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Search for non-SM Light Higgs Boson in the h -> to gamma gamma Channel at D0 in Run II PDF

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Preview Search for non-SM Light Higgs Boson in the h -> to gamma gamma Channel at D0 in Run II

February 6, 2008 17:2 WSPC/INSTRUCTION FILE ws-ijmpa International JournalofModernPhysicsA (cid:13)c WorldScientificPublishingCompany 5 0 Search for non-SM Light Higgs Boson in the h → γγ Channel at DØ in 0 2 Run II n a J ALEXMELNITCHOUK∗ 7 Department of Physics and Astronomy, 2 The Universityof Mississippi, 108 LewisHall, P.O. Box 1848 1 University,MS 38677-1848 v 7 6 Received(31October2004) 0 Revised(31October 2004) 1 0 Asearchfornon-SMlightHiggsbosonwithanenhancedbranchingfractionintophotons 5 inpp¯collisionsattheFermilabTevatronispresentedusingRunIIDØdatatakenbetween 0 April2002andSeptember2003.Weset95%CLlimitsonthediphotonbranchingfraction / x asafunctionofHiggsmassforFermiophobicandTopcolorHiggsscenarios. e - Keywords:Higgs;fermiophobic;photon. p e h 1. Motivation : v γγ is a very clean signature which makes it promising and important especially i X for the hadron collider environment. There are many extensions of the SM that r allow enhanced γγ decay rate of the Higgs largely due to suppressed couplings a 1 withfermions .WeconsiderFermiophobicHiggs(noHiggs-fermioncouplings)and Topcolor Higgs (coupling with the top quark is allowed) 2. Dataset We used the data collected by the DØ detector between April 2002 and September −1 2003.Theintegratedluminosityofthissampleis191.0±12.4pb Triggerselection a wasdonewithhighpT di-EM trigger.Offlinewe requiretworeconstructedphoton objectsinthe goodη fiducialregion(|η|<1.05,1.5<|η|<2.4)withpT >25GeV. 2 We require that the pT of the diphoton system is above 35 GeV . 3. Backgrounds ∗ Major sources of background to h →γγ are Z/γ →ee, direct diphotons, γ+jet, and multijet QCD processes. ∗Fermilab,MS#352,Batavia, IL,60510, USA. aEMstandsfor“electromagnetic object”, i.e.electronorphoton 1 February 6, 2008 17:2 WSPC/INSTRUCTION FILE ws-ijmpa 2 Alex Melnitchouk 4. Results The γγ invariant mass distributions for the data and predicted background, as well as the event yields are shown in Fig. 1. Figure 2 shows 95% CL limits on the B(h →γγ ) as a function of Higgs mass. Comparison is made with DØ Run I and 5 LEP results as well as Run II Monte Carlo studies for Tevatron . 5. Conclusions A search for non-SM light Higgs boson with an enhanced branching fraction into −1 photons was performed using 191pb of data collected by the DØ experiment in Run II of the Fermilab Tevatron.We set 95% CL limits onthe diphoton branching fractionasafunctionofHiggsmassforFermiophobicandTopcolorHiggsscenarios. Our current sensitivity is comparable with Run I. Fig. 1. γγ invariant mass distributions and event counts for different event topologies with new photon ID after analysis optimization cut (pγγ >35GeV) is applied. Points – γγ spectrum T observedindata,redrectangles–totalSMbackgroundwitherrors,greenline–QCDbackground, brownline–Drell-Yanbackground, blackline–directdiphotonbackground. Acknowledgments We thank the staffs at Fermilab and collaborating institutions, and acknowledge support from the Department of Energy and National Science Foundation (USA), Commissariat `a L’Energie Atomique and CNRS/Institut National de Physique Nucl´eaire et de Physique des Particules (France), Ministry for Science and Tech- nology and Ministry for Atomic Energy (Russia), CAPES, CNPq and FAPERJ (Brazil), Departments of Atomic Energy and Science and Education (India), Col- ciencias(Colombia),CONACyT(Mexico),MinistryofEducationandKOSEF(Ko- rea), CONICET and UBACyT (Argentina), The Foundation for Fundamental Re- search on Matter (The Netherlands), PPARC (United Kingdom), Ministry of Ed- ucation (Czech Republic), A.P. Sloan Foundation, Civilian Research and Develop- ment Foundation, Research Corporation, Texas Advanced Research Program, and the Alexander von Humboldt Foundation. February 6, 2008 17:2 WSPC/INSTRUCTION FILE ws-ijmpa Search for non-SM Light HiggsBoson in theh→γγ Channel at DØ inRun II 3 DØ Run II Preliminary )) 11 gg Run II 191 pb-1 gg fifihh B(B( Run I 100 pb-1 100 pb-1 MC predictions --11 1100 2 fb-1 benchmark LEP model 6600 8800 110000 112200 114400 ((ffeerrmmiioopphhoobbiicc)) MM ((GGeeVV)) hh DØ Run II Preliminary ) 1 g g fih ( B -1 10 60 80 100 120 140 (topcolor) M (GeV) h Fig.2. 95%CLlimitsontheHiggsdecaybranchingfractionintophotonsasafunctionofmass (blackcurve).Topplot–fermiophobicHiggsscenario,bottom plot–topcolorHiggsscenario.On the top plot exclusion contours from DØ Run I 3 (red) and LEP 4 (blue) are overlaid. Magenta linesshow100pb−1and2fb−1MonteCarlopredictionsforTevatronRunII5basedonRunIDØ andCDFefficienciesandmisIDrates.Greenpoints–theoreticalcurveforbenchmarkfermiophobic Higgsmodel4. References 1. S.Mrenna, J. Wells, Phys. Rev. D63, 015006 (2001). 2. Alex Melnitchouk,Ph.D Thesis, Brown University (2003) (Unpublished). 3. B.Abbotetal.(DØCollaboration),PhysRev.Lett.82,2244(1999);BrianLauer,Ph.D Thesis, Iowa State University(Unpublished)(1997). 4. A.Rosca, hep-ex/0212038 (2002). 5. G. Landsberg, K. Matchev, Phys.Rev. D62, 035004 (2000).

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