search for the higgs boson in h zz (*) decay modes on atlas german d carrillo montoya, lashkar...
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![Page 1: Search for the Higgs boson in H ZZ (*) decay modes on ATLAS German D Carrillo Montoya, Lashkar Kashif University of Wisconsin-Madison On behalf of the](https://reader036.vdocuments.mx/reader036/viewer/2022070414/5697c01c1a28abf838ccfcf6/html5/thumbnails/1.jpg)
Search for the Higgs boson in H->ZZ(*) decay modes on ATLAS
German D Carrillo Montoya, Lashkar KashifUniversity of Wisconsin-Madison
On behalf of the ATLAS Collaboration
DPF 2011, Brown University, Rhode IslandAugust 9, 2011
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Introduction
• H->ZZ branching ratio is large for MH > 2 MZ, second to the WW branching
• Requiring at least one real Z leads to three channels: llqq, llnn, llll
• For each, will summarize selection, results and limit curves with 2011 data
DPF11, August 9, 2011G.D. Carrillo Montoya, L. Kashif
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• These analyses based on 1.04 – 1.21 fb-1 data from March to June 2011
• Error on luminosity: 3.7%
• Already sensitive to Higgs signal in wide range 130 GeV < MH < 500 GeV
Data sample
DPF11, August 9, 2011
Dataset used in these analyses
G.D. Carrillo Montoya, L. Kashif
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The H ->ZZ -> llqq channel
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• High-pT lepton pair + 2 jets signature
• Search region: 200 GeV< MH < 600 GeV
• Bin by b-tagging: 2 b jets (tagged), <2 b jets (untagged)
Event selection
• Isolated same-flavor lepton pair
- pT > 20 GeV, 76 GeV < mll < 106 GeV
• No additional lepton in event
• At least 2 jets, with pT > 25 GeV, |h| < 2.5, 70 GeV < mjj < 105 GeV
• ETmiss < 50 GeV
• High mass (MH > 300 GeV): pT (jets) > 50 GeV, Dfll < /2, p Dfjj < /2p
G.D. Carrillo Montoya, L. Kashif
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llqq: kinematics
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llqq: backgrounds
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Z + jets: Main background
o Normalized using sidebands in mjj
o Uncertainty <10% for untagged sample, ~20% for tagged sample
Top: MC expectation validated using sidebands in mll
o ~10% theory uncertainty
QCD: data-driven techniques
o Template fit method in ee channel
o ‘ABCD’ method in mm channel using isolation and mmm
Diboson: MC-derived, ~10% theory uncertainty
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llqq: results
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• Look for bump in dilepton-dijet invariant mass spectrum
Untagged sample, MH = 400 GeV Tagged sample, MH = 400 GeV
• Observed spectra consistent with background in both untagged and tagged samples
DPF11, August 9, 2011G.D. Carrillo Montoya, L. Kashif
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llqq: limits
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MH [GeV]
• Expected limits 2.7 - 9 times SM cross-section
• Observed limit at 1.7 times SM cross-section around MH = 360 GeV
DPF11, August 9, 2011G.D. Carrillo Montoya, L. Kashif
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The H ->ZZ -> llnn channel
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• High-pT lepton pair + ETmiss signature
• Search region: 200 GeV< MH < 600 GeV
• Cuts optimized for low mass (MH < 280 GeV) and high mass regions
Event selection
• Isolated same-flavor lepton pair
• No additional lepton in event
• No b-tagged jet
• Low mass: ETmiss > 66 GeV,
Df(j1, ETmiss ) > 0.3, 1 < Dfll < 2.64
• High mass: ETmiss > 82 GeV,
Df(j1, ETmiss ) > 0.3, Df(Z, ET
miss ) > 1, Dfll < 2.25
mll [GeV]
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ll nn : backgrounds
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Main backgrounds: Top, diboson
Diboson: MC-derived, ~10% theory uncertainty
Top: MC expectation validated in data using sidebands in mll and with b-jet requirement
o ~10% theory uncertainty
W + jets: partially data-driven
o MC expectation normalized using W + jets control region requiring same-sign lepton pairs
QCD: small contribution
o data-driven techniques used as for llqq
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ll nn : results
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• Look for bump in transverse mass distribution:
• Observed distributions consistent with background, although a few interesting Z + ET
miss events seen
DPF11, August 9, 2011G.D. Carrillo Montoya, L. Kashif
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ll nn : an event of interest (thanks K. Nicolopoulos)
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llnn : limits
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MH [GeV]
• Expected limits 1.2 - 7 times SM cross-section
• Observed limits are better: this channel excludes SM Higgs in range 360 GeV < MH < 420 GeV at 95% CL
DPF11, August 9, 2011G.D. Carrillo Montoya, L. Kashif
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The H ->ZZ -> llll channel
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• So-called ‘golden’ channel: small cross-section, but very clean signature
• Search region: 110 GeV< MH < 600 GeV
Event selection
o Two pairs of isolated, same-flavor, opposite-sign leptons
o Label leptons with mll closest to mZ as 1,2, and the other two leptons as 3,4
o |m12 - mZ| < 15 GeV
o m34 < 115 GeV, m34 > mthreshold
with mthreshold defined as a function of the 4-lepton invariant mass mllll
o For mllll < 190 GeV, impact parameter
cuts on leptons 3,4G.D. Carrillo Montoya, L. Kashif
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llll : backgrounds
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Main background: ZZ -> 4l
o Normalized using MC
o ~15% theory uncertainty
• Remaining backgrounds are top and Z + jets, both suppressed by lepton isolation and impact parameter cuts
Top: MC expectation validated in data
o ~10% theory uncertainty
Z + jets: normalized using control regions
o Defined by eliminating isolation and impact parameter criteria on one lepton pair
o Estimated separately for heavy flavor decay leptons, fake leptons and leptons from EW sources
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llll: results and limit curve
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• Observed 4-lepton invariant mass spectrum consistent with background expectation
• Expected limit ~1.8 times SM cross-section at MH = 200 GeV
• Some fluctuations in observed limit due to single events
DPF11, August 9, 2011G.D. Carrillo Montoya, L. Kashif
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DPF11, August 10, 2011 17
• We have presented ATLAS Higgs search results in three final states from the H -> ZZ(*) decay
• The channels are mostly sensitive for MH > 200 GeV, except 4-lepton channel which has sensitivity at lower masses
• The H->ZZ -> llnn channel excludes Standard Model Higgs in mass range 360 GeV < MH < 420 GeV at 95% confidence level
• The LHC is increasing our dataset fast
-> expect new results soon
• Analysis improvements meanwhile
Conclusion and outlook
ATLAS SM Higgs combination
G.D. Carrillo Montoya, L. Kashif