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Higgs working group status report F'Cerutti and G'Unal on behalf of the Higgswg

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Title: Higgs working group status report F'Cerutti and G'Unal on behalf of the Higgswg


1
Higgs working group status reportF.Cerutti and
G.Unal on behalf of the Higgs-wg
  • Update since ATHENS physics workshop
  • SM discovery revisited Old channels and new
    ideas
  • Higgs properties (spin, couplings,
    self-coupling)te
  • SUSY Higgs
  • Getting ready for real data analysis
  • Plans for Rome Physics Workshop
  • Conclusions

2
Disclaimer
  • Many activities and people involved over the last
    year
  • since ATHENS 9 meetings with more than 80
    presentations
  • Not everything can be covered in this talk
    limited to few more recent items/developments
  • For complete list of recent notes and summary of
    current activities, analysis status see Higgs-wg
    web page (maintained by G.Unal)
  • http//atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/HIGG
    S/higgs.html

3
SM Higgs
  • TDR discovery channels mainly inclusive
    searches - look for mass peak over (unknown)
    continuous background (design robust analyses)
  • ttH with H-gt bb
  • H-gt g g
  • H-gt Z Z -gt 4 leptons
  • H-gt W W -gt lnln
  • EW Production mechanism reduces QCD background
    (tt, WWj, Zj) Vector Boson Fusion VBF
  • H-gt W W -gt ln ln (-gt ln jj)
  • H-gt t t -gt lnn lnn and -gt lnn hn

Discovery potential Scientific Note
2003-024 Bonn, Cracow, KEK, Mainz, Montreal,
Pisa, Sheffield, Tokio, Wisconsin
4
ttH, H-gtbb
  • Revisited recently by J.Cammin-Bonn SN 2003-024
  • Discovery potential similar to TDR loss due to
    better bkg. estimate recovered by improved
    Likelihood method used in mass reconstruction
  • Studies on background normalization,
    extrapolation
  • Use of mass sideband (very challenging)
  • Bkg. from ttjj events (reverse b tagging) mass
    shape correction from MC
  • Other ttH channels
  • H-gttt (Zivkovic,Tanaka)
  • H-gtWW (Leveque,Tanaka)
  • not discovery channels but useful for coupling
    measurements

(30 fb-1)
5
H-gt ZZ-gt 4 leptons
  • One of the most investigated channel
  • 4 m Cosenza, Frascati, Saclay, MPI, Dubna,
    Wisconsin, Athens, Thessaloniki
  • 4 electrons Wisconsin, Weizmann
  • 2e-2m Wisconsin
  • 2e-2t Weizmann (hopeless at low mass)
  • Important progress
  • Analyses revised with full simulation DC1
  • Use of multivariate techniques (NN and
    likelihood) in parallel to TDR cuts for reducible
    and irreducible bkg rejection (Cosenza-Frascati,
    Wisconsin)
  • Study of NLO/LO k-factors vs cuts for sign
    irr. Bkg (Wisconsin)
  • Study of bkg control samples and systematics
    (Cosenza-Frascati)
  • Relaxed iso-cut analysis 3 iso-lep 1
    Loose-iso-lep (Wisconsin)
  • Impact of noise and pileup on muon isolation
    investigated with full simulation negligible at
    low-luminosity (Dubna ATL-COM-PHYS-2004-037)

6
H-gt ZZ-gt 4 m
  • Mass resolution and selection efficiency studied
    with DC1 data deterioration with respect to TDR
    (both m-standalone and m-combined)
  • Some efficiency loss attributed to detector
    change (services in m-spectrometer) some to
    software problems
  • TDR performance reproduced also thanks to
    multivariate techniques a part for MH180-200
    GeV opening of ZZ on-shell background (probably
    not correctly taken into account correctly in TDR
    ?)

H-gt4m x 4
E.Meoni et al. ATLAS-PHYS-COM 2004-040
R.Nicolaidou et al.- Saclay
7
H-gt ZZ-gt 4e
  • Analyses performed on DC1 samples e-calibration
    (strong contribution of Wisconsin group) and
    e-isolation studied
  • TDR results reproduced a part for 180 GeV ! (as
    for 4 muons)

M.Riveline E.Gross Weizmann
8
H-gt ZZ-gt 4e and 2e2m
  • Proposed by Wisconsin looser lepton-isolation (1
    loose isolation required for 1 out of 4 leptons)
    slight improvement in significance 10 at the
    price of having a reducible background (Zbb) at
    similar level than the irreducible one

B.Mellado et al. Wisconsin ATL-COM-PHYS-2004-042
9
H-gt g g
  • Full simulated gg from DC1 used to check mass
    resolution performance Tartarelli-Carminati
    (Milan) also by Escalier (Paris) and Fang
    (Wisconsin)
  • Mass resolution 5-10 worse than in TDR (more
    material IDmore conversions) Still g-conversion
    identification from MC truth instead than from ID
    recon
  • Study of reducible background with full
    simulation using DC1 QCD samples Escalier,
    Loureiro(Wisconsin), Unal (LAL)
  • Study of NLO prediction for signal and
    irreducible background B.Mellado(Wisconsin),
    Unal, Escalier, Laforge
  • From inclusive to H n-jets analyses Mellado,
    Unal, Minagawa, Kanzaki (KEK), Escalier, Laforge

10
H-gt g g from DC1
  • Background from fake photons reevaluated using
    inclusive DC1 QCD-jj samples
  • Rejection similar to TDR studies (Wielers)
  • q-Jets less rejected than g-Jets (harder
    fragmentation function)
  • TDR estimate of gjet Bkg. was underestimated
    factor 2-3
  • Reducible B mostly q-jet for this process while
    rejection parameterized on QDC-jj sample
    dominated by g-jet !
  • To finalize this study
  • Tighter isolation cuts at low luminosity
  • Reconstruction of conversions with the tracker

G.Unal
11
H -gt gg NLO studies
  • Irreducible background exists at NLO (caveat
    LO and NLO not well defined for gg)
  • TDR computation LO cross-section for signal,
    BornBox production of gg (x1.5 to account for
    Bremsthralung contribution)
  • NLO computation NLO cross-section for signal,
    NLO contribution for gg Box at NLO

Irreducible bkg.
Born
LO
NLO
Box
(30 fb-1)
MH120 GeV L30fb-1
Significant uncertainty on MC background
predictions Background will be known much better
with the data !
12
H -gt gg From inclusive to H jets ?
  • Studies based on NLO MC
  • Comparison of gg1 jet with inclusive gg channel
    (old idea used by CMS, no conclusion in TDR
    because of lack of NLO computations)
    (Mellado,Unal)
  • Use other variables than Mgg to discriminate
    Signal and Background, for instance Pt gg
    (Escalier,Laforge)
  • Better S/B can be achieved
  • VBF H-gtgg channel investigated much better S/B
    but less statistical sensitivity (50
    inclusive)
  • Mellado et al.-Wisconsin ATL-PHYS-2003-036
  • Minagawa, Kanzaki Tokyo-KEK
  • VBF and inclusive channels can be combined

13
H-gt W W
  • Inclusive channel used in TDR counting
    experiment with small shape difference Signal vs
    Background
  • VBF production better significance -gt reach
    lower Higgs masses (down to 120 GeV
  • Recent developments
  • NLO computation for S and B (mostly WW, tt) for
    inclusive TDR channel (M.Duehrssen-Freiburg)
  • Shape of WW background at NLO shape of
    SignalBackground at LO (MH170 GeV) !
  • Study of VBF analysis re-optimization with
    multivariate techniques NN (improvement 30-40
    on significance) and NLO bkg. Estimate (Cranmer
    et al. - Wisconsin). Includes studies on bkg.
    control samples
  • New idea Combine WW0 jet (TDR), WW2jets
    (VBF) and WW1 jet (one jet forward) Quayle
    et al. - Wisconsin. Statistical sensitivity looks
    promising.

14
VBF H-gt t t
  • Key Issue here is Z-gttt mass tails need to study
    on full simulation
  • VBF analysis of DC1 fully simulated events
    started K.Cranmer-Wisconsin and
    I.Rottlaender-Bonn Problems with PT-miss
    calibration
  • Recent development (Mellado et al.Wisconsin
    ATL-PHS-COM 2004-023)
  • H -gt tt 1 jet , jet in intermediate h region
  • Expected to be less sensitive to detector
    systematics/calibration
  • intermediate jet tagging hJgt1
  • more relaxed jet veto in central region 30
    GeV
  • Statistical sensitivity good from fast simulation
  • Need higher order QCD correction for Bkg estimate
    and control samples from data (study started by
    Wisconsin)
  • Strong correlation with VBF channel combination
    difficult ? Choose one of the two (But VBF
    important for coupling measurement) ?

15
Higgs properties
  • Scientific note on H spin/parity measurement for
    M(H)gt200 GeV from H-gt ZZ -gt 4-leptons SN 2003-025
    (Buszello et al.)
  • At low-mass studies started measure CP in tth
    h-gtbb (Hockeppel Bonn) or in tth h-gtgg
    (McGarvie -Royal Holloway)
  • Measurement of ratios of couplings. Use all
    channels available. New study completed by
    M.Duehrssen ATL-PHYS 2003-030
  • Update on H self-coupling (Dhahloff-Freiburg)
    disagreement on tt bkg. with previous studies
    (F.Mazzucato Geneva)

some (moderate) assumptions no significant
contributions in loop from new particles and
light quarks, only one Higgs boson
16
SUSY Higgs
17
CP SUSY Higgs
  • New scenarios with CP violating SUSY couplings
    investigated
  • Couplings to SM particles are changed (production
    and decay)
  • Particularly challenging scenario suggested by
    theorist (Carena et al) H1 decouples from gauge
    bosons Very light H1 escapes LEP searches
  • Most of the parameter space covered with existing
    searches
  • Some holes left at very low MH1 under
    investigation recovered with specific topologies
    like H -gt WH1 ?

Preliminary
M.Schumacher - Bonn
18
Charged Higgs in the transition region
  • Study of charged Higgs in the transition region
    MHMtop performed K.Assamagan et al.
  • Preliminary study has been performed with fast
    simulation and is reported in ATL-COM-PHYS-2004-00
    9
  • Look for gg-gtbtH with H -gt tn 2-gt3 process
    with correct treatment of transition region (from
    on-shell to off-shell t) HERWIG version 6.4
  • Gap in transition region covered

Preliminary
19
Getting ready for real data
  • More details see report to Physics
    commissioning meeting July 2004 (FC)
  • First step Detector performance and calibration
  • e/m/t/g identification and measurement
  • jet reconstruction (forward tagging jets
    Zjet statistics will be limiting),
  • PT-miss calibration
  • ? performance groups
  • Second step estimate of background from
    data/control samples
  • Bkg estimate easy in principle for some
    inclusive channels (gg, 4-leptons)
  • More involved for more exclusive channels (like
    VBF WW, tt)
  • Bkg. Normalization measure of SM processes
    (ttnj, Wnj, Znj, WWnj, ggnJ with n0,1,2,)
    ? SM, QCD and top groups
  • Clear strategies on extrapolation from control
    samples to signal region
  • Higgs could be discovered (statistically) with
    10 fb-1 crucial to have detector
    calibration/performance and SM background
    understanding with first collected samples (we
    have 1 concurrent exp.)

20
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21
Participation to DC2
  • Higgs working group has requested SB samples for
    first DC2 phase and beyond work organized by
    B.Mellado-Wisconsin
  • http//www-wisconsin.cern.ch/bmellado/MC/
  • Larger samples (mainly background) will be needed
    to finalize some analyses
  • Validation of generators/ATLFAST for signal
    performed
  • First look at DC2 fully simulated/reconstructed
    events still long way to go for FULL DC2
    validation

S.Paganis - Wisconsin Very first look !
22
Plans for Rome physics workshop
  • Complete DC1 based re-analysis of gg and 4-lepton
    channels write SN notes with updated results
  • Finalize systematic studies of VBF tt and WW
    channels including impact of full simulation
    background systematics included based on control
    samples studies
  • Consistent update of SM discovery sensitivity
  • DC2 based analyses for Rome ? Difficult to get
    final results probably validation and some
    particular cross-checks (NLO samples, initial
    detector layout)
  • Measurement of some of the Higgs properties in
    the low mass region (CP, spin, self-coupling) to
    be revisited
  • Finalize updates on some MSSM channels

23
Conclusions (1)
  • Quite impressive amount of work performed in the
    Higgs working group since ATHENS
  • Improvement in understanding of signal and bkg
    processes (MC_at_NLO, RESBOS, K-factors)
  • Intensive use of DC1 data
  • Validation of full simulation
  • Impact of detector layout change
  • More realistic performance taken into account
  • Studies on control samples to estimate bkg. Size
    and uncertainty started in many channels
  • Complementing TDR inclusive channels with more
    exclusive ones (in addtion to VBF WW and tt)
  • H-gtgg1 jet, VBF H-gtgg
  • H-gttt 1jet
  • H-gtWW 0,1,2 jets

24
Conclusions (2)
  • Problematic issues
  • Full simulation with calibrated objects needed
    to finalize realistic analyses PT-miss
    calibration, forward jet calibration,.
  • Interaction between performance/sub-detector
    experts and Higgs wg very important November
    Physics Week is a very good opportunity/idea
  • Validation of full simulation/reconstruction
    still an issue
  • Some DC1 problems survived in DC2 production ?
  • DC2 validation difficult issue many things
    changed at the same time

25
Other developments/ongoing works not covered here
  • VBF H-gtZZ-gtqqll large mass K.Cranmer et al.
    Wisconsin, Weizmann
  • Update of VFB H-gtWW for masses 150-300 GeV
    K.Cranmer et al. Wisconsin
  • ttH with H-gttt L.Zivkovic et al - Weizmann,
    R.Tanaka - Okayama
  • h0-gta1a1-gtbbtt in NMSSM S.Baffioni-LAL
  • MSSM H/A -gt tt -gt ll nnnn T.Szymocha et al. -
    Cracow
  • WH, ZH with H-gtbb J.Vossebeld et al. - Liverpool
  • ttH with H-gt invisible B. Kersevan - D.Schroff
    - Freiburg
  • H -gt WH with H-gtbb B.Mohn et al. - Bergen,
    Uppsala
  • tt -gt WbHb X.Portell et al. - IFAE
  • Studies of NLO corrections to VBF cross section
    R.Mazini-Toronto
  • ZH with Z-gtnn and H-gtgg G.Azuelos et al. -
    Montreal
  • MSSM h-gtmm for Mh100 GeV S.Gentile et al -
    Rome/Fascati
  • Impact of PDF uncertainty on H production Paris,
    Montpellier
  • Trigger efficiency for H -gt4e - V.Perez-Real-Bern
  • t-ID algorithm in fast simulation L.Zivkovic
    and E.Gross
  • Almost all the studies documented in ATLAS notes

26
Spare slides
27
Introduction (1)
  • SM Higgs focus on low mass region- 115-250 GeV
    TDR discovery channels mainly inclusive
    searches - look for mass peak over (unknown)
    continuous background (Design robust analyses)
  • ttH with H-gt bb
  • H-gt g g
  • H-gt Z Z -gt 4 leptons
  • H-gt W W -gt lnln
  • EW Production mechanism strongly reduces QCD
    background (tt, WWj, Zj) Vector Boson Fusion VBF
    entered in the game
  • H-gt W W -gt ln ln (-gt ln jj)
  • H-gt t t -gt lnn lnn and -gt lnn hn
  • (H-gt g g)

28
Introduction (2)
  • Comments on VBF
  • Improvement in difficult region 120 GeV
  • Important contribution to coupling measurements
    more channels available at each mass (redundancy)
  • Larger S/B w.r.t. inclusive channels
  • Involves difficult detector aspects forward
    jet calibration, central jet veto, PT-miss
  • Control samples to estimate the background from
    the data (counting experiments)
  • Opened Issues on SM Discovery Potential
  • non-VBF channels are from TDR Change in
    detector performance/layout ?
  • LO Cross-section used for H production
    (conservative) NLO computations/generators for
    S and B ?
  • Only some aspects (forward jet tagging, jet
    veto) studied with full simulation Need to fully
    validate VBF results with up to date full
    simulation

VBF Discovery potential VBF Scientific Note
2003-024 Bonn, Cracow, KEK, Mainz, Montreal,
Pisa, Sheffield, Tokio, Wisconsin
29
H-gt g g from DC1
Tratarelli-Carminati
  • Mass reconstruction studied on DC1 samples
    special corrections/calibration
  • Still g-conversion identification from MC truth
    instead than from ID recon.
  • Mass resolution 5-10 worse than in TDR
  • (more material IDmore conversions)

30
From inclusive gg to gg jet(s) exclusive final
states Clear trend in S/B. S/sqrt(B) precise
predictions difficult
G. Unal
For VBF H-gtgg studies from Wisconsin
ATL-PHYS-2003-036 and Minagawa VBF and inclusive
can be combined
31
t-identification
  • Crucial for several channels VBF H-gttt, ttH with
    H-gttt, MSSM H/A-gttt with different pt and event
    topologies
  • t-id with full simulation (-gt detector
    performance group)
  • D.Cavalli, M.Heldman standard tau
    identification optimization with full simulation
  • Alternatives t-id algorithm E.Richter-Waas
    (track based), J.Tanaka
  • Problems with t-ID in fast simulation standard
    ATLFAST parameterization is not working at low-Pt
    and has a strong process-dependence (L.Zivkovic
    and E.Gross)
  • Attempt to perform an event by event t-ID in
    ATLFAST (Weizmann) using fast-shower variables
    (Mainz)
  • Not yet satisfactory results obtained with both
    approaches work in progress
  • All channels containing taus studied with fast
    simulation ONLY must be validated with full
    simulation

32
Example tt 1 jet B.Mellado et al. Wisconsin
(Atlfast)
5 sigma for MH120 GeV for 30 fb-1
33
MSSM Higgs
  • New scan for typical scenarios performed by
    M.Schumacher
  • Atlas note on the way

tt reach for (30 fb-1)
(300 fb-1)
34
Trigger issues
  • Study of impact of new HLT menu on Higgs channels
    performed in collaboration with HLT-TDAQ group
  • http//cerutti.home.cern.ch/cerutti/new_trigger_me
    nu.html
  • Inclusive approach is in general good no need of
    more exclusive triggers
  • Most problematic channels
  • bbh/A with h/A-gtbb (MSSM)
  • VBF H-gtbb (SM couplings)
  • VBF H-gt Invisible
  • Possible solutions for 4-b channels under study
    J.Kanzaki and I.Vivarelli b-tag at LVL-2 with
    looser PT-jet
  • Trigger efficiency for H -gt 4e channels studied -
    V.Perez-Real-Bern no significant loss between
    LVL1 and offline recon.
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