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Susy Searches In Multilepton Final States

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Leptons in susy processes are mainly produced in ?20,?1 decays ... correlation matrix and was implemented in /PhysicsTools by Christophe Saout (KIT) ... – PowerPoint PPT presentation

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Title: Susy Searches In Multilepton Final States


1
Susy Searches In Multilepton Final States
  • Martin Niegel
  • Karlsruhe Susy Group
  • Karlsruhe Institute of Technology

2
Introduction outline
A
  • Introduction
  • Leptons in susy processes are mainly produced in
    ?20,?1 decays
  • ?20,?1 are mainly produced in direct ?20?1
    pair production or in gluino, squark cascade
    decays
  • decay topology is related to region in the
    m0-m1/2 space
  • Outline
  • Results of PTDR trileptons from ?20?1
    production at LM9
  • Introduction of a multilepton susy search in
    inclusive mode

B
C
3
Trileptons from ?20?1 pair production
  • Exclusive search for ?20?1? 3l no jets
  • Tuned to LM9 (m0175,m1/21450,tanß50)
  • m(?10)65GeV, m(?20,?1 )120GeV
  • Backgrounds ZW,ZZ,WW,ttbar,Zjets,Wjets
  • Soft leptons and small MET due to light ?10 and
    small mass difference ?20,?1 to ?10

D(m(?20,?10 ))
MET
invariant mass
pt of first lepton
4
Results for 30fb-1
Not a first day physics channel!
  • trigger streams
  • DiMuon stream (Ptgt 5 GeV) 75
  • DiElectron stream (Ptgt17 GeV) 25

selection cuts NJets 0,Nlgt2,NOSSFgt0 Jets
itCone5, Jet_ptgt30GeV, etalt2.4 Muons
ptgt10GeV,etalt2.4 Electrons pt(1,2)gt17GeV,
ptgt10GeV,etalt2.4
Dilepton invariant mass
Discovery reach
5
Multilepton inclusive search
Inclusive any decay originating from SUSY
particles that gives leptons in the final
state
  • Motivation
  • larger cross section compared to exclusive
    trileptons (?20?1? 3l ) and can be use as first
    day physics analysis
  • clean signature (Nleptons X) since
    uncertainties on leptons are smaller compared to
    JetMET
  • (Maybe!) the selection can depend less on JetMET
    based cuts
  • simultanious analysis of different Nleptons
    final states allows to constrain the model to a
    region in m0-m1/2 space
  • becomes important in regions where JetEt MET
    is low( FocusPoint region)

Backgrounds ZJets,WJets, ttbar,WW,ZW,ZZ,...
Effective mass (SJetEtMET)
6
Multilepton signatures
Example of multilepton signatures from gluino
cascade decays
LM1
LM9
Cross section fb for multimuon final states on
generator level
7
Multimuon event properties Nmgt2 _at_LM9
CMSSW_1_6_12 CSA07DATASETS
Effective Mass
muon pt
effective mass
Muon_pt
DiMuon Minv
dimuon invariant mass
number of jets
NJets
Dimuon invariant mass GeV
8
Demo results _at_ LM9 1fb-1
NOT SOPHISTICATED!
NMuons 3
selection cuts NJets gt2,Meff gt400 Jets itCone5,
Jet1_ptgt100GeV, Jet2_ptgt60GeV, Jet3_pt3gt50
,Jet_etalt2.4 Muons TrackerMuon,TMLSTightID,
m(1,2,3)_ptgt10GeV,m_pt gt5GeV, etalt2.4
Dimuon invariant mass GeV
NMuons gt 4
NMuons 4
Dimuon invariant mass GeV
Dimuon invariant mass GeV
9
Variable selection
Challenge How to find the best discriminating
variables out of 1k different distributions ?
10
Variable selection
What are the properties of a perfect set of
variables ?
Rating example
  • most discriminating power
  • use rating algorithms
  • least correlated
  • use correlation Matrix
  • least prone to uncertainties
  • use smearing, toy experiments...
  • least model dependent
  • use FastSim scan in m0-m1/2

--------------------------------------- Rank
Variable  Separation --------------------------
-------------      1 var3     
3.834e02     2 var2       3.062e02
     3 var1       1.097e02    
4 var0       5.818e01 --------------------
-------------------
Correlations example
MVA (Multi Variate Analysis Toolkit) gives access
to a bunch of statistical algorithms, variable
rating and correlation matrix and was implemented
in /PhysicsTools by Christophe Saout (KIT)
Talk on MVA Tuesday 940h C.Saout
11
Conclusion
  • 5s can be observed with 30fb-1 in Trileptons
    from direct Neutralino/Chargino pair production,
    but is not a first day physics channel
  • Inclusive multilepton search benefits from larger
    cross section compared to exclusive search and
    has a cleaner signature (leptons) compared to Jet
    MET based analysis, since leptons are less
    prone to uncertainties
  • Simultanious analysis of different multilepton
    final states at once can constrain the model to a
    region in m0-m1/2-space
  • First analysis for inclusive multimuon search
    gives already 5s for 1fb-1 with not
    sophisticated selection
  • Next steps use MVA toolkit to improve selection,
    take uncertainties into account and try to make
    selection more model independend
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