Search for Yukawa production of a light neutral Higgs boson at LEP

被引:38
作者
Abbiendi, G [1 ]
Ainsley, C
Åkesson, PF
Alexander, G
Allison, J
Anagnostou, G
Anderson, KJ
Arcelli, S
Asai, S
Axen, D
Azuelos, G
Bailey, I
Barberio, E
Barlow, RJ
Batley, RJ
Bechtle, P
Behnke, T
Bell, KW
Bell, PJ
Bella, G
Bellerive, A
Benelli, G
Bethke, S
Biebel, O
Bloodworth, IJ
Boeriu, O
Bock, P
Böhme, J
Bonacorsi, D
Boutemeur, M
Braibant, S
Brigliadori, L
Brown, RM
Burckhart, HJ
Cammin, J
Campana, S
Carnegie, RK
Caron, B
Carter, AA
Carter, JR
Chang, CY
Charlton, DG
Clarke, PEL
Clay, E
Cohen, I
Couchman, J
Csilling, A
Cuffiani, M
Dado, S
Dallavalle, GM
机构
[1] Univ Bologna, Dipartmento Fis, I-40126 Bologna, Italy
[2] CNR, I-40126 Bologna, Italy
[3] Univ Birmingham, Sch Phys & Astron, Birmingham B15 2TT, W Midlands, England
[4] Univ Bonn, Phys Inst, 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] CERN, European Org Nucl Res, CH-1211 Geneva 23, Switzerland
[9] Univ Chicago, Enrico Fermi Inst, Chicago, IL 60637 USA
[10] Univ Chicago, Dept Phys, Chicago, IL 60637 USA
[11] Univ Freiburg, Fak Phys, D-79104 Freiburg, Germany
[12] Univ Heidelberg, Phys Inst, D-69120 Heidelberg, Germany
[13] Indiana Univ, Dept Phys, Bloomington, IN 47405 USA
[14] Univ London Queen Mary & Westfield Coll, London E1 4NS, England
[15] Rhein Westfal TH Aachen, Phys Inst 3, D-52056 Aachen, Germany
[16] UCL, London WC1E 6BT, England
[17] Univ Manchester, Schuster Lab, Dept Phys, Manchester M13 9PL, Lancs, England
[18] Univ Maryland, Dept Phys, College Pk, MD 20742 USA
[19] Univ Montreal, Lab Phys Nucl, Montreal, PQ H3C 3J7, Canada
[20] Univ Oregon, Dept Phys, Eugene, OR 97403 USA
[21] CLRC, Rutherford Appleton Lab, Didcot OX11 0QX, Oxon, England
[22] Technion Israel Inst Technol, Dept Phys, IL-32000 Haifa, Israel
[23] Tel Aviv Univ, Dept Phys & Astron, IL-69978 Tel Aviv, Israel
[24] Univ Tokyo, Int Ctr Elementary Paricle Phys, Tokyo 1130033, Japan
[25] Univ Tokyo, Dept Phys, Tokyo 1130033, Japan
[26] Kobe Univ, Kobe, Hyogo 6578501, Japan
[27] Weizmann Inst Sci, Particle Phys Dept, IL-76100 Rehovot, Israel
[28] Univ Hamburg, DESY, Inst Expt Phys 2, D-22607 Hamburg, Germany
[29] Univ Victoria, Dept Phys, Victoria, BC V8W 3P6, Canada
[30] Univ British Columbia, Dept Phys, Vancouver, BC V6T 1Z1, Canada
[31] Univ Alberta, Dept Phys, Edmonton, AB T6G 2J1, Canada
[32] Res Inst Particle & Nucl Phys, H-1525 Budapest, Hungary
[33] Inst Nucl Res, H-4001 Debrecen, Hungary
[34] Univ Munich, Sekt Phys, D-85748 Garching, Germany
[35] Max Planck Inst Phys & Astrophys, D-80805 Munich, Germany
[36] Yale Univ, Dept Phys, New Haven, CT 06520 USA
来源
EUROPEAN PHYSICAL JOURNAL C | 2002年 / 23卷 / 03期
关键词
D O I
10.1007/s100520200896
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
Within a Two-Higgs-Doublet Model (2HDM) a search for a light Higgs boson in the mass range of 4-12 GeV has been performed in the Yukawa process e(+)e(-) --> b (b) over barA/h --> b (b) over barr(+)r(-), using the data collected by the OPAL detector at LEP between 1992 and 1995 in e(+)e(-) collisions at about 91 GeV centre-of-mass energy. A likelihood selection is applied to separate background and signal. The number of observed events is in good agreement with the expected background. Within a CP-conserving 2HDM type II model the cross-section for Yukawa production depends on epsilon(d)(A) = \tan beta\ and epsilon(d)(h) \sin alpha/cos beta\ for the production of the CP-odd A and the CP-even h, respectively, where tan beta is the ratio of the vacuum expectation values of the Higgs doublets and a is the mixing angle between the neutral CP-even Higgs bosons. From our data 95% C.L. upper limits are derived for epsilon(d)(A) within the range of 8.5 to 13.6 and fur epsilon(d)(h) between 8.2 to 13.7, depending on the mass of the Higgs bosun, assuming a branching fraction into tau(+)tau(-) of 100%. An interpretation of the limits within a 2HDM type II model with Standard Model particle content is given. These results impose constraints on several models that have been proposed to explain the recent BNL measurement of the muon anomalous magnetic moment.
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收藏
页码:397 / 407
页数:11
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