001501120 001__ 1501120
001501120 005__ 20211222041538.0
001501120 0248_ $$aoai:cds.cern.ch:1501120$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT
001501120 0247_ $$2DOI$$a10.1140/epjc/s10052-013-2463-1
001501120 035__ $$9arXiv$$aoai:arXiv.org:1301.6065
001501120 035__ $$9Inspire$$a1216295
001501120 037__ $$9arXiv$$aarXiv:1301.6065$$chep-ex
001501120 037__ $$aCERN-PH-EP-2012-369
001501120 041__ $$aeng
001501120 088__ $$aCERN-PH-EP-2012-369
001501120 088__ $$9CERN-PH-EP-DRAFT-MISC-2012-010
001501120 088__ $$aLHWG-Note-2012-01
001501120 088__ $$aALEPH-2012-001-PHYSICS-2012-001
001501120 088__ $$aDELPHI-2012-001-PHYS-953
001501120 088__ $$aL3-Note-2835
001501120 088__ $$aOPAL-PR433
001501120 084__ $$2CERN Library$$aPH-EP-2012-369
001501120 100__ $$aAbbiendi, G.$$uBologna U.$$uINFN, Bologna
001501120 110__ $$aCERN. Geneva
001501120 245__ $$aSearch for Charged Higgs bosons: Combined Results Using LEP data
001501120 260__ $$c2013
001501120 269__ $$aGeneva$$bCERN$$c20 Dec 2012
001501120 300__ $$a18 p
001501120 506__ $$mcds-ph-ep-publications-referee-non-lhc [CERN]
001501120 500__ $$aComments: 19 pages, 9 figures
001501120 500__ $$9arXiv$$a17 pages, 8 figures
001501120 520__ $$aThe four LEP collaborations, ALEPH, DELPHI, L3 and OPAL, have searched for pair-produced charged Higgs bosons in the framework of Two Higgs Doublet Models (2HDMs). The data of the four experiments are statistically combined. The results are interpreted within the 2HDM for Type I and Type II benchmark scenarios. No statistically significant excess has been observed when compared to the Standard Model background prediction, and the combined LEP data exclude large regions of the model parameter space. Charged Higgs bosons with mass below 80 GeV/c$^2$ (Type II scenario) or 72.5 GeV/c$^2$ (Type I scenario, for pseudo-scalar masses above 12 GeV/c$^2$) are excluded at the 95% confidence level.
001501120 520__ $$9Springer$$aThe four LEP collaborations, ALEPH, DELPHI, L3 and OPAL, have searched for pair-produced charged Higgs bosons in the framework of Two Higgs Doublet Models (2HDMs). The data of the four experiments have been statistically combined. The results are interpreted within the 2HDM for Type I and Type II benchmark scenarios. No statistically significant excess has been observed when compared to the Standard Model background prediction, and the combined LEP data exclude large regions of the model parameter space. Charged Higgs bosons with mass below 80 (Type II scenario) or 72.5 (Type I scenario, for pseudo-scalar masses above 12 ) are excluded at the 95 % confidence level.
001501120 520__ $$9arXiv$$aThe four LEP collaborations, ALEPH, DELPHI, L3 and OPAL, have searched for pair-produced charged Higgs bosons in the framework of Two Higgs Doublet Models (2HDMs). The data of the four experiments are statistically combined. The results are interpreted within the 2HDM for Type I and Type II benchmark scenarios. No statistically significant excess has been observed when compared to the Standard Model background prediction, and the combined LEP data exclude large regions of the model parameter space. Charged Higgs bosons with mass below 80 GeV/c^2 (Type II scenario) or 72.5 GeV/c^2 (Type I scenario, for pseudo-scalar masses above 12 GeV/c^2) are excluded at the 95% confidence level.
001501120 540__ $$3Preprint$$aCC-BY-3.0
001501120 542__ $$3Preprint$$dCERN$$g2012
001501120 562__ $$cPublic comments
001501120 595__ $$aINSPIRE-PUBL-2013
001501120 595__ $$aCERN-PH-EP
001501120 6531_ $$9CERN$$aHiggs physics
001501120 6531_ $$9CERN$$aexperimental results
001501120 65017 $$2SzGeCERN$$aParticle Physics - Experiment
001501120 65027 $$2arXiv$$aParticle Physics - Phenomenology
001501120 693__ $$aCERN LEP$$eALEPH
001501120 693__ $$aCERN LEP$$eDELPHI
001501120 693__ $$aCERN LEP$$eL3
001501120 693__ $$aCERN LEP$$eOPAL
001501120 690C_ $$aCERN
001501120 690C_ $$aARTICLE
001501120 695__ $$9LANL EDS$$ahep-ex
001501120 695__ $$9LANL EDS$$ahep-ph
001501120 700__ $$aAinsley, C.$$uCambridge U.
001501120 700__ $$aAkesson, P.F.$$uCERN
001501120 700__ $$aAlexander, G.$$uTel Aviv U.
001501120 700__ $$aAnagnostou, G.$$uBirmingham U.
001501120 700__ $$aAnderson, K.J.$$uChicago U., EFI
001501120 700__ $$aAsai, S.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aAxen, D.$$uBritish Columbia U.
001501120 700__ $$aBailey, I.$$uVictoria U.
001501120 700__ $$aBarberio, E.$$uCERN
001501120 700__ $$aBarillari, T.$$uMunich, Max Planck Inst.
001501120 700__ $$aBarlow, R.J.$$uManchester U.
001501120 700__ $$aBatley, R.J.$$uCambridge U.
001501120 700__ $$aBechtle, P.$$uDESY
001501120 700__ $$aBehnke, T.$$uDESY
001501120 700__ $$aBell, K.W.$$uRutherford
001501120 700__ $$aBell, P.J.$$uBirmingham U.
001501120 700__ $$aBella, G.$$uTel Aviv U.
001501120 700__ $$aBellerive, A.$$uCarleton U.
001501120 700__ $$aBenelli, G.$$uUC, Riverside
001501120 700__ $$aBethke, S.$$uMunich, Max Planck Inst.
001501120 700__ $$aBiebel, O.$$uMunich U.
001501120 700__ $$aBoeriu, O.$$uFreiburg U.
001501120 700__ $$aBock, P.$$uHeidelberg U.
001501120 700__ $$aBoutemeur, M.$$uMunich U.
001501120 700__ $$aBraibant, S.$$uINFN, Bologna$$uBologna U.
001501120 700__ $$aBrown, Robert M.$$uRutherford
001501120 700__ $$aBurckhart, H.J.$$uCERN
001501120 700__ $$aCampana, S.$$uUC, Riverside
001501120 700__ $$aCapiluppi, P.$$uINFN, Bologna$$uBologna U.
001501120 700__ $$aCarnegie, R.K.$$uCarleton U.
001501120 700__ $$aCarter, A.A.$$uQueen Mary, U. of London
001501120 700__ $$aCarter, J.R.$$uCambridge U.
001501120 700__ $$aChang, C.Y.$$uMaryland U.
001501120 700__ $$aCharlton, D.G.$$uBirmingham U.
001501120 700__ $$aCiocca, C.$$uINFN, Bologna$$uBologna U.
001501120 700__ $$aCsilling, A.$$uBudapest, RMKI
001501120 700__ $$aCuffiani, M.$$uINFN, Bologna$$uBologna U.
001501120 700__ $$aDado, S.$$uTechnion
001501120 700__ $$aDallavalle, M.$$uINFN, Bologna$$uBologna U.
001501120 700__ $$aDe Roeck, A.$$uCERN
001501120 700__ $$aDe Wolf, E.A.$$uCERN
001501120 700__ $$aDesch, K.$$uDESY
001501120 700__ $$aDienes, B.$$uDebrecen, Inst. Nucl. Res.
001501120 700__ $$aDubbert, J.$$uMunich U.
001501120 700__ $$aDuchovni, E.$$uWeizmann Inst.
001501120 700__ $$aDuckeck, G.$$uMunich U.
001501120 700__ $$aDuerdoth, I.P.$$uManchester U.
001501120 700__ $$aEtzion, E.$$uTel Aviv U.
001501120 700__ $$aFabbri, F.$$uINFN, Bologna$$uBologna U.
001501120 700__ $$aFerrari, P.$$uCERN
001501120 700__ $$aFiedler, F.$$uMunich U.
001501120 700__ $$aFleck, I.$$uFreiburg U.
001501120 700__ $$aFord, M.$$uManchester U.
001501120 700__ $$aFrey, A.$$uCERN
001501120 700__ $$aGagnon, P.$$uIndiana U.
001501120 700__ $$aGary, John William$$uUC, Riverside
001501120 700__ $$aGeich-Gimbel, C.$$uBonn U.
001501120 700__ $$aGiacomelli, G.$$uINFN, Bologna$$uBologna U.
001501120 700__ $$aGiacomelli, P.$$uINFN, Bologna$$uBologna U.
001501120 700__ $$aGiunta, Marina$$uUC, Riverside
001501120 700__ $$aGoldberg, J.$$uTechnion
001501120 700__ $$aGross, E.$$uWeizmann Inst.
001501120 700__ $$aGrunhaus, J.$$uTel Aviv U.
001501120 700__ $$aGruwe, M.$$uCERN
001501120 700__ $$aGupta, A.$$uChicago U., EFI
001501120 700__ $$aHajdu, C.$$uBudapest, RMKI
001501120 700__ $$aHamann, M.$$uDESY
001501120 700__ $$aHanson, G.G.$$uUC, Riverside
001501120 700__ $$aHarel, A.$$uTechnion
001501120 700__ $$aHauschild, M.$$uCERN
001501120 700__ $$aHawkes, C.M.$$uBirmingham U.
001501120 700__ $$aHawkings, R.$$uCERN
001501120 700__ $$aHerten, G.$$uFreiburg U.
001501120 700__ $$aHeuer, R.D.$$uDESY
001501120 700__ $$aHill, J.C.$$uCambridge U.
001501120 700__ $$aHorvath, D.$$uBudapest, RMKI
001501120 700__ $$aIgo-Kemenes, P.$$uHeidelberg U.
001501120 700__ $$aIshii, K.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aJeremie, H.$$uMontreal U.
001501120 700__ $$aJovanovic, P.$$uBirmingham U.
001501120 700__ $$aJunk, T.R.$$uCarleton U.
001501120 700__ $$aKanzaki, J.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aKarlen, D.$$uVictoria U.
001501120 700__ $$aKawagoe, K.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aKawamoto, T.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aKeeler, R.K.$$uVictoria U.
001501120 700__ $$aKellogg, R.G.$$uMaryland U.
001501120 700__ $$aKennedy, B.W.$$uRutherford
001501120 700__ $$aKluth, S.$$uMunich, Max Planck Inst.
001501120 700__ $$aKobayashi, T.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aKobel, M.$$uBonn U.
001501120 700__ $$aKomamiya, S.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aKramer, T.$$uDESY
001501120 700__ $$aKrasznahorkay, A., Jr.$$uDebrecen, Inst. Nucl. Res.
001501120 700__ $$aKrieger, P.$$uCarleton U.
001501120 700__ $$avon Krogh, J.$$uHeidelberg U.
001501120 700__ $$aKuhl, T.$$uDESY
001501120 700__ $$aKupper, M.$$uWeizmann Inst.
001501120 700__ $$aLafferty, G.D.$$uManchester U.
001501120 700__ $$aLandsman, H.$$uTechnion
001501120 700__ $$aLanske, D.$$uAachen, Tech. Hochsch.
001501120 700__ $$aLellouch, D.$$uWeizmann Inst.
001501120 700__ $$aLetts, J.$$uUC, San Diego
001501120 700__ $$aLevinson, L.$$uWeizmann Inst.
001501120 700__ $$aLillich, J.$$uFreiburg U.
001501120 700__ $$aLloyd, S.L.$$uQueen Mary, U. of London
001501120 700__ $$aLoebinger, F.K.$$uManchester U.
001501120 700__ $$aLu, J.$$uBritish Columbia U.
001501120 700__ $$aLudwig, A.$$uBonn U.
001501120 700__ $$aLudwig, J.$$uFreiburg U.
001501120 700__ $$aMader, W.$$uBonn U.
001501120 700__ $$aMarcellini, S.$$uINFN, Bologna$$uBologna U.
001501120 700__ $$aMartin, A.J.$$uQueen Mary, U. of London
001501120 700__ $$aMashimo, T.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aMattig, P.$$uWuppertal U.
001501120 700__ $$aMcKenna, J.$$uBritish Columbia U.
001501120 700__ $$aMcPherson, R.A.$$uVictoria U.
001501120 700__ $$aMeijers, F.$$uCERN
001501120 700__ $$aMenges, W.$$uDESY
001501120 700__ $$aMerritt, F.S.$$uChicago U., EFI
001501120 700__ $$aMes, H.$$uCarleton U.
001501120 700__ $$aMeyer, N.$$uDESY
001501120 700__ $$aMichelini, A.$$uINFN, Bologna$$uBologna U.
001501120 700__ $$aMihara, S.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aMikenberg, G.$$uWeizmann Inst.
001501120 700__ $$aMiller, D.J.$$uUniversity Coll. London
001501120 700__ $$aMohr, W.$$uFreiburg U.
001501120 700__ $$aMori, T.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aMutter, A.$$uFreiburg U.
001501120 700__ $$aNagai, K.$$uQueen Mary, U. of London
001501120 700__ $$aNakamura, I.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aNanjo, H.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aNeal, H.A.$$uYale U.
001501120 700__ $$aO'Neale, S.W.$$uBirmingham U.
001501120 700__ $$aOh, A.$$uCERN
001501120 700__ $$aOkpara, A.$$uHeidelberg U.
001501120 700__ $$aOreglia, M.J.$$uChicago U., EFI
001501120 700__ $$aOrito, S.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aPahl, C.$$uMunich, Max Planck Inst.
001501120 700__ $$aPasztor, G.$$uUC, Riverside
001501120 700__ $$aPater, J.R.$$uManchester U.
001501120 700__ $$aPilcher, J.E.$$uChicago U., EFI
001501120 700__ $$aPinfold, J.$$uAlberta U.
001501120 700__ $$aPlane, D.E.$$uCERN
001501120 700__ $$aPooth, O.$$uAachen, Tech. Hochsch.
001501120 700__ $$aPrzybycien, M.$$uCERN
001501120 700__ $$aQuadt, A.$$uMunich, Max Planck Inst.
001501120 700__ $$aRabbertz, K.$$uCERN
001501120 700__ $$aRembser, C.$$uCERN
001501120 700__ $$aRenkel, P.$$uWeizmann Inst.
001501120 700__ $$aRoney, J.M.$$uVictoria U.
001501120 700__ $$aRossi, A.M.$$uINFN, Bologna$$uBologna U.
001501120 700__ $$aRozen, Y.$$uTechnion
001501120 700__ $$aRunge, K.$$uFreiburg U.
001501120 700__ $$aSachs, K.$$uCarleton U.
001501120 700__ $$aSaeki, T.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aSarkisyan, E.K.G.$$uCERN
001501120 700__ $$aSchaile, A.D.$$uMunich U.
001501120 700__ $$aSchaile, O.$$uMunich U.
001501120 700__ $$aScharff-Hansen, P.$$uCERN
001501120 700__ $$aSchieck, J.$$uMunich, Max Planck Inst.
001501120 700__ $$aSchorner-Sadenius, T.$$uCERN
001501120 700__ $$aSchroder, M.$$uCERN
001501120 700__ $$aSchumacher, M.$$uBonn U.
001501120 700__ $$aSeuster, R.$$uAachen, Tech. Hochsch.
001501120 700__ $$aShears, T.G.$$uCERN
001501120 700__ $$aShen, B.C.$$uUC, Riverside
001501120 700__ $$aSherwood, P.$$uUniversity Coll. London
001501120 700__ $$aSkuja, A.$$uMaryland U.
001501120 700__ $$aSmith, A.M.$$uCERN
001501120 700__ $$aSobie, R.$$uVictoria U.
001501120 700__ $$aSoldner-Rembold, S.$$uManchester U.
001501120 700__ $$aSpano, F.$$uChicago U., EFI
001501120 700__ $$aStahl, A.$$uAachen, Tech. Hochsch.
001501120 700__ $$aStrom, D.$$uOregon U.
001501120 700__ $$aStrohmer, R.$$uMunich U.
001501120 700__ $$aTarem, S.$$uTechnion
001501120 700__ $$aTasevsky, M.$$uCERN
001501120 700__ $$aTeuscher, R.$$uChicago U., EFI
001501120 700__ $$aThomson, M.A.$$uCambridge U.
001501120 700__ $$aTorrence, E.$$uOregon U.
001501120 700__ $$aToya, D.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aTrigger, I.$$uCERN
001501120 700__ $$aTrocsanyi, Z.$$uDebrecen, Inst. Nucl. Res.
001501120 700__ $$aTsur, E.$$uTel Aviv U.
001501120 700__ $$aTurner-Watson, M.F.$$uBirmingham U.
001501120 700__ $$aUeda, I.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aUjvari, B.$$uDebrecen, Inst. Nucl. Res.
001501120 700__ $$aVollmer, C.F.$$uMunich U.
001501120 700__ $$aVannerem, P.$$uFreiburg U.
001501120 700__ $$aVertesi, R.$$uDebrecen, Inst. Nucl. Res.
001501120 700__ $$aVerzocchi, M.$$uMaryland U.
001501120 700__ $$aVoss, H.$$uCERN
001501120 700__ $$aVossebeld, J.$$uCERN
001501120 700__ $$aWard, C.P.$$uCambridge U.
001501120 700__ $$aWard, D.R.$$uCambridge U.
001501120 700__ $$aWatkins, P.M.$$uBirmingham U.
001501120 700__ $$aWatson, A.T.$$uBirmingham U.
001501120 700__ $$aWatson, N.K.$$uBirmingham U.
001501120 700__ $$aWells, P.S.$$uCERN
001501120 700__ $$aWengler, T.$$uCERN
001501120 700__ $$aWermes, N.$$uBonn U.
001501120 700__ $$aWilson, G.W.$$uManchester U.
001501120 700__ $$aWilson, J.A.$$uBirmingham U.
001501120 700__ $$aWolf, G.$$uWeizmann Inst.
001501120 700__ $$aWyatt, T.R.$$uManchester U.
001501120 700__ $$aYamashita, S.$$uKobe U.$$uTokyo U., ICEPP
001501120 700__ $$aZer-Zion, D.$$uUC, Riverside
001501120 700__ $$aZivkovic, Lidija$$iINSPIRE-00057284$$uTechnion
001501120 700__ $$aAbdallah, J.
001501120 700__ $$aAbreu, P.
001501120 700__ $$aAdam, W.
001501120 700__ $$aAdzic, P.
001501120 700__ $$aAlbrecht, T.
001501120 700__ $$aAlderweireld, T.
001501120 700__ $$aAlemany-Fernandez, R.
001501120 700__ $$aAllmendinger, T.
001501120 700__ $$aAllport, P.P.
001501120 700__ $$aAmaldi, U.
001501120 700__ $$aAmapane, N.
001501120 700__ $$aAmato, S.
001501120 700__ $$aAnashkin, E.
001501120 700__ $$aAndreazza, A.
001501120 700__ $$aAndringa, S.
001501120 700__ $$aAnjos, N.
001501120 700__ $$aAntilogus, P.
001501120 700__ $$aApel, W.D.
001501120 700__ $$aArnoud, Y.
001501120 700__ $$aAsk, S.
001501120 700__ $$aAsman, B.
001501120 700__ $$aAugustin, J.E.
001501120 700__ $$aAugustinus, A.
001501120 700__ $$aBaillon, P.
001501120 700__ $$aBallestrero, A.
001501120 700__ $$aBambade, P.
001501120 700__ $$aBarbier, R.
001501120 700__ $$aBardin, D.
001501120 700__ $$aBarker, G.
001501120 700__ $$aBaroncelli, A.
001501120 700__ $$aBattaglia, M.
001501120 700__ $$aBaubillier, M.
001501120 700__ $$aBecks, K.H.
001501120 700__ $$aBegalli, M.
001501120 700__ $$aBehrmann, A.
001501120 700__ $$aBen-Haim, E.
001501120 700__ $$aBenekos, N.
001501120 700__ $$aBenvenuti, A.
001501120 700__ $$aBerat, C.
001501120 700__ $$aBerggren, M.
001501120 700__ $$aBerntzon, L.
001501120 700__ $$aBertrand, D.
001501120 700__ $$aBesancon, M.
001501120 700__ $$aBesson, N.
001501120 700__ $$aBloch, D.
001501120 700__ $$aBlom, M.
001501120 700__ $$aBluj, M.
001501120 700__ $$aBonesini, M.
001501120 700__ $$aBoonekamp, M.
001501120 700__ $$aBooth, P.S.L.
001501120 700__ $$aBorisov, G.
001501120 700__ $$aBotner, O.
001501120 700__ $$aBouquet, B.
001501120 700__ $$aBowcock, T.J.V.
001501120 700__ $$aBoyko, I.
001501120 700__ $$aBracko, M.
001501120 700__ $$aBrenner, R.
001501120 700__ $$aBrodet, E.
001501120 700__ $$aBruckman, P.
001501120 700__ $$aBrunet, J.M.
001501120 700__ $$aBugge, L.
001501120 700__ $$aBuschmann, P.
001501120 700__ $$aCalvi, M.
001501120 700__ $$aCamporesi, T.
001501120 700__ $$aCanale, V.
001501120 700__ $$aCarena, F.
001501120 700__ $$aCastro, Nuno Filipe$$iINSPIRE-00036257
001501120 700__ $$aCavallo, F.
001501120 700__ $$aChapkin, M.
001501120 700__ $$aCharpentier, Ph.
001501120 700__ $$aChecchia, P.
001501120 700__ $$aChierici, R.
001501120 700__ $$aChliapnikov, P.
001501120 700__ $$aChudoba, J.
001501120 700__ $$aChung, S.U.
001501120 700__ $$aCieslik, K.
001501120 700__ $$aCollins, P.
001501120 700__ $$aContri, R.
001501120 700__ $$aCosme, G.
001501120 700__ $$aCossutti, F.
001501120 700__ $$aCosta, M.J.
001501120 700__ $$aCrennell, D.
001501120 700__ $$aCuevas, J.
001501120 700__ $$aD'Hondt, J.
001501120 700__ $$aDalmau, J.
001501120 700__ $$ada Silva, T.
001501120 700__ $$aDa Silva, W.
001501120 700__ $$aDella Ricca, G.
001501120 700__ $$aDe Angelis, A.
001501120 700__ $$aDe Boer, W.
001501120 700__ $$aDe Clercq, C.
001501120 700__ $$aDe Lotto, B.
001501120 700__ $$aDe Maria, N.
001501120 700__ $$aDe Min, A.
001501120 700__ $$ade Paula, L.
001501120 700__ $$aDi Ciaccio, L.
001501120 700__ $$aDi Simone, A.
001501120 700__ $$aDoroba, K.
001501120 700__ $$aDrees, J.
001501120 700__ $$aDris, M.
001501120 700__ $$aEigen, G.
001501120 700__ $$aEkelof, T.
001501120 700__ $$aEllert, M.
001501120 700__ $$aElsing, M.
001501120 700__ $$aEspirito Santo, M.C.
001501120 700__ $$aFanourakis, G.
001501120 700__ $$aFassouliotis, D.
001501120 700__ $$aFeindt, M.
001501120 700__ $$aFernandez, J.
001501120 700__ $$aFerrer, A.
001501120 700__ $$aFerro, F.
001501120 700__ $$aFlagmeyer, U.
001501120 700__ $$aFoeth, H.
001501120 700__ $$aFokitis, E.
001501120 700__ $$aFulda-Quenzer, F.
001501120 700__ $$aFuster, J.
001501120 700__ $$aGandelman, M.
001501120 700__ $$aGarcia, C.
001501120 700__ $$aGavillet, Ph.
001501120 700__ $$aGazis, Evangelos
001501120 700__ $$aGokieli, R.
001501120 700__ $$aGolob, B.
001501120 700__ $$aGomez-Ceballos, G.
001501120 700__ $$aGoncalves, P.
001501120 700__ $$aGraziani, E.
001501120 700__ $$aGrosdidier, G.
001501120 700__ $$aGrzelak, K.
001501120 700__ $$aGuy, J.
001501120 700__ $$aHaag, C.
001501120 700__ $$aHallgren, A.
001501120 700__ $$aHamacher, K.
001501120 700__ $$aHamilton, K.
001501120 700__ $$aHaug, S.
001501120 700__ $$aHauler, F.
001501120 700__ $$aHedberg, V.
001501120 700__ $$aHennecke, M.
001501120 700__ $$aHerr, H.
001501120 700__ $$aHoffman, J.
001501120 700__ $$aHolmgren, S.O.
001501120 700__ $$aHolt, P.J.
001501120 700__ $$aHoulden, M.A.
001501120 700__ $$aHultqvist, K.
001501120 700__ $$aJackson, John Neil
001501120 700__ $$aJarlskog, G.
001501120 700__ $$aJarry, P.
001501120 700__ $$aJeans, D.
001501120 700__ $$aJohansson, Erik Karl
001501120 700__ $$aJohansson, P.D.
001501120 700__ $$aJonsson, P.
001501120 700__ $$aJoram, C.
001501120 700__ $$aJungermann, L.
001501120 700__ $$aKapusta, Frederic
001501120 700__ $$aKatsanevas, S.
001501120 700__ $$aKatsoufis, E.
001501120 700__ $$aKernel, G.
001501120 700__ $$aKersevan, B.P.
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001501120 700__ $$aWang, X.L.
001501120 700__ $$aWang, Z.M.
001501120 700__ $$aWeber, M.
001501120 700__ $$aWienemann, P.
001501120 700__ $$aWilkens, H.
001501120 700__ $$aWynhoff, S.
001501120 700__ $$aXia, L.
001501120 700__ $$aXu, Z.Z.
001501120 700__ $$aYamamoto, J.
001501120 700__ $$aYang, B.Z.
001501120 700__ $$aYang, C.G.
001501120 700__ $$aYang, H.J.
001501120 700__ $$aYang, M.
001501120 700__ $$aYeh, S.C.
001501120 700__ $$aZalite, A.
001501120 700__ $$aZalite, Yu.
001501120 700__ $$aZhang, Z.P.
001501120 700__ $$aZhao, J.
001501120 700__ $$aZhu, G.Y.
001501120 700__ $$aZhu, R.Y.
001501120 700__ $$aZhuang, H.L.
001501120 700__ $$aZichichi, A.
001501120 700__ $$aZimmermann, B.
001501120 700__ $$aZoller, M.
001501120 700__ $$aHeister, A.$$uAachen, Tech. Hochsch.
001501120 700__ $$aSchael, S.$$uAachen, Tech. Hochsch.
001501120 700__ $$aBarate, R.$$uAnnecy, LAPP
001501120 700__ $$aBruneliere, R.$$uAnnecy, LAPP
001501120 700__ $$aDe Bonis, I.$$uAnnecy, LAPP
001501120 700__ $$aDecamp, D.$$uAnnecy, LAPP
001501120 700__ $$aGoy, C.$$uAnnecy, LAPP
001501120 700__ $$aJezequel, S.$$uAnnecy, LAPP
001501120 700__ $$aLees, J.P.$$uAnnecy, LAPP
001501120 700__ $$aMartin, F.$$uAnnecy, LAPP
001501120 700__ $$aMerle, E.$$uAnnecy, LAPP
001501120 700__ $$aMinard, M.N.$$uAnnecy, LAPP
001501120 700__ $$aPietrzyk, B.$$uAnnecy, LAPP
001501120 700__ $$aTrocme, B.$$uAnnecy, LAPP
001501120 700__ $$aBoix, G.$$uBarcelona, IFAE
001501120 700__ $$aBravo, S.$$uBarcelona, IFAE
001501120 700__ $$aCasado, M.P.$$uBarcelona, IFAE
001501120 700__ $$aChmeissani, M.$$uBarcelona, IFAE
001501120 700__ $$aCrespo, J.M.$$uBarcelona, IFAE
001501120 700__ $$aFernandez, E.$$uBarcelona, IFAE
001501120 700__ $$aFernandez-Bosman, M.$$uBarcelona, IFAE
001501120 700__ $$aGarrido, Ll.$$uBarcelona, IFAE
001501120 700__ $$aGrauges, E.$$uBarcelona, IFAE
001501120 700__ $$aLopez, J.$$uBarcelona, IFAE
001501120 700__ $$aMartinez, M.$$uBarcelona, IFAE
001501120 700__ $$aMerino, G.$$uBarcelona, IFAE
001501120 700__ $$aPacheco, A.$$uBarcelona, IFAE
001501120 700__ $$aPaneque, D.$$uBarcelona, IFAE
001501120 700__ $$aRuiz, H.$$uBarcelona, IFAE
001501120 700__ $$aColaleo, A.$$uINFN, Bari$$uBari U.
001501120 700__ $$aCreanza, D.$$uINFN, Bari$$uBari U.
001501120 700__ $$aDe Filippis, N.$$uINFN, Bari$$uBari U.
001501120 700__ $$ade Palma, M.$$uINFN, Bari$$uBari U.
001501120 700__ $$aIaselli, G.$$uINFN, Bari$$uBari U.
001501120 700__ $$aMaggi, G.$$uINFN, Bari$$uBari U.
001501120 700__ $$aMaggi, M.$$uINFN, Bari$$uBari U.
001501120 700__ $$aNuzzo, S.$$uINFN, Bari$$uBari U.
001501120 700__ $$aRanieri, A.$$uINFN, Bari$$uBari U.
001501120 700__ $$aRaso, G.$$uINFN, Bari$$uBari U.
001501120 700__ $$aRuggieri, F.$$uINFN, Bari$$uBari U.
001501120 700__ $$aSelvaggi, G.$$uINFN, Bari$$uBari U.
001501120 700__ $$aSilvestris, L.$$uINFN, Bari$$uBari U.
001501120 700__ $$aTempesta, P.$$uINFN, Bari$$uBari U.
001501120 700__ $$aTricomi, A.$$uINFN, Bari$$uBari U.
001501120 700__ $$aZito, G.$$uINFN, Bari$$uBari U.
001501120 700__ $$aHuang, X.$$uBeijing, Inst. High Energy Phys.
001501120 700__ $$aLin, J.$$uBeijing, Inst. High Energy Phys.
001501120 700__ $$aOuyang, Q.$$uBeijing, Inst. High Energy Phys.
001501120 700__ $$aWang, T.$$uBeijing, Inst. High Energy Phys.
001501120 700__ $$aXie, Y.$$uBeijing, Inst. High Energy Phys.
001501120 700__ $$aXu, R.$$uBeijing, Inst. High Energy Phys.
001501120 700__ $$aXue, S.$$uBeijing, Inst. High Energy Phys.
001501120 700__ $$aZhang, J.$$uBeijing, Inst. High Energy Phys.
001501120 700__ $$aZhang, L.$$uBeijing, Inst. High Energy Phys.
001501120 700__ $$aZhao, W.$$uBeijing, Inst. High Energy Phys.
001501120 700__ $$aAbbaneo, D.$$uCERN
001501120 700__ $$aAzzurri, P.$$uCERN
001501120 700__ $$aBarklow, T.$$uCERN
001501120 700__ $$aBuchmuller, O.$$uCERN
001501120 700__ $$aCattaneo, M.$$uCERN
001501120 700__ $$aCerutti, F.$$uCERN
001501120 700__ $$aClerbaux, B.$$uCERN
001501120 700__ $$aDrevermann, H.$$uCERN
001501120 700__ $$aForty, R.W.$$uCERN
001501120 700__ $$aFrank, M.$$uCERN
001501120 700__ $$aGianotti, F.$$uCERN
001501120 700__ $$aGreening, T.C.$$uCERN
001501120 700__ $$aHansen, J.B.$$uCERN
001501120 700__ $$aHarvey, J.$$uCERN
001501120 700__ $$aHutchcroft, D.E.$$uCERN
001501120 700__ $$aJanot, P.$$uCERN
001501120 700__ $$aJost, B.$$uCERN
001501120 700__ $$aKado, M.$$uCERN
001501120 700__ $$aMato, P.$$uCERN
001501120 700__ $$aMoutoussi, A.$$uCERN
001501120 700__ $$aRanjard, F.$$uCERN
001501120 700__ $$aRolandi, Gigi$$uCERN
001501120 700__ $$aSchlatter, D.$$uCERN
001501120 700__ $$aSguazzoni, G.$$uCERN
001501120 700__ $$aTejessy, W.$$uCERN
001501120 700__ $$aTeubert, F.$$uCERN
001501120 700__ $$aValassi, A.$$uCERN
001501120 700__ $$aVideau, I.$$uCERN
001501120 700__ $$aWard, J.J.$$uCERN
001501120 700__ $$aBadaud, F.$$uClermont-Ferrand U.
001501120 700__ $$aDessagne, S.$$uClermont-Ferrand U.
001501120 700__ $$aFalvard, A.$$uClermont-Ferrand U.
001501120 700__ $$aFayolle, D.$$uClermont-Ferrand U.
001501120 700__ $$aGay, P.$$uClermont-Ferrand U.
001501120 700__ $$aJousset, J.$$uClermont-Ferrand U.
001501120 700__ $$aMichel, B.$$uClermont-Ferrand U.
001501120 700__ $$aMonteil, S.$$uClermont-Ferrand U.
001501120 700__ $$aPallin, D.$$uClermont-Ferrand U.
001501120 700__ $$aPascolo, J.M.$$uClermont-Ferrand U.
001501120 700__ $$aPerret, P.$$uClermont-Ferrand U.
001501120 700__ $$aHansen, J.D.$$uBohr Inst.
001501120 700__ $$aHansen, J.R.$$uBohr Inst.
001501120 700__ $$aHansen, P.H.$$uBohr Inst.
001501120 700__ $$aNilsson, B.S.$$uBohr Inst.
001501120 700__ $$aKyriakis, A.$$uDemocritos Nucl. Res. Ctr.
001501120 700__ $$aMarkou, C.$$uDemocritos Nucl. Res. Ctr.
001501120 700__ $$aSimopoulou, E.$$uDemocritos Nucl. Res. Ctr.
001501120 700__ $$aVayaki, A.$$uDemocritos Nucl. Res. Ctr.
001501120 700__ $$aZachariadou, K.$$uDemocritos Nucl. Res. Ctr.
001501120 700__ $$aBlondel, A.$$uEcole Polytechnique
001501120 700__ $$aBrient, J.C.$$uEcole Polytechnique
001501120 700__ $$aMachefert, F.$$uEcole Polytechnique
001501120 700__ $$aRouge, A.$$uEcole Polytechnique
001501120 700__ $$aSwynghedauw, M.$$uEcole Polytechnique
001501120 700__ $$aTanaka, R.$$uEcole Polytechnique
001501120 700__ $$aVideau, H.$$uEcole Polytechnique
001501120 700__ $$aCiulli, V.$$uINFN, Florence$$uFlorence U.
001501120 700__ $$aFocardi, E.$$uINFN, Florence$$uFlorence U.
001501120 700__ $$aParrini, G.$$uINFN, Florence$$uFlorence U.
001501120 700__ $$aAntonelli, A.$$uFrascati
001501120 700__ $$aAntonelli, M.$$uFrascati
001501120 700__ $$aBencivenni, G.$$uFrascati
001501120 700__ $$aBossi, F.$$uFrascati
001501120 700__ $$aCapon, G.$$uFrascati
001501120 700__ $$aChiarella, V.$$uFrascati
001501120 700__ $$aLaurelli, P.$$uFrascati
001501120 700__ $$aMannocchi, G.$$uFrascati
001501120 700__ $$aMurtas, G.P.$$uFrascati
001501120 700__ $$aPassalacqua, L.$$uFrascati
001501120 700__ $$aKennedy, J.$$uGlasgow U.
001501120 700__ $$aLynch, J.G.$$uGlasgow U.
001501120 700__ $$aNegus, P.$$uGlasgow U.
001501120 700__ $$aO'Shea, V.$$uGlasgow U.
001501120 700__ $$aThompson, A.S.$$uGlasgow U.
001501120 700__ $$aWasserbaech, S.$$uHaverford Coll.
001501120 700__ $$aCavanaugh, R.$$uKirchhoff Inst. Phys.
001501120 700__ $$aDhamotharan, S.$$uKirchhoff Inst. Phys.
001501120 700__ $$aGeweniger, C.$$uKirchhoff Inst. Phys.
001501120 700__ $$aHanke, P.$$uKirchhoff Inst. Phys.
001501120 700__ $$aHepp, V.$$uKirchhoff Inst. Phys.
001501120 700__ $$aKluge, E.E.$$uKirchhoff Inst. Phys.
001501120 700__ $$aLeibenguth, G.$$uKirchhoff Inst. Phys.
001501120 700__ $$aPutzer, A.$$uKirchhoff Inst. Phys.
001501120 700__ $$aStenzel, H.$$uKirchhoff Inst. Phys.
001501120 700__ $$aTittel, K.$$uKirchhoff Inst. Phys.
001501120 700__ $$aWunsch, M.$$uKirchhoff Inst. Phys.
001501120 700__ $$aBeuselinck, R.$$uImperial Coll., London
001501120 700__ $$aCameron, W.$$uImperial Coll., London
001501120 700__ $$aDavies, G.$$uImperial Coll., London
001501120 700__ $$aDornan, P.J.$$uImperial Coll., London
001501120 700__ $$aGirone, M.$$uImperial Coll., London
001501120 700__ $$aHill, R.D.$$uImperial Coll., London
001501120 700__ $$aMarinelli, N.$$uImperial Coll., London
001501120 700__ $$aNowell, J.$$uImperial Coll., London
001501120 700__ $$aRutherford, S.A.$$uImperial Coll., London
001501120 700__ $$aSedgbeer, J.K.$$uImperial Coll., London
001501120 700__ $$aThompson, J.C.$$uImperial Coll., London
001501120 700__ $$aWhite, R.$$uImperial Coll., London
001501120 700__ $$aGhete, V.M.$$uInnsbruck U.
001501120 700__ $$aGirtler, P.$$uInnsbruck U.
001501120 700__ $$aKneringer, E.$$uInnsbruck U.
001501120 700__ $$aKuhn, D.$$uInnsbruck U.
001501120 700__ $$aRudolph, G.$$uInnsbruck U.
001501120 700__ $$aBouhova-Thacker, E.$$uLancaster U.
001501120 700__ $$aBowdery, C.K.$$uLancaster U.
001501120 700__ $$aClarke, D.P.$$uLancaster U.
001501120 700__ $$aEllis, G.$$uLancaster U.
001501120 700__ $$aFinch, A.J.$$uLancaster U.
001501120 700__ $$aFoster, F.$$uLancaster U.
001501120 700__ $$aHughes, G.$$uLancaster U.
001501120 700__ $$aJones, R.W.L.$$uLancaster U.
001501120 700__ $$aPearson, M.R.$$uLancaster U.
001501120 700__ $$aRobertson, N.A.$$uLancaster U.
001501120 700__ $$aSmizanska, M.$$uLancaster U.
001501120 700__ $$avan der Aa, O.$$uLouvain U., Inst. Phys. Nucl.
001501120 700__ $$aDelaere, C.$$uLouvain U., Inst. Phys. Nucl.
001501120 700__ $$aLemaitre, V.$$uLouvain U., Inst. Phys. Nucl.
001501120 700__ $$aBlumenschein, U.$$uMainz U., Inst. Phys.
001501120 700__ $$aHolldorfer, F.$$uMainz U., Inst. Phys.
001501120 700__ $$aJakobs, K.$$uMainz U., Inst. Phys.
001501120 700__ $$aKayser, F.$$uMainz U., Inst. Phys.
001501120 700__ $$aKleinknecht, K.$$uMainz U., Inst. Phys.
001501120 700__ $$aMuller, A.S.$$uMainz U., Inst. Phys.
001501120 700__ $$aQuast, G.$$uMainz U., Inst. Phys.
001501120 700__ $$aRenk, B.$$uMainz U., Inst. Phys.
001501120 700__ $$aSander, H.G.$$uMainz U., Inst. Phys.
001501120 700__ $$aSchmeling, S.$$uMainz U., Inst. Phys.
001501120 700__ $$aWachsmuth, H.$$uMainz U., Inst. Phys.
001501120 700__ $$aZeitnitz, C.$$uMainz U., Inst. Phys.
001501120 700__ $$aZiegler, T.$$uMainz U., Inst. Phys.
001501120 700__ $$aBonissent, A.$$uMarseille, CPPM
001501120 700__ $$aCoyle, P.$$uMarseille, CPPM
001501120 700__ $$aCurtil, C.$$uMarseille, CPPM
001501120 700__ $$aEalet, A.$$uMarseille, CPPM
001501120 700__ $$aFouchez, D.$$uMarseille, CPPM
001501120 700__ $$aPayre, P.$$uMarseille, CPPM
001501120 700__ $$aTilquin, A.$$uMarseille, CPPM
001501120 700__ $$aRagusa, F.$$uINFN, Milan$$uMilan U.
001501120 700__ $$aDavid, A.$$uMunich, Max Planck Inst.
001501120 700__ $$aDietl, H.$$uMunich, Max Planck Inst.
001501120 700__ $$aGanis, G.$$uMunich, Max Planck Inst.
001501120 700__ $$aHuttmann, K.$$uMunich, Max Planck Inst.
001501120 700__ $$aLutjens, G.$$uMunich, Max Planck Inst.
001501120 700__ $$aManner, W.$$uMunich, Max Planck Inst.
001501120 700__ $$aMoser, H.G.$$uMunich, Max Planck Inst.
001501120 700__ $$aSettles, R.$$uMunich, Max Planck Inst.
001501120 700__ $$aWolf, G.$$uMunich, Max Planck Inst.
001501120 700__ $$aBoucrot, J.$$uOrsay, LAL
001501120 700__ $$aCallot, O.$$uOrsay, LAL
001501120 700__ $$aDavier, M.$$uOrsay, LAL
001501120 700__ $$aDuflot, L.$$uOrsay, LAL
001501120 700__ $$aGrivaz, J.F.$$uOrsay, LAL
001501120 700__ $$aHeusse, P.$$uOrsay, LAL
001501120 700__ $$aJacholkowska, A.$$uOrsay, LAL
001501120 700__ $$aSerin, L.$$uOrsay, LAL
001501120 700__ $$aVeillet, J.J.$$uOrsay, LAL
001501120 700__ $$ade Vivie de Regie, J.B.$$uOrsay, LAL
001501120 700__ $$aYuan, C.$$uOrsay, LAL
001501120 700__ $$aBagliesi, Giuseppe$$uPisa, Scuola Normale Superiore$$uINFN, Pisa$$uPisa U.
001501120 700__ $$aBoccali, T.$$uPisa, Scuola Normale Superiore$$uINFN, Pisa$$uPisa U.
001501120 700__ $$aFoa, L.$$uPisa, Scuola Normale Superiore$$uINFN, Pisa$$uPisa U.
001501120 700__ $$aGiammanco, A.$$uPisa, Scuola Normale Superiore$$uINFN, Pisa$$uPisa U.
001501120 700__ $$aGiassi, A.$$uPisa, Scuola Normale Superiore$$uINFN, Pisa$$uPisa U.
001501120 700__ $$aLigabue, F.$$uPisa, Scuola Normale Superiore$$uINFN, Pisa$$uPisa U.
001501120 700__ $$aMessineo, A.$$uPisa, Scuola Normale Superiore$$uINFN, Pisa$$uPisa U.
001501120 700__ $$aPalla, F.$$uPisa, Scuola Normale Superiore$$uINFN, Pisa$$uPisa U.
001501120 700__ $$aSanguinetti, G.$$uPisa, Scuola Normale Superiore$$uINFN, Pisa$$uPisa U.
001501120 700__ $$aSciaba, A.$$uPisa, Scuola Normale Superiore$$uINFN, Pisa$$uPisa U.
001501120 700__ $$aTenchini, R.$$uPisa, Scuola Normale Superiore$$uINFN, Pisa$$uPisa U.
001501120 700__ $$aVenturi, A.$$uPisa, Scuola Normale Superiore$$uINFN, Pisa$$uPisa U.
001501120 700__ $$aVerdini, P.G.$$uPisa, Scuola Normale Superiore$$uINFN, Pisa$$uPisa U.
001501120 700__ $$aAwunor, O.$$uRoyal Holloway, U. of London
001501120 700__ $$aBlair, G.A.$$uRoyal Holloway, U. of London
001501120 700__ $$aCowan, G.$$uRoyal Holloway, U. of London
001501120 700__ $$aGarcia-Bellido, A.$$uRoyal Holloway, U. of London
001501120 700__ $$aGreen, M.G.$$uRoyal Holloway, U. of London
001501120 700__ $$aJones, L.T.$$uRoyal Holloway, U. of London
001501120 700__ $$aMedcalf, T.$$uRoyal Holloway, U. of London
001501120 700__ $$aMisiejuk, A.$$uRoyal Holloway, U. of London
001501120 700__ $$aStrong, J.A.$$uRoyal Holloway, U. of London
001501120 700__ $$aTeixeira-Dias, P.$$uRoyal Holloway, U. of London
001501120 700__ $$aClifft, R.W.$$uRutherford
001501120 700__ $$aEdgecock, T.R.$$uRutherford
001501120 700__ $$aNorton, P.R.$$uRutherford
001501120 700__ $$aTomalin, I.R.$$uRutherford
001501120 700__ $$aBloch-Devaux, Brigitte$$uDAPNIA, Saclay
001501120 700__ $$aBoumediene, D.$$uDAPNIA, Saclay
001501120 700__ $$aColas, P.$$uDAPNIA, Saclay
001501120 700__ $$aFabbro, B.$$uDAPNIA, Saclay
001501120 700__ $$aLancon, E.$$uDAPNIA, Saclay
001501120 700__ $$aLemaire, M.C.$$uDAPNIA, Saclay
001501120 700__ $$aLocci, E.$$uDAPNIA, Saclay
001501120 700__ $$aPerez, P.$$uDAPNIA, Saclay
001501120 700__ $$aRander, J.$$uDAPNIA, Saclay
001501120 700__ $$aTuchming, B.$$uDAPNIA, Saclay
001501120 700__ $$aVallage, B.$$uDAPNIA, Saclay
001501120 700__ $$aKonstantinidis, N.$$uUC, Santa Cruz
001501120 700__ $$aLitke, A.M.$$uUC, Santa Cruz
001501120 700__ $$aTaylor, G.$$uUC, Santa Cruz
001501120 700__ $$aBooth, C.N.$$uSheffield U.
001501120 700__ $$aCartwright, S.$$uSheffield U.
001501120 700__ $$aCombley, F.$$uSheffield U.
001501120 700__ $$aHodgson, P.N.$$uSheffield U.
001501120 700__ $$aLehto, M.$$uSheffield U.
001501120 700__ $$aThompson, L.F.$$uSheffield U.
001501120 700__ $$aBoehrer, Armin$$uSiegen U.
001501120 700__ $$aBrandt, S.$$uSiegen U.
001501120 700__ $$aGrupen, C.$$uSiegen U.
001501120 700__ $$aHess, J.$$uSiegen U.
001501120 700__ $$aNgac, A.$$uSiegen U.
001501120 700__ $$aPrange, G.$$uSiegen U.
001501120 700__ $$aSieler, U.$$uSiegen U.
001501120 700__ $$aBorean, C.$$uINFN, Trieste$$uTrieste U.
001501120 700__ $$aGiannini, G.$$uINFN, Trieste$$uTrieste U.
001501120 700__ $$aHe, H.$$uWashington U., Seattle
001501120 700__ $$aPutz, J.$$uWashington U., Seattle
001501120 700__ $$aRothberg, J.$$uWashington U., Seattle
001501120 700__ $$aArmstrong, S.R.$$uWisconsin U., Madison
001501120 700__ $$aBerkelman, Karl$$uWisconsin U., Madison
001501120 700__ $$aCranmer, K.$$uWisconsin U., Madison
001501120 700__ $$aFerguson, D.P.S.$$uWisconsin U., Madison
001501120 700__ $$aGao, Y.$$uWisconsin U., Madison
001501120 700__ $$aGonzalez, S.$$uWisconsin U., Madison
001501120 700__ $$aHayes, O.J.$$uWisconsin U., Madison
001501120 700__ $$aHu, H.$$uWisconsin U., Madison
001501120 700__ $$aJin, S.$$uWisconsin U., Madison
001501120 700__ $$aKile, J.$$uWisconsin U., Madison
001501120 700__ $$aMcNamara, P.A., III$$uWisconsin U., Madison
001501120 700__ $$aNielsen, J.$$uWisconsin U., Madison
001501120 700__ $$aPan, Y.B.$$uWisconsin U., Madison
001501120 700__ $$avon Wimmersperg-Toeller, J.H.$$uWisconsin U., Madison
001501120 700__ $$aWiedenmann, W.$$uWisconsin U., Madison
001501120 700__ $$aWu, J.$$uWisconsin U., Madison
001501120 700__ $$aWu, Sau Lan$$uWisconsin U., Madison
001501120 700__ $$aWu, X.$$uWisconsin U., Madison
001501120 700__ $$aZobernig, G.$$uWisconsin U., Madison
001501120 700__ $$aDissertori, G.$$uZurich, ETH
001501120 700__ $$aHeinemeyer, S.
001501120 710__ $$gALEPH, DELPHI, L3 and OPAL Collaborations
001501120 710__ $$5PH-EP
001501120 710__ $$gLEP working group for Higgs boson searches
001501120 773__ $$c2463$$pEur. Phys. J. C$$v73$$y2013
001501120 859__ [email protected]
001501120 8564_ $$8745155$$s414591$$uhttps://cds.cern.ch/record/1501120/files/CERN-PH-EP-2012-369.pdf$$zMoved stamp
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001501120 8564_ $$uhttp://arxiv.org/pdf/1301.6065.pdf$$yPreprint
001501120 8564_ $$8763789$$s34264$$uhttps://cds.cern.ch/record/1501120/files/fig1.png$$y00002 \small \it Type II 2HDM: contours based on the observed p-values $CL_b$ as a function of \mHpm\ and the branching ratio Br(\Hp\ra\tp$\nu$), indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$8763787$$s22791$$uhttps://cds.cern.ch/record/1501120/files/fig2.png$$y00003 \small \it Type II 2HDM: excluded regions in the Br(\Hp\ra\tp$\nu$) vs \mHpm\ plane, based on the combined data collected by the four LEP experiments at centre-of-mass energies from 183 to 209~GeV. The shaded area is excluded at the 95\% or higher C.L. The expected exclusion limit (at the 95\% C.L.) is indicated by the thin solid line and the thick dotted line inside the shaded area is the observed limit at the 99.7\% C.L.Caption not extracted
001501120 8564_ $$8763788$$s28394$$uhttps://cds.cern.ch/record/1501120/files/fig3.png$$y00004 Caption not extracted
001501120 8564_ $$8763781$$s19477$$uhttps://cds.cern.ch/record/1501120/files/fig4a.png$$y00005 \small \it Type II 2HDM: the 95\% C.L. upper limits on the production cross-section as a function of \mHpm\ for four different values of the branching ratio Br(\Hp\ra\tp$\nu$), combining the data collected by the four LEP experiments at centre-of-mass energies from 183 to 209~GeV. The solid lines represent the observed exclusion limits, while the expected exclusion limits are indicated by the dashed lines. The shaded bands represent the $\pm 1\sigma$ and $\pm 2\sigma$ excursions around the expected limits. The intersections of the curves (solid or dashed) with the thick line showing the theoretical (tree-level) charged Higgs cross-section represent the (observed or expected) 95\% C.L. lower limits on the charged Higgs boson mass.
001501120 8564_ $$8763780$$s23160$$uhttps://cds.cern.ch/record/1501120/files/fig4b.png$$y00006 \small \it Type II 2HDM: the 95\% C.L. upper limits on the production cross-section as a function of \mHpm\ for four different values of the branching ratio Br(\Hp\ra\tp$\nu$), combining the data collected by the four LEP experiments at centre-of-mass energies from 183 to 209~GeV. The solid lines represent the observed exclusion limits, while the expected exclusion limits are indicated by the dashed lines. The shaded bands represent the $\pm 1\sigma$ and $\pm 2\sigma$ excursions around the expected limits. The intersections of the curves (solid or dashed) with the thick line showing the theoretical (tree-level) charged Higgs cross-section represent the (observed or expected) 95\% C.L. lower limits on the charged Higgs boson mass.
001501120 8564_ $$8763779$$s26184$$uhttps://cds.cern.ch/record/1501120/files/fig4c.png$$y00007 \small \it Type II 2HDM: the 95\% C.L. upper limits on the production cross-section as a function of \mHpm\ for four different values of the branching ratio Br(\Hp\ra\tp$\nu$), combining the data collected by the four LEP experiments at centre-of-mass energies from 183 to 209~GeV. The solid lines represent the observed exclusion limits, while the expected exclusion limits are indicated by the dashed lines. The shaded bands represent the $\pm 1\sigma$ and $\pm 2\sigma$ excursions around the expected limits. The intersections of the curves (solid or dashed) with the thick line showing the theoretical (tree-level) charged Higgs cross-section represent the (observed or expected) 95\% C.L. lower limits on the charged Higgs boson mass.
001501120 8564_ $$8763778$$s25075$$uhttps://cds.cern.ch/record/1501120/files/fig4d.png$$y00008 \small \it Type II 2HDM: the 95\% C.L. upper limits on the production cross-section as a function of \mHpm\ for four different values of the branching ratio Br(\Hp\ra\tp$\nu$), combining the data collected by the four LEP experiments at centre-of-mass energies from 183 to 209~GeV. The solid lines represent the observed exclusion limits, while the expected exclusion limits are indicated by the dashed lines. The shaded bands represent the $\pm 1\sigma$ and $\pm 2\sigma$ excursions around the expected limits. The intersections of the curves (solid or dashed) with the thick line showing the theoretical (tree-level) charged Higgs cross-section represent the (observed or expected) 95\% C.L. lower limits on the charged Higgs boson mass.
001501120 8564_ $$8763786$$s76475$$uhttps://cds.cern.ch/record/1501120/files/fig5.png$$y00008 \small \it Type I 2HDM: decay branching fractions as functions of the boson masses and \tanb.
001501120 8564_ $$8763790$$s26134$$uhttps://cds.cern.ch/record/1501120/files/fig6a.png$$y00009 \small \it Type I 2HDM: contours based on the observed p-values $CL_b$ as a function of $m_{\mathrm{H}^{\pm}}$ and $\tan \beta$ or $m_{\mathrm{A}}$, indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation, for four values of $m_{\mathrm{A}}$ and two values of $\tan \beta$. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$8763783$$s27576$$uhttps://cds.cern.ch/record/1501120/files/fig6b.png$$y00010 \small \it Type I 2HDM: contours based on the observed p-values $CL_b$ as a function of $m_{\mathrm{H}^{\pm}}$ and $\tan \beta$ or $m_{\mathrm{A}}$, indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation, for four values of $m_{\mathrm{A}}$ and two values of $\tan \beta$. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$8763794$$s26447$$uhttps://cds.cern.ch/record/1501120/files/fig6c.png$$y00012 \small \it Type I 2HDM: contours based on the observed p-values $CL_b$ as a function of $m_{\mathrm{H}^{\pm}}$ and $\tan \beta$ or $m_{\mathrm{A}}$, indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation, for four values of $m_{\mathrm{A}}$ and two values of $\tan \beta$. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$8763784$$s24545$$uhttps://cds.cern.ch/record/1501120/files/fig6d.png$$y00013 \small \it Type I 2HDM: contours based on the observed p-values $CL_b$ as a function of $m_{\mathrm{H}^{\pm}}$ and $\tan \beta$ or $m_{\mathrm{A}}$, indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation, for four values of $m_{\mathrm{A}}$ and two values of $\tan \beta$. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$8763793$$s22441$$uhttps://cds.cern.ch/record/1501120/files/fig6e.png$$y00014 \small \it Type I 2HDM: contours based on the observed p-values $CL_b$ as a function of $m_{\mathrm{H}^{\pm}}$ and $\tan \beta$ or $m_{\mathrm{A}}$, indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation, for four values of $m_{\mathrm{A}}$ and two values of $\tan \beta$. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$8763796$$s21133$$uhttps://cds.cern.ch/record/1501120/files/fig6f.png$$y00015 \small \it Type I 2HDM: contours based on the observed p-values $CL_b$ as a function of $m_{\mathrm{H}^{\pm}}$ and $\tan \beta$ or $m_{\mathrm{A}}$, indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation, for four values of $m_{\mathrm{A}}$ and two values of $\tan \beta$. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$8763785$$s76307$$uhttps://cds.cern.ch/record/1501120/files/fig7.png$$y00016 \small \it Type I 2HDM: Observed (left) and expected (right) 95\% C.L. lower limits on the mass of the charged Higgs boson. The colour-mass correspondence is indicated on the right hand side (units are \Gcs).
001501120 8564_ $$8763795$$s28264$$uhttps://cds.cern.ch/record/1501120/files/fig8.png$$y00017 \small \it Type I 2HDM: Excluded regions at 95\% C.L. in the (\mHpm,\tanb) plane for different values of \mA: 12, 30, 50 and 70 \Gcs. The dashed line represents the expected exclusion limit.
001501120 8564_ $$8763782$$s353808$$uhttps://cds.cern.ch/record/1501120/files/arXiv:1301.6065.pdf
001501120 8564_ $$8743915$$s410000$$uhttps://cds.cern.ch/record/1501120/files/CERN-PH-EP-DRAFT-MISC-2012-010 - draft.pdf$$yDraft (restricted)$$zStamped by WebSubmit: 18/01/2013
001501120 8564_ $$8743915$$s457971$$uhttps://cds.cern.ch/record/1501120/files/CERN-PH-EP-DRAFT-MISC-2012-010 - draft.pdf?subformat=pdfa$$xpdfa$$yDraft (restricted)$$zStamped by WebSubmit: 18/01/2013
001501120 8564_ $$81288450$$s19477$$uhttps://cds.cern.ch/record/1501120/files/xsec_tn.png$$y00009 \small \it Type II 2HDM: the 95\% C.L. upper limits on the production cross-section as a function of \mHpm\ for four different values of the branching ratio Br(\Hp\ra\tp$\nu$), combining the data collected by the four LEP experiments at centre-of-mass energies from 183 to 209~GeV. The solid lines represent the oserved exclusion limits, while the expected exclusion limits are indicated by the dashed lines. The shaded bands represent the $\pm 1\sigma$ and $\pm 2\sigma$ excursions around the expected limits. The intersections of the curves (solid or dashed) with the thick line showing the theoretical (tree-level) charged Higgs cross-section represent the (observed or expected) 95\% C.L. lower limits on the charged Higgs boson mass.
001501120 8564_ $$81288451$$s28264$$uhttps://cds.cern.ch/record/1501120/files/fig9.png$$y00017 \small \it Type I 2HDM: Excluded regions at 95\% C.L. in the (\mHpm,\tanb) plane for different values of \mA: 12, 30, 50 and 70 \Gcs. The dashed line represents the expected exclusion limit.
001501120 8564_ $$81288452$$s76475$$uhttps://cds.cern.ch/record/1501120/files/figtyp1.png$$y00013 \small \it Type I 2HDM: decay branching fractions as functions of the boson masses and \tanb.
001501120 8564_ $$81288453$$s26184$$uhttps://cds.cern.ch/record/1501120/files/xsec_02.png$$y00011 \small \it Type II 2HDM: the 95\% C.L. upper limits on the production cross-section as a function of \mHpm\ for four different values of the branching ratio Br(\Hp\ra\tp$\nu$), combining the data collected by the four LEP experiments at centre-of-mass energies from 183 to 209~GeV. The solid lines represent the oserved exclusion limits, while the expected exclusion limits are indicated by the dashed lines. The shaded bands represent the $\pm 1\sigma$ and $\pm 2\sigma$ excursions around the expected limits. The intersections of the curves (solid or dashed) with the thick line showing the theoretical (tree-level) charged Higgs cross-section represent the (observed or expected) 95\% C.L. lower limits on the charged Higgs boson mass.
001501120 8564_ $$81288454$$s17141$$uhttps://cds.cern.ch/record/1501120/files/aleph_lim.png$$y00001 \small \it Type II 2HDM: the 95\% C.L. bounds on \mHpm\ as a function of the branching ratio Br(\Hp\ra\tp$\nu$), for each of the four LEP experiments separately. The expected exclusion limits are indicated by the thin solid line and the observed limits by the thick solid line. The shaded area is excluded at the 95\% C.L. or higher.
001501120 8564_ $$81288455$$s25075$$uhttps://cds.cern.ch/record/1501120/files/xsec_cs.png$$y00011 \small \it Type II 2HDM: the 95\% C.L. upper limits on the production cross-section as a function of \mHpm\ for four different values of the branching ratio Br(\Hp\ra\tp$\nu$), combining the data collected by the four LEP experiments at centre-of-mass energies from 183 to 209~GeV. The solid lines represent the oserved exclusion limits, while the expected exclusion limits are indicated by the dashed lines. The shaded bands represent the $\pm 1\sigma$ and $\pm 2\sigma$ excursions around the expected limits. The intersections of the curves (solid or dashed) with the thick line showing the theoretical (tree-level) charged Higgs cross-section represent the (observed or expected) 95\% C.L. lower limits on the charged Higgs boson mass.
001501120 8564_ $$81288456$$s17891$$uhttps://cds.cern.ch/record/1501120/files/delphi_lim.png$$y00002 \small \it Type II 2HDM: the 95\% C.L. bounds on \mHpm\ as a function of the branching ratio Br(\Hp\ra\tp$\nu$), for each of the four LEP experiments separately. The expected exclusion limits are indicated by the thin solid line and the observed limits by the thick solid line. The shaded area is excluded at the 95\% C.L. or higher.
001501120 8564_ $$81288457$$s23160$$uhttps://cds.cern.ch/record/1501120/files/xsec_tq.png$$y00010 \small \it Type II 2HDM: the 95\% C.L. upper limits on the production cross-section as a function of \mHpm\ for four different values of the branching ratio Br(\Hp\ra\tp$\nu$), combining the data collected by the four LEP experiments at centre-of-mass energies from 183 to 209~GeV. The solid lines represent the oserved exclusion limits, while the expected exclusion limits are indicated by the dashed lines. The shaded bands represent the $\pm 1\sigma$ and $\pm 2\sigma$ excursions around the expected limits. The intersections of the curves (solid or dashed) with the thick line showing the theoretical (tree-level) charged Higgs cross-section represent the (observed or expected) 95\% C.L. lower limits on the charged Higgs boson mass.
001501120 8564_ $$81288458$$s21133$$uhttps://cds.cern.ch/record/1501120/files/clb_tb100.png$$y00015 \small \it Type I 2HDM: contours based on the observed p-values $CL_b$ as a function of $m_{\mathrm{H}^{\pm}}$ and $\tan \beta$ or $m_{\mathrm{A}}$, indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation, for four values of $m_{\mathrm{A}}$ and two values of $\tan \beta$. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$81288459$$s34264$$uhttps://cds.cern.ch/record/1501120/files/adlo_clb.png$$y00005 \small \it Type II 2HDM: contours based on the observed p-values $CL_b$ as a function of \mHpm\ and the branching ratio Br(\Hp\ra\tp$\nu$), indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$81288460$$s17151$$uhttps://cds.cern.ch/record/1501120/files/opal_lim.png$$y00004 \small \it Type II 2HDM: the 95\% C.L. bounds on \mHpm\ as a function of the branching ratio Br(\Hp\ra\tp$\nu$), for each of the four LEP experiments separately. The expected exclusion limits are indicated by the thin solid line and the observed limits by the thick solid line. The shaded area is excluded at the 95\% C.L. or higher.
001501120 8564_ $$81288461$$s28394$$uhttps://cds.cern.ch/record/1501120/files/adlo_chan.png$$y00007 Caption not extracted
001501120 8564_ $$81288462$$s22441$$uhttps://cds.cern.ch/record/1501120/files/clb_tb10.png$$y00014 \small \it Type I 2HDM: contours based on the observed p-values $CL_b$ as a function of $m_{\mathrm{H}^{\pm}}$ and $\tan \beta$ or $m_{\mathrm{A}}$, indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation, for four values of $m_{\mathrm{A}}$ and two values of $\tan \beta$. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$81288463$$s26447$$uhttps://cds.cern.ch/record/1501120/files/clb_ma50.png$$y00012 \small \it Type I 2HDM: contours based on the observed p-values $CL_b$ as a function of $m_{\mathrm{H}^{\pm}}$ and $\tan \beta$ or $m_{\mathrm{A}}$, indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation, for four values of $m_{\mathrm{A}}$ and two values of $\tan \beta$. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$81288464$$s16241$$uhttps://cds.cern.ch/record/1501120/files/l3_lim.png$$y00003 \small \it Type II 2HDM: the 95\% C.L. bounds on \mHpm\ as a function of the branching ratio Br(\Hp\ra\tp$\nu$), for each of the four LEP experiments separately. The expected exclusion limits are indicated by the thin solid line and the observed limits by the thick solid line. The shaded area is excluded at the 95\% C.L. or higher.
001501120 8564_ $$81288465$$s22791$$uhttps://cds.cern.ch/record/1501120/files/adlo_lim.png$$y00006 \small \it Type II 2HDM: excluded regions in the Br(\Hp\ra\tp$\nu$) vs \mHpm\ plane, based on the combined data collected by the four LEP experiments at centre-of-mass energies from 183 to 209~GeV. The shaded area is excluded at the 95\% or higher C.L.. The expected exclusion limit (at the 95\% C.L.) is indicated by the thin solid line and the thick dotted line inside the shaded area is the observed limit at the 99.7\% C.L..\small \it Type II 2HDM: regions in the Br(\Hp\ra\tp$\nu$) vs \mHpm\ plane excluded at the 95\% or higher C.L., based on the combined data collected by the four LEP experiments at centre-of-mass energies from 183 to 209~GeV, for each of the three decay channels separately. The solid (dashed) lines are the observed (expected) limits.Caption not extracted
001501120 8564_ $$81288466$$s26134$$uhttps://cds.cern.ch/record/1501120/files/clb_ma12.png$$y00014 \small \it Type I 2HDM: contours based on the observed p-values $CL_b$ as a function of $m_{\mathrm{H}^{\pm}}$ and $\tan \beta$ or $m_{\mathrm{A}}$, indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation, for four values of $m_{\mathrm{A}}$ and two values of $\tan \beta$. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$81288467$$s24545$$uhttps://cds.cern.ch/record/1501120/files/clb_ma70.png$$y00013 \small \it Type I 2HDM: contours based on the observed p-values $CL_b$ as a function of $m_{\mathrm{H}^{\pm}}$ and $\tan \beta$ or $m_{\mathrm{A}}$, indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation, for four values of $m_{\mathrm{A}}$ and two values of $\tan \beta$. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$81288468$$s27576$$uhttps://cds.cern.ch/record/1501120/files/clb_ma30.png$$y00015 \small \it Type I 2HDM: contours based on the observed p-values $CL_b$ as a function of $m_{\mathrm{H}^{\pm}}$ and $\tan \beta$ or $m_{\mathrm{A}}$, indicating the statistical significance, N$_{\sigma}$, of local departures from the background expectation, for four values of $m_{\mathrm{A}}$ and two values of $\tan \beta$. The black solid line indicates the change of sign of this significance, i.e. where there is a transition from excess to deficit.
001501120 8564_ $$81288469$$s76307$$uhttps://cds.cern.ch/record/1501120/files/2HDMtype1.png$$y00016 \small \it Type I 2HDM: Observed (left) and expected (right) 95\% C.L. lower limits on the mass of the charged Higgs boson. The colour-mass correspondence is indicated on the right hand side (units are \Gcs).
001501120 8564_ $$8763791$$s9563$$uhttps://cds.cern.ch/record/1501120/files/fig00000.png$$y00000 noimg: \small\it Overview of the searches for charged Higgs bosons performed by the four LEP experiments, whose results are used in this combination. Where relevant, \mA\ varies from 2$m_b$ to $m_{\Hpm}$. Each experiment analysed typically around 650 \pb of data.: \small\it Individual search results for the \ee\ra\Hp\Hm\ fermionic final states. All limits are given at the 95\% C.L. The OPAL selection is mass-dependent; the numbers of events given here are for \mHpm = {\rm 80}~\Gcs.: \small\it Combined and individual $CL_b$ values for the three mass points with a deviation from expectation larger than 2 $\sigma$. All values, obtained with the statistical procedure of the overall combination, compare well to those published by the experiments. (*) ALEPH and L3 did not provide inputs for this mass.: \small\it The combined 95\% C.L. lower bounds on the mass of the charged Higgs boson (in \Gcs), expected and observed, for fixed values of the branching ratio Br(\Hp\ra\tp$\nu$) and for any Br(\Hp\ra\tp$\nu$). All mass limits have been rounded down to the nearest half a \Gcs\ to take into account the effect of neglecting the correlations between systematic uncertainties. (*) The interval from 83 to 88 \Gcs\ is also excluded at the 95\% C.L.
001501120 901__ $$uCERN
001501120 9031_ $$aApproval requested for number CERN-PH-EP-2012-369$$bCERN-PH-EP-2012-369$$cEPPHAPP$$d2012-12-20 11:34:29$$e2012-12-27 11:34:[email protected]$$swaiting
001501120 9031_ $$aFurther internal refereeing of the paper$$bCERN-PH-EP-2012-369$$cEPPHAPP$$d2012-12-20 12:30:[email protected]$$sreviewing
001501120 9031_ $$aDocument approved$$bCERN-PH-EP-2012-369$$cEPPHAPP$$d2013-01-18 10:23:[email protected]$$sapproved
001501120 916__ $$sn$$w201251$$ya2013
001501120 960__ $$a13
001501120 981__ $$a1510316
001501120 980__ $$aARTICLE
001501120 980__ $$aALEPH_Papers
001501120 980__ $$aDELPHI_Papers
001501120 980__ $$aOPAL_Papers
001501120 980__ $$aL3_Papers