CERN Accelerating science

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000555566 005__ 20211029042622.0
000555566 0247_ $$2DOI$$a10.1140/epjc/s2002-01115-1
000555566 0248_ $$aoai:cds.cern.ch:555566$$pcerncds:hep-ex$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT
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000555566 035__ $$9SLAC$$a4962869
000555566 035__ $$9CERN annual report$$a2003-3.0333
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000555566 035__ $$9Inspire$$a588105
000555566 037__ $$9arXiv$$ahep-ex/0206022$$chep-ex
000555566 037__ $$aCERN-EP-2002-032
000555566 041__ $$aeng
000555566 084__ $$2CERN Library$$aEP-2002-032
000555566 088__ $$9ep-2002-032
000555566 088__ $$aCERN-EP-2002-032
000555566 100__ $$aAbbiendi, G.
000555566 245__ $$aDecay-mode independent searches for new scalar bosons with the OPAL detector at LEP
000555566 260__ $$c2003
000555566 269__ $$aGeneva$$bCERN$$c14 May 2002
000555566 300__ $$a36 p
000555566 340__ $$apaper
000555566 500__ $$arevised version number 1 submitted on 2003-01-13 15:51:05
000555566 500__ $$9arXiv$$a36 pages, 14 figures
000555566 520__ $$aThis paper describes topological searches for neutral scalar bosons S0 produced in association with a Z0 boson via the Bjorken process e+e- -> S0Z0 at centre-of-mass energies of 91 GeV and 183-209 GeV. These searches are based on studies of the recoil mass spectrum of Z0 -> e+e- and mu+mu- events on a search for S0Z0 with Z0 -> nunu bar and S0 -> e+e- or photons. They cover the decays of the S0 into an arbitrary combination of hadrons, leptons, photons and invisible particles as well as the possibility that it might be stable. No indication for a signal is found in the data and upper limits on the cross section of the Bjorken process are calculated. Cross-section limits are given in terms of a scale factor k with respect to the Standrad Model cross section for the Higgs-strahlung process e+e- -> H0smZ0. These results can be interpreted in general scenarios independently of the decay modes of the S0. The examples considered here are the production of a single new scalar particle with a decay width smaller than the detector mass resolution, and for the first time, two scenarios with continuous mass distributions, due to a single very broad state or several states close in mass.
000555566 520__ $$9arXiv$$aThis paper describes topological searches for neutral scalar bosons S0 produced in association with a Z0 boson via the Bjorken process e+e- -> S0Z0 at centre-of-mass energies of 91 GeV and 183-209 GeV. These searches are based on studies of the recoil mass spectrum of Z0 -> e+e- and mu+mu- events on a search for S0Z0 with Z0 -> nunu bar and S0 -> e+e- or photons. They cover the decays of the S0 into an arbitrary combination of hadrons, leptons, photons and invisible particles as well as the possibility that it might be stable. No indication for a signal is found in the data and upper limits on the cross section of the Bjorken process are calculated. Cross-section limits are given in terms of a scale factor k with respect to the Standrad Model cross section for the Higgs-strahlung process e+e- -> H0smZ0. These results can be interpreted in general scenarios independently of the decay modes of the S0. The examples considered here are the production of a single new scalar particle with a decay width smaller than the detector mass resolution, and for the first time, two scenarios with continuous mass distributions, due to a single very broad state or several states close in mass.
000555566 540__ $$3Preprint$$aCC-BY-4.0
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000555566 595__ $$aSIS:2004 PR/LKR added
000555566 595__ $$aaffil a faire
000555566 595__ $$i7660923
000555566 65017 $$2SzGeCERN$$aParticle Physics - Experiment
000555566 6531_ $$9INSPEC$$aBjorken process
000555566 6531_ $$9INSPEC$$aHiggs strahlung
000555566 6531_ $$9INSPEC$$aS0 boson
000555566 6531_ $$9INSPEC$$aS0 decay into positron electron
000555566 6531_ $$9INSPEC$$aZ0 decay into muon muon
000555566 6531_ $$9INSPEC$$aZ0 decay into neutrino antineutrino
000555566 6531_ $$9INSPEC$$aZ0 decay into positron electron
000555566 6531_ $$9INSPEC$$across section
000555566 6531_ $$9INSPEC$$aelectron positron producing H0 Z0
000555566 6531_ $$9INSPEC$$aelectron positron producing S0 Z0
000555566 6531_ $$9INSPEC$$aneutral scalar bosons
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000555566 694__ $$9INSPEC$$aA1480F (Intermediate and Higgs bosons)
000555566 694__ $$9INSPEC$$aA1480K (Other elementary particles)
000555566 694__ $$9INSPEC$$aA1210C (Standard model of unification)
000555566 695__ $$9LANL EDS$$aHigh Energy Physics - Experiment
000555566 695__ $$9INSPEC$$aelectron-positron-inclusive-interactions
000555566 695__ $$9INSPEC$$ahypothetical-particles
000555566 695__ $$9INSPEC$$aintermediate-boson-decay
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000555566 695__ $$9INSPEC$$aleptonic- decays
000555566 695__ $$9INSPEC$$astandard-model
000555566 700__ $$aAinsley, C.
000555566 700__ $$aAkesson, P.F.
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000555566 700__ $$aAllison, John
000555566 700__ $$aAmaral, P.
000555566 700__ $$aAnagnostou, G.
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000555566 700__ $$aArcelli, S.
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000555566 700__ $$aAxen, D.
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000555566 700__ $$aBechtle, P.
000555566 700__ $$aBehnke, T.
000555566 700__ $$aBell, Kenneth Watson
000555566 700__ $$aBell, P.J.
000555566 700__ $$aBella, G.
000555566 700__ $$aBellerive, A.
000555566 700__ $$aBenelli, G.
000555566 700__ $$aBethke, S.
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000555566 700__ $$aBloodworth, I.J.
000555566 700__ $$aBoeriu, O.
000555566 700__ $$aBock, P.
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000555566 700__ $$aBraibant, S.
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000555566 700__ $$aCuffiani, M.
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000555566 773__ $$c311-29$$n3$$pEur. Phys. J. C$$v27$$y2003
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000555566 859__ [email protected]
000555566 8564_ $$uhttp://weblib.cern.ch/abstract?CERN-EP-2002-032$$yPreprint
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000555566 901__ $$uSchool of Physics and Astronomy, Univ. Birmingham
000555566 901__ $$uUniv. Bologna and INFN Bologna
000555566 901__ $$uPhysikalisches Institut, Univ. Bonn
000555566 901__ $$uUniv. Calif. Riverside
000555566 901__ $$uCavendish Lab., Cambridge
000555566 901__ $$uOttawa-Carleton Inst. Phys., Carleton Univ.
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000555566 901__ $$uEnrico Fermi Inst., Univ. Chicago
000555566 901__ $$uFakultat fur Physik, Albert Ludwigs Univ., Freiburg
000555566 901__ $$uPhysikalisches Inst., Univ. Heidelberg
000555566 901__ $$uIndiana Univ., Bloomington
000555566 901__ $$uQueen Mary and Westfield Coll., Univ. London
000555566 901__ $$uTechnische Hochschule Aachen, III Physikalisches Inst., Aachen
000555566 901__ $$uUniv. College London
000555566 901__ $$uSchuster Lab., Manchester
000555566 901__ $$uUniv. Maryland, College Park
000555566 901__ $$uLab. Phys. Nucl., Univ. Montreal
000555566 901__ $$uUniv. Oregon, Eugene
000555566 901__ $$uCLRC Rutherford Appleton Lab., Chilton
000555566 901__ $$uTechnion-Israel Inst. Technol., Haifa
000555566 901__ $$uTel Aviv Univ.
000555566 901__ $$uInt. Centre Elementary Part. Phys., Univ. Tokyo
000555566 901__ $$uKobe Univ.
000555566 901__ $$uWeizmann Inst. Sci., Rehovot
000555566 901__ $$uUniv. Hamburg/DESY
000555566 901__ $$uUniv. Victoria
000555566 901__ $$uUniv. British Columbia, Vancouver
000555566 901__ $$uUniv. Alberta, Edmonton
000555566 901__ $$uRes. Inst. Part. Nucl. Phys., Budapest
000555566 901__ $$uInst. Nucl. Res., Debrecen
000555566 901__ $$uLudwigs-Maximilians-Univ. Munchen
000555566 901__ $$uMax-Planck-Inst. Phys., Munchen
000555566 901__ $$uYale Univ., New Haven
000555566 916__ $$sn$$w200223$$ya2003
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