Flavour-independent h0A0 search and two Higgs doublet model interpretation of neutral Higgs boson searches at LEP

被引:6
|
作者
Abbiendi, G [1 ]
Ainsley, C
Åkesson, PF
Alexander, G
Allison, J
Amaral, P
Anagnostou, G
Anderson, KJ
Asai, S
Axen, D
Bailey, I
Barberio, E
Barillari, T
Barlow, RJ
Batley, RJ
Bechtle, P
Behnke, T
Bell, KW
Bell, PJ
Bella, G
Bellerive, A
Benelli, G
Bethke, S
Biebel, O
Boeriu, O
Bock, P
Boutemeur, M
Braibant, S
Brown, RM
Burckhart, HJ
Campana, S
Capiluppi, P
Carnegie, RK
Carter, AA
Carter, JR
Chang, CY
Charlton, DG
Ciocca, C
Csilling, A
Cuffiani, M
Dado, S
De Roeck, A
De Wolf, EA
Desch, K
Dienes, B
Donkers, M
Dubbert, J
Duchovni, E
Duckeck, G
Duerdoth, IP
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 0H3, England
[7] Carleton Univ, Dept Phys, Ottawa Carleton Inst Phys, Ottawa, ON K1S 5B6, Canada
[8] CERN, European Org Nucl Res, CH-1211 Geneva, 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, Inst Phys, 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] Tech Hsch Aachen, Inst Phys 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, Phys Nucl Lab, Montreal, PQ H3C 3J7, Canada
[20] Univ Oregon, Dept Phys, Eugene, OR 97403 USA
[21] Rutherford Appleton Lab, CCLRC, 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 Particle 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, 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 | 2005年 / 40卷 / 03期
关键词
D O I
10.1140/epjc/s2005-02122-4
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
Upper limits on the cross-section of the pair-production process e(+)e(-) -> h(0)A(0), assuming 100 % branching fraction to hadrons, are derived from a new search for the h(0)A(0) -> hadrons final state, independently of the hadronic flavour of the decay products. This study, combined with previously published searches for the neutral Higgs bosons h(0) and A(0), is used to constrain the Type II Two Higgs Doublet Model (2HDM(II)) with no CP violation in the Higgs sector and no additional non-Standard Model particles besides the five Higgs bosons. The analysis combines LEP1 and LEP2 data collected with the OPAL detector up to the highest available centre-of-mass energies. The searches are sensitive to the h(0), A(0) -> q (q) over bar, gg, tau(+)tau(-) and h(0) -> A(0)A(0) decay modes of the Higgs bosons. A benchmark scan of the 2HDM(II) parameter space is performed. Large regions of the 2HDM( II) parameter space explored are excluded at the 95% CL in the (m(h), m(A)), (m(h), tan beta) and (m(A), tan beta) planes, using both direct neutral Higgs boson searches and indirect limits derived from Standard Model high precision measurements. The region 1 less than or similar to m(h) less than or similar to 55 GeV and 3 less than or similar to m(A) less than or similar to 63 GeV is excluded at 95 % CL, independently of m(h), m(A), tan beta and for selected values of alpha which are representative of a complete alpha-scan.
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收藏
页码:317 / 332
页数:16
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