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Search for BSM Higgs Bosons with ATLAS Jochen Dingfelder University of Bonn On behalf of the ATLAS Collaboration SEARCH 2012 Workshop University of Maryland, March 17-19, 2012 Overview New prelim. results (4.9 fb -1 ) New prelim. results (4.6


  1. Search for BSM Higgs Bosons with ATLAS Jochen Dingfelder University of Bonn On behalf of the ATLAS Collaboration SEARCH 2012 Workshop University of Maryland, March 17-19, 2012

  2. Overview New prelim. results (4.9 fb -1 ) New prelim. results (4.6 fb -1 ) Published in PRD (1.6 fb -1 ) 2

  3. Fermiophobic Higgs • Suppressed Higgs couplings to fermions in 2HDM and Higgs triplet models Here: simple benchmark model (LEP) • no fermion-Higgs couplings • SM boson-Higgs couplings • Production: Vector-boson fusion and associated production with W/Z • Decays to γγ , WW, ZZ, Z γ Here: focus on H ➝ γγ γγ ⇒ larger σ× BR than SM for light Higgs ⇒ higher Higgs p T 3

  4. Fermiophobic Higgs ➝ γγ • Selection: (identical to SM H ➝ γγ ) • 2 isolated photons with p T > 40, 20 GeV • Di-photon mass: 100 < m γγ γγ < 160 GeV • 9 categories based on p Tt < 40 GeV • presence of γ conversions • γ calorimeter impact point • p Tt : related to di-photon p T ATLAS-CONF-2012-013 • Signal m γγ γγ model Crystal Ball (core) + wide Gaussian (tail) p Tt > 40 GeV • Background m γγ γγ model Exponential 4

  5. Fermiophobic Higgs ➝ γγ : Exclusion limits Largest excess at m H =125.5 GeV Including look-elsewhere effect: Significance: 1.6 σ Prob. of background fluctuation: 5% Observed m H exclusion: [110.0, 118.0], [119.5, 121.0] Expected m H exclusion: [110.0, 123.5] 5

  6. Neutral MSSM Higgs gluon-gluon fusion: gg ➝ h/H/A b-associated production: bbh/H/A • MSSM requires 2 Higgs doublets ⇒ 5 Higgs bosons: Φ = h, H, A ; H + ,H - • h/H and A nearly mass degenerate • 2 parameters at tree level: m A , tan β • Enhanced couplings to b and τ in large parts of parameter space σ bbh/H/A ∝ tan 2 β 6

  7. Tau signature and identification Hadronic τ decay ( τ had ): • Narrow, collimated jet • isolated energy deposits and tracks • large electromagnetic component • low track multiplicity ( 1 or 3 ) τ had identification • high leading track momentum fraction 7

  8. Neutral MSSM Higgs : Selection τ had + τ had e/ µ + τ had e + µ • Di- τ had trigger • 1 isolated e / µ with • 1 isolated e with p T > 25 / 20 GeV p T > 25 GeV • 2 τ had with • 1 τ had with • 1 isolated µ with p T > 45 / 30 GeV p T > 20 GeV p T > 20 GeV • Opposite charges • Opposite charges • Opposite charges • E T miss > 25 GeV • Di-lepton veto (Z, top) • E T miss + p T e + p T µ < 120 GeV (QCD suppression) • E T miss > 20 GeV (QCD) ΔΦ ΔΦ ( e ,µ) ,µ) > 2.0 rad • m T < 30 GeV (W) (top, WW, ZZ suppression) Multi- Z ➝ ττ jet top W+jet 8

  9. Neutral MSSM Higgs : Mass reconstruction • Visible mass : (invariant mass of visible tau decay products) • Effective mass: A.Elagin, P.Murat, A.Pranko, A.Safonov, Nucl. Inst. Meth. A654 (2011) 481 Effective mass • Missing mass calculator (MMC): • 7 unknown parameters: two “missing” 3-momenta, m νν • 4 constraints from E x miss , E y miss , m τ 1 , m τ 2 MMC mass ⇒ scan over ΔΦ ( ν , l ), ΔΦ ( ν , h ), m νν ⇒ weight solution according to probability of 3D angle in solution ⇒ MMC mass = Max. of weighted m ττ distribution 9

  10. Neutral MSSM Higgs : Background estimation Background estimation based on data control samples : • Z/ γ * ➝ ττ ττ from τ -embedded Z/ γ * ➝ µµ data sample • Multijet background from samples with same-sign charges and low E T miss or inverted lepton isolation • W+jets from high-m T (l,E T miss ) sample W+jets (OS) W+jets (SS) + other bkg • No significant charge correlation • Expect no large E T miss From high-m T control sample • Mostly non-isolated or fake leptons 10

  11. Neutral MSSM Higgs : Results τ had + τ had e/ µ + τ had e + µ 11

  12. Neutral MSSM Higgs : Exclusion limits σ × BR ( Φ ➝ ττ ) (m A , tan β ) plane • Assume only one resonance ( Φ ): • Need to assume specific 100% gg ➝ Φ or (c)MSSM scenario 100% bb Φ production • Here: m h max scenario (acceptances similar) • Useful to test arbitrary models ATLAS-CONF-2011-132 12

  13. Neutral MSSM Higgs : Exclusion limits Comparison of search channels Update to full 4.9 fb -1 data set & inclusion of b-tagging in progress! 13

  14. Charged Higgs • Predicted in Higgs doublet (e.g. MSSM) and triplet models • m H+ < m t : dominant production in top quark decays • m H+ > m t : gb → tH + production important, but more data needed • for tan β > 3, preferred decay mode is H ➝ τν (here: assume BR of 100%) τν : lepton + jets : τ had + lepton : τ had + jets 14

  15. Charged Higgs: Lepton + jets channel Selection: • 1 isolated e / µ with p T > 25 / 20 GeV _ • ≥ 4 jets (2 b-tagged) with p T > 20 GeV τ ➝ e/ µ νν • E T miss > 40 GeV if | Φ l,miss | > π /6 q E T miss × |sin( Φ l,miss )| > 20 GeV if | Φ l,miss | < π /6 _ q’ • Identify “hadronic side” by choosing combination of 1 b-jet and 2 light jets that minimizes Discriminating variables: generator generator level level Lower bound ~ Discriminates mass of charged between leptons boson (H + or W) from τ and W 15

  16. Charged Higgs: Lepton + jets channel Signal region: cos θ l * < - 0.6, m T (l,E T miss ) < 60 GeV Dominant background from top pairs ! Simulated with MC@NLO, normalized in -0.2 < cos θ * l < 1 Misidentified-lepton background determined from control sample with loosened lepton ID 16

  17. Charged Higgs: τ had + lepton channel Selection: • 1 isolated e / µ with p T > 25 / 20 GeV τ ➝ had ν • 1 τ had with p T > 20 GeV e/ µ • ≥ 2 jets ( ≥ 1 b-tagged) with p T > 20 GeV • Sum of primary-vertex track p T : ν ν Discriminating variable: E T miss • Background contributions with misidentified taus : µ: 0.05%, e: 1%, jets: 55% ; jet ➝ τ had mis-ID measured with W+jets • True-tau background taken from simulation 17

  18. A candidate event in τ had + lepton channel 18

  19. Charged Higgs: τ had + jets channel Selection: • τ + E T miss trigger • 1 τ had with p T > 40 GeV τ ➝ had ν q • ≥ 4 jets ( ≥ 1 b-tagged) with p T > 20 GeV _ • E T miss > 65 GeV q’ • E T miss significance: • jjb combination (hightest p T ) consistent m top Discriminating variable: • True-tau background estimated with τ embedding in µ+jets events (with top-pair like event topology) • Mis-id. tau background: as for τ had +lepton 19

  20. Charged Higgs: τ had + jets channel Multijet background estimated by fitting E T miss shapes to data . Multijet shape from control sample with inverted τ and b ID 20

  21. Charged Higgs: Exclusion limits ATLAS-CONF-2012-011 Tevatron limits: BR < 10-15% Combined 21

  22. Charged Higgs: Exclusion limits (MSSM) ATLAS-CONF-2012-011 Combined …we will probably be able to rule out low-mass charged Higgs with 2012 data, if it doesn’t exist! 22

  23. _ Charged Higgs: H + ➝ cs c ATLAS-CONF-2011-094 _ s e/ µ ν _ • H ➝ cs dominates for tan β < 1 • Require large E T miss and m T to suppress multijet background • Kinematic fit with W and top mass contraints to find best H + candidate T evatron • Set limits on BR(t ➝ H + b) assuming _ BR(H + ➝ cs) = 100% 23

  24. Doubly-charged Higgs H ++ H ++ H -- • Relevant e.g. in Higgs triplet , Little Higgs and Left-Right Symmetric models WZ, ZZ, W ± W ± , ttW • Select µ pairs with same-sign charges and p T > 20 GeV • Look for resonance in µ ± µ ± mass spectrum • No significant excess over SM background found 24

  25. Doubly-charged Higgs: Exclusion limits Assuming predicted cross Set limits on H ++ H -- pair production via section, set limits on BR Drell Yan process pp ➝ Z/ γ * ➝ H ++ H -- Tevatron (CDF) upper limit: 205-245 GeV 25 Phys.Rev.D 88 (2012) 032004

  26. NMSSM a 1 ➝ µ + µ - • NMSSM : introduces singlet scalar field to solve µ problem ⇒ 3 CP-even scalars (h 1 , h 2 , h 3 ) 2 CP-odd scalars ( a 1 , a 2 ) • a 1 can be very light ! m a1 < 2 m B Analysis: • Opposite-sign di-muons (P T >4GeV) • Likelihood ratio selection based on µ + µ - vertex χ 2 and µ isolation • Set limits by fitting to mass spectrum • Y region excluded 26 ATLAS-CONF-2011-020

  27. Conclusions • Various interesting BSM Higgs scenarios are being probed in parallel to SM Higgs search • No indication for BSM Higgs bosons yet … but lots of upper limits on cross sections/branching ratios • Searches continue with more data and improved methods ⇒ There is still significant room for BSM Higgs searches for the year ahead … and after! 27

  28. Backup Slides 28

  29. Fermiophobic Higgs ➝ γγ : Exclusion limits 29

  30. Fermiophobic Higgs ➝ γγ : Systematics 30

  31. MSSM Higgs sector • MSSM: 2 Higgs doublets ⇒ 5 Higgs bosons: h 0 (CP=1) , H 0 (CP=1) , A 0 (CP=-1), H ± • At tree level described by two parameters: m A , tan β = v u /v d • Fixed mass relations at tree level: • Upper mass bound modified by radiative corrections (depend on SUSY parameters, e.g. mixing in stop sector) 31

  32. MSSM Higgs production 32

  33. Estimation of Z ➝ τ τ Background • Reliable Z ➝ τ τ model important for low-mass Higgs • Desirable to use real data, but cannot be selected signal-free • Instead, use high-purity Z ➝ µ µ sample (~ signal-free due to small Higgs-µ coupling) 33

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