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Overview Motivation Detector and algorithm description Aspects of t jet reconstruction

Reconstruction of Z -> tt ->e+ t jet events with early data in CMS Konstantinos A. Petridis IOP Conference Lancaster 31 st March 2008. Overview Motivation Detector and algorithm description Aspects of t jet reconstruction Results Background estimation Conclusions.

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Overview Motivation Detector and algorithm description Aspects of t jet reconstruction

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  1. Reconstruction of Z->tt->e+t jet events with early data in CMS Konstantinos A. PetridisIOP Conference Lancaster31st March 2008 • Overview • Motivation • Detector and algorithm description • Aspects of t jet reconstruction • Results • Background estimation • Conclusions IOP Lancaster

  2. IOP Lancaster Introduction • Motivation for reconstructing and selecting Z->tt->e+t jet events • Benchmark for light SM/SUSY H->tt->e+t jet discoveries • Main channel to measure t jet tagging efficiency • Vital ingredients for the measurement of x-section of events involving t jets • Input to measurements of SUSY studies • Analysis is based on methods to be applied on data from first physics run • Events have been simulated accounting for the detector conditions (calibration, alignement) with the first 100pb-1 of data

  3. IOP Lancaster The CMS Detector Ecal+Hcal Jet axis Ldg Trk Rm Signal coneRsig Riso L1=1st Level Trigger HLT=High Level Trigger Tau Jet L1+HLT: Calorimeter isolation at L1. At HLT build calo-jets out of “L1 accepted objects”. Build pixel seeded tracks and require Ecal and Pixel/Track isolation Electron L1+HLT: Calorimeter isolation at L1. At HLT build Ecal clusters out of “L1 accepted” objects. Build pixel seeded tracks and require E/P, HCal and Tracker isolation cuts. Tau Jet Offline: Calo/PF jet with isolated tracks. Variations of isolation (varying RS, h-f, q-f cone definitions…. ) Offline Electron Id: Based on H/E, E/P, cluster shape, brem fraction, track-cluster matching …cuts.

  4. Triggering on Z->tt->e+t jet IOP Lancaster L1+HLTe Turn on curve • Ideally trigger using HLT e+et jet trigger • At 1032cm-2s-1: HLTe ETe>15GeV HLTe+tjet ETe>12GeV ETt jet>20GeV • No gain of HLTe+t jet on top of HLTe at 1032cm-2s-1 • HLTe+t jet becomes important at higher L scenario when HLTe ET threshold increases • Therefore trigger on these events using HLTe HLTe = Single electron HLT HLTe+t jet = Single electron AND t jet HLT HLT e+et jet = HLTe OR HLTe+tjet Level-1+HLT e+et (22.9+/-0.4)% ~(12+/-4)Hz Level-1+HLT e (22.4+/-0.4)% ~(12+/-4)Hz

  5. IOP Lancaster Offline t jet tracker isolation performance Ldg Trk Finding efficiency factored in ET>20GeV Pass electron Rejection Isolation Cone Size

  6. IOP Lancaster e-t jet misidentification • Electrons are ideal candidates to pass t jet identification criteria since they are single isolated tracks. Need to be able to reject them. • ETmaxHT = Max Hcal Tower ET of Jet • Emfrac= EM fraction of Jet • Best performance byET3x3HT/PTLdgTr= Sum of 3x3 HCal Tower ET around leading track impact point on Calo Surface divided by Ldg Trk PT • For ET3x3HT/PTLdgTr>0.1 • (85+/-0.2)% t jet efficiency • (2.7+/-0.2)% e efficiency Reco t jet ET>20GeV Rm=0.1 PTLdgTr>6.GeV Riso=0.45 Rsig=0.07 • Further apply veto for candidates with LdgTr @ Ecal pointing to h cracks giving a total • ~80% t jet efficiency • ~1% e efficiency

  7. IOP Lancaster Offline Signal Performance t jet id eff e id eff w.r.t HLT

  8. IOP Lancaster Background Estimation • The charges of the electron and t jet in Signal events are opposite • This gives a good handle for selecting a Signal-Free mass window by looking at Same Sign (SS) Me+t jet • Background contribution in the Opposite Sign (OS) mass window can be extracted by looking at the number of events and shape of the SS mass window • Treat QCD and EWK processes separately • Use dedicated analyses to get the number of events for the corresponding luminosity and apply the selections efficiencies obtained from MC simulations to extract NW+jetsSS, NttbarSS, NZ+jets->eeSS • The (OS/SS)EWK ratios are obtained from MC simulations and verified with data • For QCD: • And (OS/SS)QCD can be obtained by looking at events passing a Non-Isolated electron trigger. This trigger has just been approved by CMS so this study is ongoing

  9. IOP Lancaster W+jets and ttbar Background Estimation Extracting Visible OS mass dist’n from SS NOS=NSSx(OS/SS)MC W+jets ttbar+jets (OS/SS)W+jets=3.4 (OS/SS)ttbar=2.3 NOS=10.4 NSSx(OS/SS)MC = 9 NOS=27.5 NSSx(OS/SS)MC = 25

  10. IOP Lancaster Z->ee Background Estimation • Extract OS Z->ee contribution by looking at events with reverse electron rejection criteria ET3x3HT/PTLdgTr<0.1(t-veto) • Hence NZ->OSe-veto=NZ->eeOSt-vetoxeZ->eee-veto/eZ->eet-veto • This requires knowledge of eZ->eee-veto/eZ->eet-vetowhich can be extracted using “Tag and Probe” methods (See Backup) • Can also extract mass shape however there are still some discrepancies that need to be understood

  11. IOP Lancaster Mass Plot Look at invariant mass between Opposite Sign (OS) reconstructed visible Z products Me+t jet since want to minimise the use of Missing ET at startup Stacked Scaled to 100pb-1 from 1st physics run Signal: 195.8 W+jets: 27.5 ttbar+jets: 10.4 Z->ee: 17 S/√(S+B) ~26 Contribution of QCD is currently being evaluated

  12. IOP Lancaster Conclusions • Presented a brief description of some of the aspects of selecting and reconstructing Z->tt->e+t jet events • Performance of the algorithms was discussed • For 100pb-1 we have ~200 Signal with ~ 55 Bkg events (QCD omitted) • Effect of QCD is currently being studied. • Methods for extracting the number and shape of background events from data were discussed • Finally data driven methods for measuring the “per jet” t tagging efficiency are being studied.

  13. IOP Lancaster Backup

  14. IOP Lancaster Samples used • Data Sets used • Signal: Pythia Ztte+t jet with |h|e,t jet<2.5 70GeV/c2<mZ<110GeV/c2 • Pythia Zee |h|e<2.5 mZ>40GeV/c2 • Alpgen W+0,1,2 jets • Alpgen ttbar+0,1,2 jets • Pythia QCD pThat 25-170GeV

  15. IOP Lancaster Triggering on Z->tt->e+t jet events • Ideally a logical OR between Single Isolated e HLT (e HLT) and the X-channel et HLT should be used • However current trigger table designed for L=1032cm-2s-1 has low ETthreshold for eHLT • For startup L use only Single e HLT which is ideal for t tagging efficiency measurement “CMS HLT exercise” Table Very similar thresholds Gain of using et HLT on top of e HLT is minimal both at HLT and offline • However as L increases, e HLT ET threshold will need to increase accordingly • Gain of et HLT on top of e HLT will be more evident

  16. IOP Lancaster Look at isolation + leading track finding efficiency in Signal QCD 25<pThat<50 and QCD 50<pThat<170 t id tightening Seff/Beff , distribution Riso=0.45 Seff/Beff , distribution Riso=0.45 7.1 8.3 Full Sim QCD 50<pThat<170 Full Sim QCD 25<pThat<50 “Per jet” efficiency w.r.t jets that pass: ETt cand>20GeV, ET3x3HT/PTLdg>0.1, DhLdgTr-HTmax<0.1, Tighten cuts: Rsig=0.05, PTLdgTr>16GeV QCD_25_50 per jet S/B~22 QCD_50_170 per jet S/B~15

  17. IOP Lancaster Kinematic Variables

  18. IOP Lancaster Mass Resolutions

  19. IOP Lancaster Measuring Electron Rejection Efficiency on Electrons using Z->ee • Based on tag-probe method used by Egamma people • Use events triggered by Single Iso elec HLT • Tag: electron passing offline and HLT Id – Require only 1 per event • Probe: t candidate passing isolation but without applying e-rej criteria AND not collinear to Tag electron • Then plot M(tag-probe) for: • a) No e-rejection criteria applied. Events in window=Ntot • b) With reversed e-rejection (t-veto) criteria applied . Events in window=Nt veto • Contrary to tag-probe method of Egamma we define M(tag-probe) energy and direction of t candidate and not track information. • et veto=Nt veto/Ntot and hence can get the e-rej efficiencyee veto=1-et veto

  20. IOP Lancaster View of M(tag+probe) Probe = Ctf Track of 1-prong t candidate Probe = Calo Jet of t candidate EHTT3x3/PTLdgTr>0.1 No cut EHTT3x3/PTLdgTr<0.1 Combining good electron with calo t matching 2nd MCe from Z. Mass is recovered. Mass shape discrepancy due to HCAL. (extent of difference under investigation) Large lower tail since combining “good” electron with CTF track of calo t matching 2nd MCe from Z that does not appear in elec cand list (Bad elec)

  21. IOP Lancaster Feasibility of measurement Me+t jet for Z->ee and backgrounds with reverse e-rej (t veto) criteria applied Me+t jet for Z->ee and backgrounds with no e-rej criteria applied QCD omitted QCD omitted >100 times more Z->ee than backgrounds within window. Can easily extract Ntot and Nt veto and hence ee veto=1-Nt veto/Ntot and Ne veto=Nt vetox(1-et veto)/et veto Effect of QCD is under estimation

  22. Tau tagging efficiency measurement method (I) • Method based on CMS Note 2006/074 (see backup) (A. Nikitenko, A. Kalinowski ). ORCA based, 30fb-1 • Ratio of x-sections of Z→ll / Z→→l+-jet using events (l = e in this study) which fire single-lepton trigger • Detailed explanation of efficiency definitions in next slide • Parameters which can be extracted from data: • Nmease+tau-jet , Nmeasee, • Br(Z→ee), Br(Z→e+) from e.g LEP • Parameters known from MC or data: • Nbkge+tau- jet ,ee, effHLT, effmass reco

  23. IOP Lancaster Tau tagging efficiency measurement method (II) • Definition of efficiencies • Want to measure t tagging efficiency on as a pure sample of t jets as possible, so apply electron rejection selections with efficiency etq before t Id is applied • Definition of efficiency measured in note • For purpose of note Ldg Track finding efficiency was factored in efficiency • This is a global efficiency given that electron rejection criteria are satisfied • Efficiency as a function of t jet ET is underway

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