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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 1 Polarization studies in tt events with full simulation 1.Physics motivations 2.Full simulation objects (leptons, jets, E T miss) 3.tt event reconstruction: masses, angles 4.W and top polarization measurements 5.Conclusions F. Hubaut, E. Monnier, P. Pralavorio, B. Resende – CPPM C. Zhu – CPPM/SDU
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 2 Motivations: test top production and decay LHC σ ~300 pb Weak Interaction single top Tevatron σ ~3 pb Top polarization BR(t Wb)~100% No top hadronization tWb vertex Top production Top decay W polarization Full hadronic (3.7M) : jets Dileptonic (0.4M) : 2 l + 2 b + 2 Semileptonic (2.5M) : l + + 2b + jets tt final states (10 fb -1 ) Test SM, Search for anomalous couplings LHC σ ~850 pb Tevatron σ ~7 pb Strong Interaction gg,qq tt pairs ATLAS sensitivity to polarization with Atlfast in SN-ATLAS-2005-052 Accepted for publication in EPJC
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 3 Angle between: lepton in W rest frame and W in top rest frame Standard Model (M top =175 GeV) 0.7030.2970.000 W polarization in top decay Test the top decay (in fully reconstructed tt) with W polarization... Longitudinal W + (F 0 )Left-handed W + (F L ) Right-handed W + (F R ) NLO0.6950.3040.001 ...by measuring angular distribution of charged lepton in W rest frame Sensitive to EWSBTest of V-A structure 1/21 cos 1/N dN/dcos W+W+ b l+l+ t spin
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 4 tt spin correlation Test the top production … t and t not polarised in tt pairs, but correlations between spins of t and t … by measuring angular distributions of daughter particles in top rest frames A D =-0.29 M tt <550 GeV A D =-0.24 Angle between spin analysers Angle between t(t) and spin analysers top spin ≠1/2, anomalous coupling, t H + b A=0.42 A=0.33
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 5 Measurement method apply weights event by event Reconstruction and cuts Correction function : parton level Selection cuts and reconstruction distort the parton level distribution Use an independent sample to parametrize these effects Apply this method for W polarization and spin correlation cos 1/weight cos 1/N dN/dcos
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 6 Scope of full simulation studies SN-ATLAS-2005-052: with 10 fb -1 and combining semilep+dilep (Atlfast): Spin correlationW polarization AADAD F0F0 FRFR SM0.422-0.2900.7030.000 ± Stat± 0.014± 0.008± 0.004± 0.003 ± Syst± 0.023± 0.010± 0.015± 0.024 F 0, F R driven by semileptonic and A, A D by dileptonic Precision between 1% and 5% dominated by systematics. Challenging ! Perform the same study in full simulation
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 7 Full simulation Rome samples Signal samples – semileptonic tt, lepton = e, : TopReX+PYTHIAAOD/CBNT1500 pb -1 375k# 4520, 4521 MC@NLO+HERWIGAOD/CBNT 500 pb -1 130k# T1 Background samples (most important with Atlfast): W+4jetsAOD 75 pb -1 180k# A7 Single TopAOD 950 pb -1 1800 pb -1 9200 pb -1 90k 70k 19k # 4511 # 4530, 4531 # 4540 Understand performance for each object: extensive comparison AOD/CBNT very useful Quantify NLO effects on polarization measurements (angle resolution): extensive comparison MC@NLO/TopReX
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 8 Understand objects in tt events Electron Muon Jets (light and b) E T miss Reconstruct tt events Masses Background tt( ), W+4jets, single top Reconstruct angles in W and top rest frames Understand p T, , resolutions and spectra of W and tops lep jet and angle resolutions Results on W and top polarizations Topics of the presentation Refine selection (isolation, calibration,...) Understand p T, , resolutions and spectra
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 9 p T (GeV) Electron selection Algorithm: author = 1 (high p T electron : egamma) Identification with simple cuts: IsEM&2047=0 + hasTrack Isolation: E T (EM+HAD in R=0.3*) < 10 GeV around electron (loose cut) Rec. Eff. = 81.4% Selection: 1 e p T >20 GeV, | <2.5 Efficiency = 60.5% Purity = 98.9% AOD = CBNT *:0.2 preferred but is not filled in AODs
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 10 Algorithm: author = 1 (high p T muon) AOD (Moore) ≠ CBNT (MuonBoy) Identification (combined information): hasCombinedTrack=1 with 2 /ndof<20 Reject muons from and K decays (bad 2 ) Isolation: E T (EM in R=0.2) <10 GeV around muon track (loose cut) Reject muons from b and c-jets Rec. Eff. (MuID) = 85.2% Selection: 1 p T >20 GeV, | <2.5 Efficiency = 58.9% Purity = 99.2% p T (GeV) Muon selection
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 11 Selected lepton resolution in tt e EM p T scale is correct to 0.4% =2.0 % e ID =3.2 % comb =2.6 % e EM =20.10 -3 e ID =0.6.10 -3 =0.13 mrad =0.6.10 -3 =0.21 mrad No correction of track curvature comb p T scale is correct to 0.4% Electron: E in EM calorimeter (brem. recovery) and , in ID (Not AOD default !) Comparison with Atlfast : p T OK, ( ) not gaussian in Atlfast Same resolutions with MC@NLO p T /p T resolution resolution resolution =1 mrad e EM
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 12 NTRTHits Electron : problem with # of TRTHits ? 10% of electron tracks with no TRT hits ? Muons OK Those tracks degrade p T )/p T by 40% and resolutions degraded by 10% and 20% e + 2 times more affected than e - NTRTHits
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 13 Jets Algorithm : cone with R size of 0.7 Electron/muon in jets : if R(isolated el. - jet)<0.2 remove the jet (80%) if 0.2< R(isolated el. - jet)<0.7 subtract electron 4-momentum from jet (15%) Add muon 4-momentum if R(muon-jet)<0.2 In situ calibration : the 2 jets coming from W Reduce combinatorial background Selection : ≥ 4jets with p T >30 GeV, | <2.5 Efficiency = 37.6% AOD ≠ CBNT : same , but p T (slightly) different... ?
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 14 b-tagging, p T miss CBNT: SV2 weight > 3 Efficiency = 60% R uds = 84 R c = 8 AOD: SV1 + IP3D weight > 3 Efficiency = 53% R uds = 93 R c = 11 B-tagging selection : ≥ 2 b-jets p T miss : >20 GeV Efficiency = 91.2%
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 15 Jet/p T miss resolution in tt events light jet p T scale correct to 1% = 9.8 % b-jet = 8.6 % = 18 % = 0.03 = 22 mrad = 0.27 = 0.22 rad = 0.03 = 18 mrad Large negative shift for p T miss?? Resolutions as expected. Same resolutions (and p T miss shift !) with MC@NLO resolution resolution pT/pT resolution p T scale correct to 1% shifted by 9% b-jet light jet
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 16 Reconstructed masses, Background Kinematic cuts efficiency: 6.5 %. With M tops <35 GeV: 5.0 % Agreement with Atlfast and MC@NLO Non tt background (W+4jets, single top) increases by a factor 2-3 wrt Atlfast (still preliminary) S/B~10 ; still dominated by internal background tt + X M=175.5 ± 0.3 GeV =7.5 ± 0.4 GeV M=172.7 ± 0.3 GeV =7.2 ± 0.6 GeV hadronic top leptonic top
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 17 Ws resolution: Full vs fast sim reco – true reco – true (p Treco –p Ttrue )/p Ttrue Good overall agreement between TopReX Full simulation and Atlfast Difference in leptonic W p T resolution explained by p T miss miscalibration W had. W lept. W had. W lept. 1. 1.1. 1. 1.1.
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 18 Resolution on angle in W rest frame Cos Cos true Full sim ATLfast TopReX MC@NLO Very good agreement between TopReX Full simulation and Atlfast... ... and between TopReX and MC@NLO Cos Cos true Angle between: lepton in W rest frame and W in top rest frame 1/21 W+W+ b l+l+ t spin
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 19 Results: W polarization TopReX Atlfast 10 fb -1 TopReX full sim 1.5 fb -1 F 0 =0.699 ± 0.005 F L =0.299 ± 0.003 F R =0.002 ± 0.003 F 0 =0.677 ± 0.015 F L =0.309 ± 0.009 F R =0.014 ± 0.009 MC@NLO full sim 0.5 fb -1 Values compatible with SM expectations in each case F 0 =0.684 ± 0.021 F L =0.307 ± 0.011 F R =0.009 ± 0.011
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 20 Top resolution: Full vs fast sim Good overall agreement between TopReX Full simulation and Atlfast Difference in leptonic top p T resolution explained by p T miss miscalibration top had. top lept. top had. top lept. reco – true reco – true (p Treco –p Ttrue )/p Ttrue
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 21 Resolution on angles in top rest frame Full sim ATLfast TopReX MC@NLO cos lep-lej cos lep cos jet Very good agreement between TopReX Full simulation and Atlfast Small differences between TopReX and MC@NLO
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 22 Results: top spin correlation A (±stat)A D (±stat) SM values0.42-0.29 TopReX Atlfast 0.42 0.02-0.29 0.01 TopReX Full sim 0.45 0.06-0.29 0.03 MC@NLO Full sim 0.02 0.090.00 0.05 Toprex values compatible with SM expectations MC@NLO have no spin correlation included... Check only it gives 0
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 23 Conclusions Fast simulation (SN-ATLAS-2005-052) shown that ATLAS can measure precisely W polarization ~1-2% and top spin correlation ~5% after 10fb -1 This precision requires a deep understanding of all objects: Electrons: OK except N(TRT). Combine E from calo and angles from tracker Muons: switch to more recent version of Moore/MuID Jets: switch to cone size 0.4 for jets Shift in p T miss scale : ? Good agreement between Fast/Full sim. and TopReX/MC@NLO Next step: systematics update with full simulation light/b-jet miscalibration, b-tagging efficiency, …
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 24 Spare: W, t performances : TopReX vs MC@NLO Good overall agreement between TopReX and MC@NLO for the Ws Difference in tops under invetsigation (b-jet association?) top had. W had. W lept. top lept. W had. W lept. p T /p T
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B. Resende Top WG 28/10/05 Polarization studies in ttbar events 25 Spare: Correction functions tt spin correlation : A D tt spin correlation : A W polarization Good agreement within statistics with Atlfast Agrees also with MC@NLO Full sim ATLfast
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