Ontology type: schema:ScholarlyArticle Open Access: True
1991-06
AUTHORSL3 Collaboration, B. Adeva, O. Adriani, M. Aguilar-Benitez, H. Akbari, J. Alcaraz, A. Aloisio, G. Alverson, M. G. Alviggi, Q. An, H. Anderhub, A. L. Anderson, V. P. Andreev, T. Angolov, L. Antonov, D. Antreasyan, P. Arce, A. Arefiev, R. de Asmundis, T. Azemoon, T. Aziz, P. V. K. S. Baba, P. Bagnaia, J. A. Bakken, L. Baksay, R. C. Ball, S. Banerjee, J. Bao, L. Barone, A. Bay, U. Becker, J. Behrens, S. Beingessner, Gy. L. Bencze, J. Berdugo, P. Berges, B. Bertucci, B. L. Betev, A. Biland, R. Bizzarri, J. J. Blaising, P. Blömeke, B. Blumenfeld, G. J. Bobbink, M. Bocciolini, R. Bock, A. Böhm, B. Borgia, D. Bourilkov, M. Bourquin, D. Boutigny, B. Bouwens, J. G. Branson, I. C. Brock, F. Bruyant, C. Buisson, A. Bujak, J. D. Burger, J. P. Burq, J. Busenitz, X. D. Cai, M. Capell, F. Carbonara, P. Cardenal, F. Carminati, A. M. Cartacci, M. Cerrada, F. Cesaroni, Y. H. Chang, U. K. Chaturvedi, M. Chemarin, A. Chen, C. Chen, G. M. Chen, H. F. Chen, H. S. Chen, M. Chen, M. L. Chen, W. Y. Chen, G. Chiefari, C. Y. Chien, F. Chollet, C. Civinini, I. Clare, R. Clare, H. O. Cohn, G. Coignet, N. Colino, V. Commichau, G. Conforto, A. Contin, F. Crijns, P. Criscuolo, X. Y. Cui, T. S. Dai, R. D'Alessandro, A. Degré, K. Deiters, E. Dénes, P. Denes, F. DeNotaristefani, M. Dhina, D. DiBitonto, M. Diemoz, F. Diez-Hedo, H. R. Dimitrov, C. Dionisi, R. Divià, M. T. Dova, E. Drago, T. Driever, D. Duchesneau, P. Duinker, I. Duran, H. El Mamouni, A. Engler, F. J. Eppling, F. C. Erné, P. Extermann, R. Fabbretti, G. Faber, M. Fabre, S. Falciano, Q. Fan, S. J. Fan, O. Fackler, J. Fay, J. Fehlmann, T. Ferguson, G. Fernandez, F. Ferroni, H. Fesefeldt, J. Field, F. Filthaut, G. Finocchiaro, P. H. Fisher, G. Forconi, T. Foreman, K. Freudenreich, W. Friebel, M. Fukushima, M. Gailloud, Yu. Galaktionov, E. Gallo, S. N. Ganguli, P. Garcia-Abia, S. S. Gau, D. Gele, S. Gentile, M. Glaubman, S. Goldfarb, Z. F. Gong, E. Gonzalez, A. Gordeev, P. Göttlicher, D. Goujon, G. Gratta, C. Grinnell, M. Gruenewald, M. Guanziroli, J. K. Guo, A. Gurtu, H. R. Gustafson, L. J. Gutay, H. Haan, A. Hasan, D. Hauschildt, C. F. He, T. Hebbeker, M. Hebert, G. Herten, U. Herten, A. Hervé, K. Hilgers, H. Hofer, H. Hoorani, L. S. Hsu, G. Hu, G. O. Hu, B. Ille, M. M. Ilyas, V. Innocente, E. Isiksal, H. Janssen, B. N. Jin, L. W. Jones, A. Kasser, R. A. Khan, Yu. Kamyshkov, Y. Karyotakis, M. Kaur, S. Khokhar, V. Khoze, M. N. Kienzle-Focacci, W. Kinnison, D. Kirkby, W. Kittel, A. Klimentov, A. C. König, O. Kornadt, V. Koutsenko, R. W. Kraemer, T. Kramer, V. R. Krastev, W. Krenz, J. Krizmanic, K. S. Kumar, V. Kumar, A. Kunin, V. Lalieu, G. Landi, D. Lanske, S. Lanzano, P. Lebrun, P. Lecomte, P. Lecoq, P. LeCoultre, D. Lee, I. Leedom, J. M. LeGoff, L. Leistam, R. Leiste, M. Lenti, E. Leonardi, J. Lettry, P. M. Levchenko, X. Leytens, C. Li, H. T. Li, J. F. Li, L. Li, P. J. Li, Q. Li, X. G. Li, J. Y. Liao, Z. Y. Lin, F. L. Linde, B. Lindemann, D. Linnhofer, R. Liu, Y. Liu, W. Lohmann, E. Longo, Y. S. Lu, J. M. Lubbers, K. Lübelsmeyer, C. Luci, D. Luckey, L. Ludovici, X. Lue, L. Luminari, W. G. Ma, M. MacDermott, R. Magahiz, M. Maire, P. K. Malhotra, R. Malik, A. Malinin, C. Maña, D. N. Mao, Y. F. Mao, M. Maolinbay, P. Marchesini, A. Marchionni, B. Martin, J. P. Martin, L. Martinez-Laso, F. Marzano, G. G. G. Massaro, T. Matsuda, K. Mazumdar, P. McBride, T. McMahon, D. McNally, Th. Meinholz, M. Merk, L. Merola, M. Meschini, W. J. Metzger, Y. Mi, G. B. Mills, Y. Mir, G. Mirabelli, J. Mnich, M. Möller, B. Monteleoni, G. Morand, R. Morand, S. Morganti, N. E. Moulai, R. Mount, S. Müller, E. Nagy, M. Napolitano, H. Newman, C. Neyer, M. A. Niaz, L. Niessen, H. Nowak, D. Pandoulas, F. Plasil, G. Passaleva, G. Paternoster, S. Patricelli, Y. J. Pei, D. Perret-Gallix, J. Perrier, A. Pevsner, M. Pieri, D. Piccolo, P. A. Piroué, V. Plyaskin, M. Pohl, V. Pojidaev, N. Produit, J. M. Qian, K. N. Qureshi, R. Raghavan, G. Rahal-Callot, P. Razis, K. Read, D. Ren, Z. Ren, S. Reucroft, A. Ricker, S. Riemann, O. Rind, C. Rippich, H. A. Rizvi, B. P. Roe, M. Röhner, S. Röhner, U. Roeser, L. Romero, J. Rose, S. Rosier-Lees, R. Rosmalen, Ph. Rosselet, A. Rubbia, J. A. Rubio, M. Rubio, W. Ruckstuhl, H. Rykaczewski, M. Sachwitz, J. Salicio, J. M. Salicio, G. Sanders, M. S. Sarakinos, G. Sartorelli, G. Sauvage, A. Savin, V. Schegelsky, K. Schmiemann, D. Schmitz, P. Schmitz, M. Schneegans, H. Schopper, D. J. Schotanus, S. Shotkin, H. J. Schreiber, R. Schulte, S. Schulte, K. Schultze, J. Schütte, J. Schwenke, G. Schwering, C. Sciacca, I. Scott, R. Sehgal, P. G. Seiler, J. C. Sens, I. Sheer, D. Z. Shen, V. Shevchenko, S. Shevchenko, X. R. Shi, K. Shmakov, V. Shoutko, E. Shumilov, N. Smirnov, E. Soderstrom, A. Sopczak, C. Spartiotis, T. Spickermann, B. Spiess, P. Spillantini, R. Starosta, M. Steuer, D. P. Stickland, F. Sticozzi, W. Stoeffl, H. Stone, K. Strauch, B. C. Stringfellow, K. Sudhakar, G. Sultanov, R. L. Sumner, L. Z. Sun, H. Suter, R. B. Sutton, J. D. Swain, A. A. Syed, X. W. Tang, E. Tarkovsky, L. Taylor, C. Timmermans, Samuel C. C. Ting, S. M. Ting, Y. P. Tong, F. Tonisch, M. Tonutti, S. C. Tonwar, J. Tóth, G. Trowitzsch, C. Tully, K. L. Tung, J. Ulbricht, L. Urbán, U. Uwer, E. Valente, R. T. Van de Walle, I. Vetlitsky, G. Viertel, P. Vikas, U. Vikas, M. Vivargent, H. Vogel, H. Vogt, G. Von Dardel, I. Vorobiev, A. A. Vorobyov, An. A. Vorobyov, L. Vuilleumier, M. Wadhwa, W. Wallraff, C. R. Wang, G. H. Wang, J. H. Wang, Q. F. Wang, X. L. Wang, Y. F. Wang, Z. Wang, Z. M. Wang, A. Weber, J. Weber, R. Weill, T. J. Wenaus, J. Wenninger, M. White, C. Willmott, F. Wittgenstein, D. Wright, R. J. Wu, S. L. Wu, S. X. Wu, Y. G. Wu, B. Wyslouch, Y. Y. Xie, Y. D. Xu, Z. Z. Xu, Z. L. Xue, D. S. Yan, X. J. Yan, B. Z. Yang, C. G. Yang, G. Yang, K. S. Yang, Q. Y. Yang, Z. Q. Yang, C. H. Ye, J. B. Ye, Q. Ye, S. C. Yeh, Z. W. Yin, J. M. You, M. Yzerman, C. Zaccardelli, L. Zehnder, P. Zemp, M. Zeng, Y. Zeng, D. H. Zhang, Z. P. Zhang, J. F. Zhou, R. Y. Zhu, H. L. Zhuang, A. Zichichi
ABSTRACTWe have studied the reactionse+e−→hadrons,e+e−, μ+ μ− and τ+ τ−, in the energy range 88.2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $$ \leqq \sqrt s \leqq 94.2$$ \end{document} GeV. A total luminosity of 5.5 pb−1, corresponding to approximately 115000 hadronic and 10000 leptonicZ0 decays, has been recorded with the L3 detector. From a simultaneous fit to all of our measured cross section data, we obtain assuming lepton universality:\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $$\begin{gathered} M_z = 91.181 \pm 0.010 \pm 0.02 (LEP) GeV, \hfill \\ \Gamma _z = 2501 \pm 17 MeV, \hfill \\ \Gamma _{had} = 1742 \pm 19 MeV, \Gamma _t = 83.6 \pm 0.8 MeV. \hfill \\ \end{gathered}$$ \end{document}If we do not assume lepton universality, we obtain for the partial decay widths of theZ0 intoe+e− μ+ μ− and τ+ τ−:\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $$\begin{gathered} \Gamma _e = 83.3 \pm 1.1 MeV, \Gamma _\mu = 84.5 \pm 2.0 MeV, \hfill \\ \Gamma _\tau = 84.0 \pm 2.7 MeV. \hfill \\ \end{gathered}$$ \end{document}From the measured ratio of the invisible and the leptonic decay widths of theZ0, we determine the number of light neutrino species to beNv=3.05±0.10. We include our measurements of the forward-backward asymmetry for the leptonic channels in a fit to determine the vector and axial-vector neutral current coupling constants of charged leptons to theZ0. We obtain\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $$\bar g_V = - 0.046_{ - 0.012}^{ + 0.015}$$ \end{document} and\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $$\bar g_A = - 0.500 \pm 0.003$$ \end{document}. In the framework of the Standard Model, we estimate the top quark mass to bemt=193−69+52±16 (Higgs) GeV, and we derive a value for the weak mixing angle of sin2θW=1−(MW/MZ)2=0.222 ± 0.008, corresponding to an effective weak mixing angle of\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $$\sin ^2 \bar \theta _W = 0.2315 \pm 0.0025$$ \end{document}. More... »
PAGES179-203
http://scigraph.springernature.com/pub.10.1007/bf01475788
DOIhttp://dx.doi.org/10.1007/bf01475788
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