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LHC Higgs Searches Physics at the LHC, UK HEP Forum, Cosener’s 2011

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Presentation on theme: "LHC Higgs Searches Physics at the LHC, UK HEP Forum, Cosener’s 2011"— Presentation transcript:

1 LHC Higgs Searches Physics at the LHC, UK HEP Forum, Cosener’s 2011
C. H. Shepherd-Themistocleous PPD, Rutherford Appleton Laboratory

2 Outline Results from Higgs searches at the LHC
SM Higgs production and Decay Search for SM Higgs at low, medium and High masses Searches for non-SM Higgs EWK results (brief) Cosener's Forum C.H. Shepherd-Themistocleous - RAL

3 Luminosity ATLAS CMS At EPS reported on ~1 fb-1.
At LP many analyses used close to 1.7 fb-1 and even 2.3 fb-1.

4 Higgs Production Cosener's Forum C.H. Shepherd-Themistocleous - RAL

5 Higgs Decay Analyses can be classed in approximate mass ranges
Low (< 130 GeV) , medium ( GeV) high (> 200 GeV) Searches are characterized by BR and width. Cosener's Forum C.H. Shepherd-Themistocleous - RAL

6 best overall sensitivity Low mass H → gg , H-> tautau , VH-> bb
High masses WW and ZZ modes Intermediate masses WW key channel with best overall sensitivity Low mass H → gg , H-> tautau , VH-> bb Cosener's Forum C.H. Shepherd-Themistocleous - RAL

7 Key background cross sections

8 Low mass Higgs searches
Channels for mass range ~ GeV H →  Best sensitivity at low masses H →  Useful (potential in SUSY scenarios) H → bb Large BR but rather challenging

9 H → gg Rare decay through loops Irreducible gg backgrounds
Reducible from jets faking photons. jet-jet supression ~ 108 Require very good mass resolution. ECAL critical. Photon class (converted or not) plus region of calorimeter vary resolution. Used to define classes for analyses. Test of ECAL calibration using Z → ee peak.

10 Resolution comparison
Comparison of resolutions in ATLAS (black) and CMS (blue) using tuned MC. Best case barrel no conversions All categories combined

11 H → gg Both experiments divide data into quality classes.
Fit background plus signal shape No evidence of a signal – set limits 1.08 fb-1 1.6 fb-1

12 H→ gg ATLAS 1.08 fb-1 CMS 1.66 fb-1. No evidence for SM Higgs
Sensitivity currently 3-4 times SM.

13 H → tt Sensitivity in cleaner VBF (non-VBF also used) modes. Both use ll and l-had final states. Forward tagging jets suppress SM backgrounds. Main backgrounds: Z + jets (Z→ tt irreducible), W → ln+jets, diboson, top, QCD. Background suppression makes use of event topology CMS use visible mass, ATLAS use collinear approx. and estimate mtt. Fits peformed to spectra. ATLAS ee, em, mm channels QCD, W+jets, Z→ tt from data Other bg MC. CMS e-had example. QCD, W+jets from data Z → tt + rest from MC

14 H → tt Combination of large number of channels.
Sensitivity some way off SM, but also useful for SUSY.

15 H→ bb Dominant decay mode at low mass BUT QCD background huge.
Interesting because potentially provides information on Higgs to quark coupling. Searches in VH production and require b-tagging. Backgrounds V+jets, VV, top, QCD. CMS & ATLAS Z→ ll, W→ ln. CMS also Z → nn ZH → llbb CMS sensitivity rather larger than ATLAS’s

16 Intermediate mass Channels for mass range ~ 130-200 GeV
H → WW → llnn Greatest overall sensitivity to SM Higgs

17 H→ WW → llnn Excellent sensitivity where this BR is large 130-200 Gev.
Challenging Higgs mass cannot be reconstructed. Search both latest results cut based. Look for 2 opp. sign leptons , missing ET. Jets 0,1 both; 2 (VBF) CMS. Scalar Higgs - make use of Df(ll) cut. CMS Major requirements: Lepton Pt > 10 GeV, tight ID & Isolation removes QCD & W+jets contamination Large MET & Z  μμ, ee veto removes Drell-Yan contamination Class # of jets (PT > 30 GeV) & b-jet veto removes Top contamination Kinematic discriminants: Mll & ΔΦ (l+l-) mitigates pp  WW background MH–dependent cut optimization ATLAS similar. Use ETmissrel After ET and pT cuts

18 H→ WW → llnn ATLAS Mll after pT cuts on leptons ATLAS MT after all
0 jets 1 jet ATLAS Mll after pT cuts on leptons For 0 jet WW dominates for 1 jet increased ttbar. 0 jets 1 jet ATLAS MT after all other cuts

19 H→ WW → llnn 0 jets 0 jets 1 jet

20 H→ WW → llnn Main backgrounds WW, ttbar, D-Y, W+jets, WZ/ZZ.
Estimated from data for major backgrounds, minor use MC. ATLAS and CMS similar WW using high mass ll events where no/little signal. ttbar invert b tagging cut and extrapolate using tagging efficiencies. W+jets, QCD using fake rate derived from data. D-Y using ll events inverting Z veto cut and extrapolating. Example of ATLAS Expectations from MC and observation using data driven methods

21 H→ WW → llnn SM Higgs 147 < MH < 194 GeV at 95% CL.
Selection change 1.5 fb-1 1.7 fb-1 SM Higgs 147 < MH < 194 GeV at 95% CL. Expected sensitivity 136 < MH < 200 GeV SM Higgs 154 < MH < 186 GeV at 95% CL. Expected sensitivity 135 < MH < 196 GeV

22 High mass Channels for mass range > 200 GeV ZZ → 4l ZZ → 2l2n
ZZ → 2l2q ZZ → 2l2t WW→ln2q WW → 2l2n

23 H → ZZ(*) → 4l Clean signal 4 isolated leptons from common vertex. One or two Zs on shell. Full mass reconstruction. (4e, 4m, 2m2e) Backgrounds: Zbb, tt. Suppress with impact parameter and isolation requirements ZZ Continuum: Shape known at NLO. Rate obtained from Z yield in data & theoretical prediction for ratio of ZZ to Z cross sections PT 43 GeV 26 GeV 20 GeV 48 GeV M4μ = 201 GeV

24 H → ZZ(*) → 4l CMS Cosener's Forum C.H. Shepherd-Themistocleous - RAL

25 H → ZZ(*) → 4l Fits to mass spectra performed to extract limits
Cosener's Forum C.H. Shepherd-Themistocleous - RAL

26 H → ZZ→ ll nn Cut and count analyses in ee and 
Production of Z with large missing energy Cut and count analyses in ee and  Major backgrounds: Z+jets, ttbar, WZ Cuts on MET, MT, Δ (MET,jet) Residual backgrounds: ZZ (NLO+LO),WZ(NLO) from MC Z+jets estimated from +jet data. Non resonant ttbar & WW use e events

27 H → ZZ→ ll nn ATLAS CMS CMS 1.6 fb-1 , ATLAS 1.04 fb-1
Exclusion GeV (CMS) , GeV 95% CL Cosener's Forum C.H. Shepherd-Themistocleous - RAL

28 H → ZZ(*) → 2l2q Highest rate for Z channel
Events categorized by presence of 0, 1, 2 b-jets Mass reconstructed from l and jets. Major background: Z+jets ; ttbar suppressed by MET requirement CMS Use 5 angles of scalar H  ZZ  2l 2q in a likelihood discriminant Background shape, normalization  data sideband CMS Preliminary 1.04 fb-1 1.6 fb-1 Cosener's Forum C.H. Shepherd-Themistocleous - RAL

29 H → ZZ(*) → 2l2q Cosener's Forum C.H. Shepherd-Themistocleous - RAL

30 H → ZZ(*) → 2l2t Fake rate estimated from Z+jet sample.
New CMS analysis. One Z → ll ( 60 < m < 120 GeV); Z → thth , mth , eth em ( 30 < mvis < 80 GeV) Backgrounds: ZZ estimated using observed number of Z and ratio of SM s(ZZ)/s(Z). Reducible Z+jets, ZW+jets, ttbar ,QCD. non-isolated l or jet can fake th. Fake rate estimated from Z+jet sample. event eeet

31 H→ WW → ln qq x100 x100

32 Non-SM Higgs Tevatron BR limit : 0.15 – 0.2
Searches have started for possible non-SM Higgs. MSSM SUSY has 5 h,H0,A0,H+/-. CMS F → tt, H+ → tn. Make use of bbF production (large tanb no VBF) Significant improvement on previous results Tevatron BR limit : 0.15 – 0.2 Cosener's Forum C.H. Shepherd-Themistocleous - RAL

33 Doubly Charged Higgs Doubly charged pair produced H++ → l+l+,t+t+
Arises in models with extra Higgs triplets F++, F+, F0 Triplet responsible for small neutrino mass Unknown neutrino mass matrix  unknown branching ratios  broad search Below M ≈2MW, only leptonic decays 3l f.s. 3 or 4 leptons in final state used for search

34 All limits CMS Preliminary

35 CMS combination Expected exclusion mass range: 130 – 440 GeV
Analysed data between fb-1 Expected exclusion mass range: 130 – 440 GeV Observed exclusion mass range: , , GeV Cosener's Forum C.H. Shepherd-Themistocleous - RAL

36 ATLAS combination Expected exclusion mass range: 130 – 440 GeV
Observed exclusion mass range: , , GeV Cosener's Forum C.H. Shepherd-Themistocleous - RAL

37 p-values Probability of an upward background fluctuation as high or higher than observed in data Interpretation requires “look elsewhere effect” correction Cosener's Forum C.H. Shepherd-Themistocleous - RAL

38 Summary of Higgs searches
Large number of searches performed by both ATLAS and CMS. Impressive work on combinations of results Similar exclusion regions in each of the experiments. CMS: , , GeV ATLAS: , , GeV Excess in low mass range less significant than at time of EPS. Factor of 2 in integrated luminosity between EPS and LP. Hope for another similar factor this year.

39 W mass Huge production x-section at 7TeV Pile up a challenge
pdfs affect precision Kinematics important for precision measurement, pT dist. Cosener's Forum C.H. Shepherd-Themistocleous - RAL

40 TGCs Will profit from increased stats
Can search for evidence in NP in deviation from expectations or forbidden vertices. SM vertices WWZ, WWg forbidden ZZZ ZZg No anomalous coupling observed WW leptonic WW leptonic

41 THE END

42 Backup Cosener's Forum C.H. Shepherd-Themistocleous - RAL

43 Search potential wrt Tevatron
Ratio of int. luminosities LHC (40 pb-1) /TEV (5fb-1) ~ 1/100 For ratios of parton luminosities > 100 LHC wins (Fn of initial state) Pair production of Intermediate mass particles from gg, qg, qq Production of massive objects > ~ 1TeV Cosener's Forum C.H. Shepherd-Themistocleous - RAL

44 Add table for ATLAS Mode Mass Range Data Used (fb-1) CMS Document
H  γγ 1.7 HIG H  bb 1.1 HIG (NEW) H  ττ HIG H WW 2l 2ν 1.5 HIG H  ZZ 4l HIG H  ZZ 2l2τ HIG (NEW) H  ZZ 2l2j 1.6 HIG H  ZZ 2l2ν HIG Cosener's Forum C.H. Shepherd-Themistocleous - RAL


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