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Search for a charged Higgs in H + cs using 4.7 fb -1. A. Martyniuk a , P. Miyagawa b , M. Owen c , O. Trifis c , V. Chavda c , and U.K. Yang c a: University of Victoria b: University of Sheffield c: University of Manchester Higgs Meeting, August 27, 2012.
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Search for a charged Higgs in H+cs using 4.7 fb-1 A. Martyniuka, P. Miyagawab, M. Owenc, O. Trifisc, V. Chavdac, and U.K. Yangc a: University of Victoria b: University of Sheffield c: University of Manchester Higgs Meeting, August 27, 2012 Thanks to the Editorial Board: Michel Vetterli (Chair) Martin zur Nedden, Wouter Verkerke, James Ferrando
Introduction • A charged Higgs boson is predicted by the Beyond SM: Two Higgs Doublet Model: H0, h0, A0, H± • Charged Higgs productions from top quark decays • Huge top production, focus on H+cs at low tanb • Complementary to H+tn at high tanb e/m W+ b-jet ν jet W/H- b-jet jet
Analysis Overview • Semi-leptonic tt sample • Dijet mass c2 fitter e/m W+ b-jet ν jet W/H- b-jet jet • Likelihood Fit, Br(tH+b): • Discovery or 95% Limits
Analysis History • Previous analysis with 35 pb-1 data (≥ 1 b-tag), comparable to the Tevatron limits ( ATL-CONF-2011-127, ATL-COM-PHYS-2011-130) • Updated analysis with 4.7 pb-1 (2011 full data) • High-pt lepton with 4 jets (at least 2 b-tag) • Single lepton trigger samples • Use the Top group selection cuts and have a good agreement • Lep Pt>25 (e), 20 (m), Jet Pt>25, MET> 35(e), 20(m), MV1 w>0.6 • The list of the full event selections cuts is in the backup slide • Supporting document • ATL-COM-PHYS-2012-660 • The updated analysis has a conditional approval in June, 2012 • Issues with systematic • Issues with fit stability
Analysis Essential 1 • A dijet mass c2 fitter: lepton plus 4 jets • Improved the dijet mass dist. by reconstructing whole ttbar event • Constrain W(e/m) and top quarks masses to be the PDG values, by floating jet/lepton energy within their resolutions • The 5th jet can be replaced as a W daughter jets with any of the two untagged 3rd, 4th jets • Remove poorly reconstructed events with c2<10 Before Fitting After Fitting
Analysis Essential 2 • Signals and background templates • Seven H+ signal templates from 90 to 150 GeV by 10 GeV step • SM ttbar template • Non-ttbar template (10%): • Single top, W/Z+jets, QCD, • and diboson
Analysis Essential 3 • Set limits on the branching ratio to charged Higgs boson using the frequentic procedure • A likelihood function is define as where ni: observed events, ni: expected events in each bin • Limits are calculated on a test Statistics qb based on a profile Likelihood ratio The exp. events of ttbar bkg and H+ signal as BR(tH+b)
Issues Raised in the Higgs Approval meeting and by the Edboard • Missing contributions in the limits • b-JES/c-JES syst. • Mtop syst. • Updated Stop t-ch. norm • Implementation of the syst. band in the kinematic distributions • Check the output nuisance parameters and their correlations • (N-1) limits to show the syst. effect of each item • Limits without a constraint on the s(ttbar) Limits presented in the approval meeting in June
Updates • Missing syst. contributions (b-/c-JES, Mtop, proper Stop t-ch. norm.) are included. Their contributions are small(done) • After ICHEP deadline passed, we decided to update our analysis • Use the most updated JES calibration and it’s uncertainty ( tag 00-05-09): lower eff. for Njet>=4 cut • Use the updated luminosity with small error: 4.66 /fb with 1.8% (old: 4.71/fb with 3.4%) no change in the data, but the bkgd prediction based on the MC is reduced by 1.2% • Implementation of the syst. band the kinematic distributions (done) • Check the output nuisance parameters and their correlations (done) • Limits without a constraint on the s(ttbar) (done) • (N-1) limits to show the syst. effect of each item (done)
Data vs Predictions old new data old new SMttbar
Results • The fit results are consistent with null Higgs hypothesis Stat. Only
Results on the Nuisance Parameters mH=90 GeV mH=110 GeV
(N-1) Limits? • The effect of the individual syst.? • The only one syst. Item is removed in the fit, “(N-1)” limit • Basically, the (N-1) limits are close to the N limits due to the correlations with other parameters
Correlations: nuisance parameters mH=90 GeV • Groups of the correlated systematic • JES, Mtop, bJES: c • bTag, s(ttbar) • Gen, I/FSR, PS and JER
(N-x) Limits • A group of the correlated parameters (x) is removed in the fit to check the effect of their syst. on the limits • The (N-x) limits look reasonable
The effect of the s(ttbar) constraint? • In the current fit, s(ttbar) is constrained with +7%/-9% uncertainties • What if we remove this constraint? basically 2 parameter fitting: Br(tH+b) and s(ttbar) • The limits are not changed • The resulting cross sections are consistent with the SM
Conclusions • The full 2011 data (4.7 fb-1) have been analyzed to search for a charged Higgs from top quark decays. • The results are consistent with null Higgs hypothesis • The 95% limits on Br(tH+b) are set between 5% to 1%, depending mHare improved by a factor of 5 to 10, with respect to the current best limits in csbar channel • The limits, equivalent to the limits from the three combined tau channels. • We plan to publish these results
Event Selection • Semi-leptonic channel: e/m plus at least 4 jets (2 b-tag) • Use the Top group selection cuts and have full agreement: acceptance challenge • Cuts are: • One el with ET> 25 GeV & |η| < 2.47, with a veto (1.37 < |η| < 1.52), OR one mu with pT> 20 GeV and |η| < 2.5 with single lepton triggers (EF_e20_medium,EF_e22_medium, EF_mu18, EF_mu18_medium) • Remove events tagged as e-mu overlap • Require a primary vertex with at least five tracks • MET > 35 GeV (el), OR MET > 20 GeV (mu) • Mt(W) > 25 GeV (el) OR MET + Mt(W) > 60 GeV (mu) • ≥ 4 jets with ET> 25 GeV and |η| < 2.5 and |JVF|>0.75 • Events with loose bad jets with pT> 20 GeV are rejected • ≥ 2 jet tagged with MV1 weight > 0.601713
Background estimations • SM ttbar (~90% of the total bkgd) • Use MC@NLO sample for shape and normalization with NNLO cross section • W+jets, Wbb/cc+jets, Wc+jets (~3.6% of the total bkgd) • Use ALPGEN interfaced with Herwig samples for shape and normalization • Normalized with K*cross sections plus the SFs derived from the Top W+jets group based on the W+/W- charge asymmetry in the data • Single top (~3.7% of the total bkgd) • Use MC@NLO sample for Wt and s-channel, but AcerMC for t-channel normalized with NNLO cross section (also shape) • Multi-jets (~2.5% of the total bkgd) • Use anti-electron data-driven method provided by the Top fake group (normalization)
Updated PS systematic • Powheg plus Herwig vs Pythia? • With Pythia AMTB1 tune: 11% difference in acceptance, disfavored by the jet shape data. • New PS syt. with Pythia Perugia 2011 C tune:3% difference in acceptance • The effect due to the PS on the limit is very minimal. Pythia Perugia 2011 C tune Pythia AMBT1 tune