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Status Report on hbb Analysis Jyothsna Rani for the hbb group Andy, Avto, Marine, Tim, Boris All D0 Meeting 28 th January 2005 28 th January 2005.

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Presentation on theme: "Status Report on hbb Analysis Jyothsna Rani for the hbb group Andy, Avto, Marine, Tim, Boris All D0 Meeting 28 th January 2005 28 th January 2005."— Presentation transcript:

1 Status Report on hbb Analysis Jyothsna Rani for the hbb group Andy, Avto, Marine, Tim, Boris All D0 Meeting 28 th January 2005 28 th January 2005

2 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR2 Outline  Introduction  Higgs production  Signal kinematics  Analysis overview  Limits and Exclusion plots  Summary & Outlook

3 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR3 Introduction MSSM has pairs of Higgs doublet fields – H u couples to up-type quarks and leptons and H d to down- type – The ratio of their VEV ’s is defined as: tan  = / – 5 Higgs particles after EWSB: h 0, H 0, A 0, H +, H - – h 0 is ‘guaranteed’ to be light: m h0 < ~ 130 GeV (MSSM) TOP  5FNS BOTTOM  4FNS h 0, H 0, A 0 production at Tevatron

4 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR4 bh vs bbh Cross-section (fb) Inclusion of closed top loop diagrams Solid  4FNS Dashed  5FNS

5 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR5 Higgs Production and Large tan   Large tan  → enhanced bbh/H/A  At tree level, cross section rises like tan 2   A and h/H are produced simultaneously. CP odd Higgs CP even Higgs h H A Total cross section

6 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR6 Neutral MSSM Higgs Branching Ratio CP odd Higgs CP even Higgs tan  = 5 tan  = 40

7 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR7 Masses and Widths Using M. Spira’s HDECAY 3.101, tan  = 30

8 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR8 QCD Calculations at NLO Significant progress has been recently made by theorists –Have d  /dpT, d  /d  at NLO –Uncertainties from renormalization/ factorization scales variation –PDF errors evaluated following CTEQ prescription For generator cuts: |  | 15 GeV

9 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR9 MSSM Framework SUSY  Only recently did thorough investigations.  Have tan  enhancement factors in 5 MSSM scenarios at one-loop level.  Significantly different from tree level assumption of tan 2   Along the lines of the Tevatron SHWG studies  More importantly, have  ×BR enhancement factors in terms of tan  effective vs. tan 

10 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR10 MSSM scenarios Function of various SM/SUSY parameters: X t =A t -  cot , , M g, M q, etc. Loop level corrections to cross section and BR with

11 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR11 Pre-selection and Luminosity  Pre-selection cuts:  “at least three offline jets with lead jet pt > 20 GeV and two jets with pT >15 GeV (uncorrected) and |  | < 2.6”  Data collected during Nov 2002 – June 2004 with v9 – v12 Trigger List versions.  87.5M events corresponding to Integrated Luminosity 260 pb -1  Exclude Jet/MET badLBNs for v9 – v12 Trigger List.

12 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR12 Event Selection - Triggering NewOldLevel 3 * 5GeV4 * 5GeV L1: tower E T 2 * 25GeV 1 * 15GeV 3 * 15GeVL3: jet E T 3 * 8GeV 50GeV L2: jet E T  (E T >5GeV)  Three levels of triggering (old and new trigger version).  Efficiencies relative to offline selection of 68-80%, depending on Higgs Mass.

13 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR13 Event Selection - Offline Loose initial analysis cuts Optimized analysis cuts for each signal mass

14 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR14 Jet pT and  distributions  distribution JES corrected pT In Data after the Kinematical cuts.

15 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR15 MC Samples (Signal and Background) Signal Samples: –h(  bb)b, 3b final state with parton pT > 15GeV mh=90, 100, 110,120, 130 and150 GeV each 100K events using PYTHIA generator. Background Samples: –Heavy Flavor Multijet process “bbjj” (ALPGEN). –QCD Irreducible process “bbbb” (ALPGEN). –Fake Jets, “jjjj” (obtained from DATA). –ttbar (PYTHIA). –Z(  bb)+X (PYTHIA). –Z(  bb)+b (PYTHIA).

16 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR16 Analysis Overview Signal hb(120)  Signal:  at least 3 b-tagged jets  Invariant mass of leading jets at mh  Backgrounds:  “QCD heavy flavor” : bbjj, ccjj, cccc, bbcc, bbbb  “QCD fakes” : jjjj  “Other” : Z(bb,cc), tt  Kinematic cuts  Cut on ET of leading jets  Optimize for each Higgs mass  Look at the di-jet invariant mass of the leading ET jet combination.  Search for an excess of events consistent with a Higgs signal shape. Fitted Background Data

17 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR17 Background Estimation Full multi-jet data sample Double b- tagged data sample Calculate TRF (E T & 3 Regions of  ) Apply TRF Triple b- tagged background shape Fit outside to real triple b-tagged distribution Tag Rate Function Probability to b-tag a jet Cross-check of background estimation methods

18 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR18 HF Correction to Tag Rate Function Full multi-jet data sample Double b- tagged data sample Calculate TRF (E T & 3 Regions of  ) Fit with sum of the backgrounds Assuming only light jets, no HF HF Normalizatio n Calculate HF corrected TRF (E T & 3 Regions of  ) After the HF correction. bbjj, bbbb, ttbar, zb, jjjj (fakes from DATA)

19 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR19 Efficiency and Tag Rate functions SVT Loose

20 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR20 Double b-tag  Cross-check performed on double b-tagged events  ALPGEN bbj+bbjj samples  Tests:  TRF parameterization and background estimation methods  Trigger modelling  b-tagging efficiency and kinematic bias  Jet reconstruction efficiency and kinematic bias Before HF correction After HF correction

21 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR21 Double b-tag Mbb and Triple b-tag The 3-b background is also estimated using the MC and compared as a cross-check. Requiring the two jets to be b-tagged (Mbb) in double b-tagged events.

22 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR22 Triple b-tag background fit At the 95 % exclusion For tan  = 100

23 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR23Systematics  Acceptance uncertainties:  Higgs pT spectra (theory)  Trigger efficiency  Di-jet mass resolution  Jet reco/ID efficiency  Jet energy scale uncertainty  b-tagging efficiency  Background uncertainties: (roughly independent of mass)  Quality of the Tag Rate Function parameterizations (χ2)  Statistics of the 3 b-tagged data outside the signal region Totals: Signal ~ 20% Background ~ 3% IN Parcentage %

24 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR24 Exclusion Plot with 260pb -1 data  Exclusion limits are calculated using ROOT’s TLimit CL S = CL S+B / CL B  Sweep through tan , given mA Measured rate Tree Level Assumption

25 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR25 Exclusion Plot Tree Level Assumption

26 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR26 Future Projections  Using the expected (m A, tan  ) limit, future projections with higher Int. Lumi are made.  Sensitivity to tan  down to ~40 for mA=100GeV with 4fb -1 data and with the current assumptions and performances. Int Lumi in pb -1

27 ADM, 28th Jan 2005K. Jyothsna Rani -- TIFR27 Summary and Outlook  Improvements since Moriond 2004 result:  Better theoretical understanding.  Twice the amount of data.  Better b-tagging.  We believe we have the (almost) state of the art phenomenological interpretation of our measurements.  Future:  b-tag combination  Neural Network


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