Precise determination of the Z resonance parameters at LEP:: "Zedometry"

被引:48
作者
Abbiendi, G [1 ]
Ainsley, C
Akesson, PF
Alexander, G
Allison, J
Anagnostou, G
Anderson, KJ
Arcelli, S
Asai, S
Ashby, SF
Axen, D
Azuelos, G
Bailey, I
Ball, AH
Barberio, E
Barlow, RJ
Behnke, T
Bell, KW
Bella, G
Bellerive, A
Benelli, G
Bentvelsen, S
Beeston, C
Bethke, S
Biebel, O
Bloodworth, IJ
Boeriu, O
Bock, P
Böhme, J
Bonacorsi, D
Boutemeur, M
Braibant, S
Bright-Thomas, P
Brigliadori, L
Brown, RM
Burckhart, HJ
Cammin, J
Capiluppi, P
Carnegie, RK
Caron, B
Carter, AA
Carter, JR
Chang, CY
Charlton, DG
Clarke, PEL
Clay, E
Cohen, I
Conboy, JE
Cooke, OC
Couchman, J
机构
[1] Univ Birmingham, Sch Phys & Astron, Birmingham B15 2TT, W Midlands, England
[2] Univ Bologna, Dipartimento Fis, I-40126 Bologna, Italy
[3] Ist Nazl Fis Nucl, I-40126 Bologna, Italy
[4] Univ Bonn, Inst Phys, D-53115 Bonn, Germany
[5] Univ Calif Riverside, Dept Phys, Riverside, CA 92521 USA
[6] Cavendish Lab, Cambridge CB3 0HE, England
[7] Carleton Univ, Dept Phys, Ottawa Carleton Inst Phys, Ottawa, ON K1S 5B6, Canada
[8] Carleton Univ, Ctr Res Particle Phys, Ottawa, ON K1S 5B6, Canada
[9] CERN, European Org Nucl Res, CH-1211 Geneva 23, Switzerland
[10] Univ Chicago, Eurico Fermi Inst, Chicago, IL 60637 USA
[11] Univ Chicago, Dept Phys, Chicago, IL 60637 USA
[12] Univ Freiburg, Fak Phys, D-79104 Freiburg, Germany
[13] Heidelberg Univ, Inst Phys, D-69120 Heidelberg, Germany
[14] Indiana Univ, Dept Phys, Bloomington, IN 47405 USA
[15] Queen Mary Univ London, London E1 4NS, England
[16] Tech Hsch Aachen, Inst Phys 3, D-52056 Aachen, Germany
[17] UCL, London WC1E 6BT, England
[18] Univ Manchester, Schuster Lab, Dept Phys, Manchester M13 9PL, Lancs, England
[19] Univ Maryland, Dept Phys, College Pk, MD 20742 USA
[20] Univ Montreal, Nucl Phys Lab, Montreal, PQ H3C 3J7, Canada
[21] Univ Oregon, Dept Phys, Eugene, OR 97403 USA
[22] Rutherford Appleton Lab, CLRC, Didcot OX11 0QX, Oxon, England
[23] Technion Israel Inst Technol, Dept Phys, IL-32000 Haifa, Israel
[24] Tel Aviv Univ, Dept Phys & Astron, IL-69978 Tel Aviv, Israel
[25] Univ Tokyo, Int Ctr Elementary Particle Phys, Tokyo 1130033, Japan
[26] Univ Tokyo, Dept Phys, Tokyo 1130033, Japan
[27] Kobe Univ, Kobe, Hyogo 6578501, Japan
[28] Weizmann Inst Sci, Particle Phys Dept, IL-76100 Rehovot, Israel
[29] Univ Hamburg, DESY, Inst Expt Phys 2, D-22607 Hamburg, Germany
[30] Univ Victoria, Dept Phys, Victoria, BC V8W 3P6, Canada
[31] Univ British Columbia, Dept Phys, Vancouver, BC V6T 1Z1, Canada
[32] Univ Alberta, Dept Phys, Edmonton, AB T6G 2J1, Canada
[33] Res Inst Particle & Nucl Phys, H-1525 Budapest, Hungary
[34] Inst Nucl Res, H-4001 Debrecen, Hungary
[35] Univ Munich, Sekt Phys, D-85748 Garching, Germany
[36] Max Planck Inst Phys & Astrophys, D-80805 Munich, Germany
[37] Yale Univ, Dept Phys, New Haven, CT 06520 USA
[38] Duke Univ, Dept Phys, Durham, NC 27708 USA
[39] TRIUMF, Vancouver, BC V6T 2A3, Canada
[40] Inst Nucl Res, H-4001 Debrecen, Hungary
[41] Stanislaw Staszic Univ Min & Met, PL-30059 Krakow, Poland
[42] Univ Debrecen, Dept Expt Phys, Debrecen, Hungary
[43] MPI Munchen, Munich, Germany
[44] Res Inst Particle & Nucl Phys, Budapest, Hungary
[45] Univ Calif Riverside, High Energy Phys Grp, Riverside, CA 92521 USA
[46] CERN, Div EP, CH-1211 Geneva 23, Switzerland
[47] Tel Aviv Univ, Sch Phys & Astron, IL-69978 Tel Aviv, Israel
来源
EUROPEAN PHYSICAL JOURNAL C | 2001年 / 19卷 / 04期
关键词
D O I
10.1007/s100520100627
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
This final analysis of hadronic and leptonic cross-sections and of leptonic forward-backward asymmetries in e(+)e(-) collisions With the OPAL detector makes use of the full LEP 1 data sample comprising 161pb(-1) of integrated luminosity and 4.5 x 10(6) selected Z decays. An interpretation of the data in terms of contributions from pure Z exchange and from gamma /Z interference allows the parameters of the Z resonance to be determined in a model-independent way. Our results are in good agreement with lepton universality anti consistent with the vector and axial-vector couplings predicted in the Standard Model. A fit to the complete dataset yields the fundamental Z resonance parameters: m(z) = (91.1852 +/- 0.0030) GeV. Gamma (Z) = 12.4948 +/- 0.0041) GeV. sigma (0)(h) = (41.501 +/- 0.055) nb. R-l = 20.823 +/- 0.044, and A(FB)(0,l) = 0.0145 +/- 0.0017. Transforming these parameters gives a measurement of the ratio between the decay width into invisible particles and the width to a single species of charged lepton. Gamma (inv)/Gamma (ll) = 5.942 +/- 0.027. Attributing the entire invisible width to neutrino, decays and assuming the Standard Model couplings for neutrinos. this translates into a measurement of the effective number of light neutrino species. N-nu = 2.984 +/- 0.013. Interpreting the data within the context of the Standard Model allows the mass of the top quark, m(t) = (162(-16)(+29)) GeV, to be determined through its influence oil radiative corrections. Alternatively, utilising the direct external measurement of m(t) as an additional constraint leads to a measurement of the strong coupling constant and the mass of the Higgs boson: alpha (s)(m(Z)) = 0.127 +/- 0.005 and m(H) = (390(-280)(+750)) GeV.
引用
收藏
页码:587 / 651
页数:65
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