Koetke;T. Kokott;M. Kolrep;S. Komamiya;T. Kress;P. Krieger;J. Krogh;P. Kyberd;R. Lahmann;W. Lai;D. Lanske;J. Lauber;S. Lautenschlager;J. Layter;D. Lazic;A. Lee;E. Lefebvre;D. Lellouch;J. Letts;L. Levinson;S. Lloyd;F. Loebinger;G. D. Long;M. Losty;J. Ludwig;D. Lui;A. Macchiolo;A. Macpherson;M. Mannelli;S. Marcellini;C. Markopoulos;C. Markus;A. Martin;J. Martin;G. Martinez;T. Mashimo;W. Mcdonald;J. Mckenna;E. Mckigney;T. Mcmahon;R. McPherson;F. Meijers;S. Menke;F. Merritt;H. Mes;J. Meyer;A. Michelini;G. Mikenberg;D. Miller;A. Mincer;R. Mir;W. Mohr;A. Montanari;T. Mori;U. M. Uller;S. Mihara;K. Nagai;I. Nakamura;H. Neal;B. Nellen;R. Nisius;S. O'neale;F. G. Oakham;F. Odorici;H. Ogren;A. Oh;N. Oldershaw;M. Oreglia;S. Orito;J. Pater;G. Patrick;J. Patt;R. Perez;S. Petzold;P. Pfeifenschneider;J. Pilcher;J. Pinfold;D. Plane;P. enberger;B. Poli;A. Posthaus;C. Rembser;S. Robertson;S. Robins;N. Rodning;J. Roney;A. Rooke;A. Rossi;P. Routenburg;Y. Rozen;K. Runge;O. Rúnolfsson;U. Ruppel;D. Rust;R. Ryłko;K. Sachs;T. Saeki;W. Sang;E. Sarkisyan;C. Sbarra;A. Schaile;O. Schaile;F. Scharf;P. Schar;J. Schieck;P. Schleper;B. Schmitt;S. Schmitt;H. Schultz;M. Schumacher;C. Schwick;W. Scott;T. Shears;B. Shen;C. Shepherd;P. Sherwood;G. Siroli;A. Sittler;A. Skillman;A. Skuja;A. Smith;G. Snow;R. Sobie;R. Springer;M. Sproston;K. Stephens;J. Steuerer;B. Stockhausen;K. Stoll;D. Strom;P. Szymański;S. Talbot;S. Tanaka;P. Taras;S. Tarem;R. Teuscher;M. Thiergen;M. Thomson;E. Torrence;E. Tsur;A. Turcot;M. F. Turner;P. Utzat;R. Kooten;M. Verzocchi;P. Vikas;E. Vokurka;H. Voss;A. Wagner;C. Ward;D. Ward;P. Watkins;A. Watson;N. Watson;P. Wells;N. Wermes;J. S. White
The branching ratios of theanddecays have been measured using the 1991–1995 data recorded with the OPAL detector at LEP. These branching ratios are measured simultaneously using three selection criteria and are found to be \[ \begin{array} {l c c} {\rm BR}(\tau^- \rightarrow h^- \nu_\tau) & = & (11.98 \pm 0.13 \pm 0.16) \%\\ {\rm BR}(\tau^-\rightarrow h^- \pi^0 \nu_\tau) & = & (25.89 \pm 0.17 \pm 0.29) \%\\ {\rm BR}(\tau^- \rightarrow h^- \geq 2 \pi^0 \nu_\tau ) & = & ( 9.91 \pm 0.31 \pm 0.27) \% \end{array} \] where the first error is statistical and the second is systematic.