Physics with e+e- linear colliders

被引:349
|
作者
Accomando, E
Andreazza, A
Anlauf, H
Ballestrero, A
Barklow, T
Bartels, J
Bartl, A
Battaglia, M
Beenakker, W
Belanger, G
Bernreuther, W
Biebel, J
Binnewies, J
Blumlein, J
Boos, E
Borzumati, F
Boudjema, F
Brandenburg, A
Bussey, PJ
Cacciari, M
Casalbuoni, R
Corsetti, A
De Curtis, S
Cuypers, F
Daskalakis, G
Deandrea, A
Denner, A
Diehl, M
Dittmaier, S
Djouadi, A
Dominici, D
Dreiner, H
Eberl, H
Ellwanger, U
Engel, R
Flottmann, K
Franz, H
Gajdosik, T
Gatto, R
Genten, H
Godbole, R
Gounaris, G
Greco, M
Grivaz, JF
Guetta, D
Haidt, D
Harlander, R
He, HJ
Hollik, W
Huitu, K
机构
[1] DESY, D-22603 Hamburg, Germany
[2] Ist Nazl Fis Nucl, I-10125 Turin, Italy
[3] Univ Turin, Dipartimento Fis Teor, I-10125 Turin, Italy
[4] Univ Milan, Dipartimento Fis, I-20133 Milan, Italy
[5] Ist Nazl Fis Nucl, I-20133 Milan, Italy
[6] Tech Univ Darmstadt, Inst Kernphys, D-64289 Darmstadt, Germany
[7] Stanford Univ, Stanford Linear Accelerator Ctr, Stanford, CA 94309 USA
[8] Univ Hamburg, Inst Theoret Phys 2, D-22761 Hamburg, Germany
[9] Univ Vienna, Inst Theoret Phys, A-1090 Vienna, Austria
[10] CERN, CH-1211 Geneva 23, Switzerland
[11] Leiden Univ, Lorentz Inst Theoret Phys, NL-2300 RA Leiden, Netherlands
[12] ENSLAPP, F-74941 Annecy Le Vieux, France
[13] Rhein Westfal TH Aachen, Phys Zentrum, D-52074 Aachen, Germany
[14] DESY, Inst Hochenergiephys, D-15738 Zeuthen, Germany
[15] Moscow MV Lomonosov State Univ, Inst Nucl Phys, RU-119899 Moscow, Russia
[16] Weizmann Inst Sci, Dept Particle Phys, IL-76100 Rehovot, Israel
[17] Univ Glasgow, Dept Phys, Glasgow G12 8QQ, Lanark, Scotland
[18] Univ Florence, Dipartimento Fis, I-50125 Florence, Italy
[19] Northeastern Univ, Dept Phys, Boston, MA 02115 USA
[20] Ist Nazl Fis Nucl, I-50125 Florence, Italy
[21] Paul Scherrer Inst, CH-5232 Villigen, Switzerland
[22] NRCPS Demokritos, Inst Nucl Phys, GR-15310 Athens, Greece
[23] CNRS Marseille Luminy, Ctr Phys Theor, F-13288 Marseille 9, France
[24] Univ Cambridge, Dept Appl Math & Theoret Phys, Cambridge CB3 9EW, England
[25] Univ Montpellier 2, Phys Math Lab, F-34095 Montpellier 5, France
[26] Rutherford Appleton Lab, Didcot OX11 0QX, Oxon, England
[27] Austrian Acad Sci, Inst Hochenergiephys, A-1050 Vienna, Austria
[28] Univ Paris 11, LAL, F-91405 Orsay, France
[29] Univ Leipzig, Fachbereich Phys, D-04109 Leipzig, Germany
[30] Univ Geneva, Dept Phys Theor, CH-1211 Geneva 4, Switzerland
[31] Indian Inst Sci, Ctr Theoret Studies, Bangalore 560012, Karnataka, India
[32] Aristotle Univ Thessaloniki, Dept Theoret Phys, GR-54006 Thessaloniki, Greece
[33] Ist Nazl Fis Nucl, Lab Nazl Frascati, I-00044 Frascati, Italy
[34] Univ Bologna, Dipartimento Fis, I-40126 Bologna, Italy
[35] Univ Karlsruhe, Inst Theoret Phys, D-76128 Karlsruhe, Germany
[36] Univ Helsinki, Helsinki Inst Phys, FIN-00014 Helsinki, Finland
[37] Heidelberg Univ, Inst Phys, D-69120 Heidelberg, Germany
[38] Silesian Univ, Dept Theoret Phys, PL-40007 Katowice, Poland
[39] Swiss Fed Inst Technol, Lab Hochenergiephys, CH-8093 Zurich, Switzerland
[40] Univ Warsaw, Inst Theoret Phys, PL-00681 Warsaw, Poland
[41] Max Planck Inst Phys & Astrophys, Werner Heisenberg Inst Phys, D-80805 Munich, Germany
[42] Ludwig Maximillians Univ, Inst Theoret Phys, D-80333 Munich, Germany
[43] Univ Autonoma Barcelona, E-08193 Barcelona, Spain
[44] Ist Nazl Fis Nucl, Sez Roma 1, I-00185 Rome, Italy
[45] Univ Roma La Sapienza 1, Dipartimento Fis, I-00185 Rome, Italy
[46] UCL, Dept Phys & Astron, London WC1E 6BT, England
[47] Univ Barcelona, Fac Fis, E-08028 Barcelona, Spain
[48] Univ Bergen, Inst Phys, N-5007 Bergen, Norway
[49] Univ Trieste, Dipartimento Fis Teor, I-34014 Trieste, Italy
[50] Turku Univ, Dept Appl Phys, FIN-20500 Turku, Finland
来源
关键词
e(+)e(-) linear colliders; top quark; electroweak gauge bosons; Higgs; supersymmetry; compositeness;
D O I
10.1016/S0370-1573(97)00086-0
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The physics potential of e(+) e(-) linear colliders is summarized in this report. These machines are planned to operate in the first phase at a center-of-mass energy of 500 GeV, before being scaled up to about 1 TeV. In the second phase of the operation, a final energy of about 2 TeV is expected. The machines will allow us to perform precision tests of the heavy particles in the Standard Model, the top quark and the electroweak bosons. They are ideal facilities for exploring the properties of Higgs particles, in particular in the intermediate mass range. New vector bosons and novel matter particles in extended gauge theories can be searched for and studied thoroughly. The machines provide unique opportunities for the discovery of particles in supersymmetric extensions of the Standard Model, the spectrum of Higgs particles, the supersymmetric partners of the electroweak gauge and Higgs bosons, and of the matter particles. High precision analyses of their properties and interactions will allow for extrapolations to energy scales close to the Planck scale where gravity becomes significant. In alternative scenarios, i.e. compositeness models, novel matter particles and interactions can be discovered and investigated in the energy range above the existing colliders lip to the TeV scale. Whatever scenario is realized in Nature, the discovery potential of e(+) e(-) linear colliders and the high precision with which the properties of particles and their interactions can be analyzed, define an exciting physics program complementary to hadron machines. (C) 1998 Elsevier Science B.V. All rights reserved.
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页码:1 / 78
页数:78
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