Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.04 1 Analysis of Invisible Higgs production in the tth channel Introduction Analysis overview.

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Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.04 1 Analysis of Invisible Higgs production in the tth channel Introduction Analysis overview Results so far Comparison to reference Kinematic fit Conclusion Ricardo Goncalo Pedro Teixeira-Dias

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.042 Introduction Motivation: Motivation: –Several scenarios for physics BSM predict a significant invisible branching ratio –Complementary to the VBF channel with invisible Higgs Build upon work done at Royal Holloway: Build upon work done at Royal Holloway: (E.Brambilla, talk at Higgs WG meeting, May 2002; T.L.Cheng, MSc.Thesis, available at: Aim to reproduce and build upon results from previous analysis: Aim to reproduce and build upon results from previous analysis: (B.Kersevan, M.Malawski, E.Richter-Was, Eur. Phys. J C29 (2003) 541, ATL-COM-PHYS ; M.Malawski, MSci Thesis, hep-ph/ )

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.043 Analysis overview Cut-based analysis Only signal and tt backg so far Difficulties: Two components of missing momentum: cant reconstruct t b l Two components of missing momentum: cant reconstruct t b l ttbar is the most significant background and is very similar to signal ttbar is the most significant background and is very similar to signal Signal/Background ~10 -3 Signal/Background ~10 -3 Process xBR xBR tth330 (*) fb tt fb bbW, W l fb bbZ, Z l + l fb ttW, W l 420 fb ttZ, Z 190 fb (*) =520 fb in reference analysis, with SM couplings

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.044 Cuts Reference analysis cuts: 1 electron (p T >25GeV; | | 25GeV; | |<2.5) or 1 muon (p T >20GeV; | | 20GeV; | |<2.5) Veto on additional electron (p T >10GeV) Veto on additional electron (p T >10GeV) or additional muon (p T >6GeV) 2 b-tagged jets 2 b-tagged jets 2 or more un-tagged jets 2 or more un-tagged jets t bjj reconstruction: t bjj reconstruction: –|m jj -m W |<15GeV; | |<2.0 for jets in W jj –|m bjj -m t |<25GeV m T > 120 GeV m T > 120 GeV Missing E T > 150GeV Missing E T > 150GeV Scalar sum of p T of reconstructed l j j b b: E T >250GeV Scalar sum of p T of reconstructed l j j b b: E T >250GeV In reconstructed W jj: R jj = ( 2 jj + 2 jj ) < 2.2 (to reject lep-tau decays) In reconstructed W jj: R jj = ( 2 jj + 2 jj ) < 2.2 (to reject lep-tau decays)

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.045 Simulation Channel: Higgs (m h = 120 GeV) decaying to neutralinos in MSSM Channel: Higgs (m h = 120 GeV) decaying to neutralinos in MSSM –(tan = 5, m A = 1 TeV; M 1 = 44 GeV, M 2 = 220 GeV, M 3 = 1 TeV) PYTHIA for signal and background PYTHIA for signal and background Generated 60 M tt + 10 M tth Generated 60 M tt + 10 M tth Atlfast simulation, ATLAS release Atlfast simulation, ATLAS release –Low luminosity setting –Cone jets (R cone = 0.4) –Jet tagging: b jets 60%; c mistag 10%; u,d,s, mistag 1% –CTEQ5L PDFs –m top = 175 GeV (..historical) Interfaced code to Atlfast within Athena to produce dedicated ntuple Interfaced code to Atlfast within Athena to produce dedicated ntuple

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.046 The truth! At parton level: At parton level: –tops back-to-back in background –more mercedes star-like in signal –Most missing p T from Higgs decay (especially in had-had channel) tt t t t h (,E T miss ) (h,E T miss )

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.047 Signal and tt background Transverse mass, E T and E T miss are good discriminating variables Transverse mass, E T and E T miss are good discriminating variables m T has sharp edge for tt background at ~m W m T has sharp edge for tt background at ~m W But background xsection ~1000 times higher than signal But background xsection ~1000 times higher than signal Tails of background distributions very large Tails of background distributions very large No cuts; Lumi = 1fb -1 m T (GeV) ttbar tth E T miss (GeV) E T (GeV)

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.048 Results so far… Relaxed E T miss cut to 120GeV wrt reference analysis Relaxed E T miss cut to 120GeV wrt reference analysis Background much higher than tth Background much higher than tth Signal and background normalized to 30 fb -1 Signal and background normalized to 30 fb -1

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.049 Results so far… Most background comes from lep-tau and lep-lep decays of tt, as concluded in reference paper Most background comes from lep-tau and lep-lep decays of tt, as concluded in reference paper decays increase the missing E T decays increase the missing E T W jj reconstructed from ISR/FSR jets in lep-tau and lep-lep events W jj reconstructed from ISR/FSR jets in lep-tau and lep-lep events lep-leplep-tautau-tau lep-had had-had

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.0410 Results so far… Main problem in tt background is the lep- tau channel decays with fake W jj Main problem in tt background is the lep- tau channel decays with fake W jj tth signal much more pure wrt W jj (were looking at the tails of tt background) tth signal much more pure wrt W jj (were looking at the tails of tt background) Not much point in rejecting taus in Atlfast, must look for other possibilities Not much point in rejecting taus in Atlfast, must look for other possibilities

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.0411 Results so far… No cut found so far that can be targeted at lep-tau and lep- lep channels in tt production in addition to what was found in the reference analysis No cut found so far that can be targeted at lep-tau and lep- lep channels in tt production in addition to what was found in the reference analysis

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.0412 Results so far Accepted events for 30 fb -1 tth x-section scaled to SM value as used in reference analysis tth x-section scaled to SM value as used in reference analysis tth: x-section= 520 fb -1 tth: x-section= 520 fb -1 Signal = 44.3 events Signal = 44.3 events tt: x-section= fb -1 tt: x-section= fb -1 Background= 812 events Background= 812 events S/ B = 1.55

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.0413 Comparison with reference analysis Cumulative efficiency of cuts: Reasonable agreement with reference analysis: ~10-20% for signal (check column) Reasonable agreement with reference analysis: ~10-20% for signal (check column) Agreement wrt tt background efficiency becomes worse (factor 1.35 – 2.8) for cuts after m T cut Agreement wrt tt background efficiency becomes worse (factor 1.35 – 2.8) for cuts after m T cut Testing all t bjj combinations against m W and m t gives efficiency ~30% better wrt cross check (this analysis column) both for signal and background (small) net gain in significance Testing all t bjj combinations against m W and m t gives efficiency ~30% better wrt cross check (this analysis column) both for signal and background (small) net gain in significance CutReference tth Cross check tth this analysis tth Reference ttCross check tt this analysis tt Lepton22%23.6% 22%23.6%23.7% Jets/b jets5.0%5.7% 4.9%5.01%5.02% t bjj 2.6%2.9%3.4%2.4%2.60%2.98% mTmT 0.87%1.12%1.33%0.041%0.055%0.063% E T miss 0.41%0.51%0.67%2.0x x10 -5 ±0.64.9x10 -5 E T 0.40%0.50%0.67%2.0x x10 -5 ±0.64.6x10 -5 R jj 0.28%0.33%0.44%7.5x x10 -5 ±0.52.8x10 -5

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.0414 mWmW W b t e/ mtmt Kinematic fit Tried something different: Assume p T miss comes from and h only Build grid of points in p T and (l, ) and calculate p Z p Z can be found from p T and p lep assuming W on mass-shell From p b, p and p lep, calculate m t for each point Propagate errors in m t from grid spacing to obtain mt and calculate 2

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.0415 Kinematic fit results Kinematic fit ~works for signal: (p T h )~85GeV Kinematic fit ~works for signal: (p T h )~85GeV Will try to use fit results for discrimination against tt background Will try to use fit results for discrimination against tt background The hope is that this allows other cuts to be relaxed The hope is that this allows other cuts to be relaxed Correlations to m T and E T miss may be important Correlations to m T and E T miss may be important

Ricardo Gonçalo - RHUL Higgs WG meeting - Physics Week - Oct.0416 Conclusions Major background to tth has been studied Major background to tth has been studied Reasonable agreement with reference analysis – still work to be done to find remaining differences Reasonable agreement with reference analysis – still work to be done to find remaining differences Some improvement in significance may be achieved by different reconstruction of t bjj Some improvement in significance may be achieved by different reconstruction of t bjj Simple kinematic fit to semileptonic top decay may be useful to discriminate against background Simple kinematic fit to semileptonic top decay may be useful to discriminate against background