RunII Analysis (Z-> b b, Z-> mu mu) - PowerPoint PPT Presentation

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RunII Analysis (Z-> b b, Z-> mu mu)

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applying NN techniques. 10/4/09. Silvia Tentindo Repond , FSU Meeting 8/12/02. 7. Dimuon DATA ... in the TOP mu jet streamed sample. ... – PowerPoint PPT presentation

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Title: RunII Analysis (Z-> b b, Z-> mu mu)


1
RunII Analysis (Z-gt b b, Z-gt mu mu)
  • Silvia Tentindo Repond, FSU
  • 12 August 2002
  • FSU Group

2
Overview
  • _at_ DATA - TOP data streams p11.09
  • di-muons
  • muonjet
  • production started on the farms, 1/10 of
    data reprocessed so far. Old p10. had no
    certified global muons nor good muon alignment.
  • _at_ MC - Z-bb new p10.15 - need p11.09
  • bb-inclusive p10.08
  • good for jet studies, not good for muons ,
    and jets with muons.
  • Jpsi-mu mu p10.15 ( need
    p11.09 for
  • higher efficiency.) right peak if global
    muons used

3
Physics channels
  • Signal(s) cross
    sections
  • Z ? b b (b?mu) 2 nb ( BR
    10)
  • Z ? mu mu
  • Jpsi ? mu mu
  • Ypsilon ? mu mu
  • Background
  • b b inclusive
    2 ub

4
flavor creation
b bbar production at Tev
  • Other contributions
  • Flavor excitation
  • Parton/shower fragmentation

Underlying event
b
P
P
Init state radiation
b
5
Signal(s) and Background diagrams
q
q
b
b
Z
g
b
q
q
b
mu
mu
mu
Jpsi
q
Ypsilon
Z
mu
mu
q
mu
6
Strategy
  • R Signal/Background ratio 10 -3
  • Improve R by
  • after b tagging ( sec. Vertex, muon ) !
  • - imposing kinematical cuts to data (JetE,
  • JetPt, JetDphi,E3, muonPt, etc.)
  • - applying energy corrections
  • - selecting appropriate window in Inv Mass
    spectrum
  • - applying NN techniques

7
Dimuon DATA
8
Dimuon DATA , selections and cuts
  • Top sample p11.09 ( July 2002 )
  • streamed di-muon events 11K so far
  • -- Analysis criteria
  • select quality muons (MuonId branch)
  • select isolated muons ( distance from
    jets gt0.5)
  • -- Invariant Mass cuts
  • 2 leading muons , p_t gt 2 Gev
  • 2 leading muons, Egt 8 Gev

9
Dimuon DATA muons (Global) All
10
Dimuon DATA muons (Global) Good
11
Dimuon DATA Inv Mass
12
Dimuon DATA Inv Mass
13
(Dimuon) Dijet DATA
14
Jets DATA , selections and cuts
  • Top sample p11.09 ( July 2002)
  • muonjet stream ( L1 1jet 1muon trigger)
  • -- Analysis criteria
  • use b tagging lepton only for now,
    extend to impact parameter and sec
    vertex next.
  • select quality jets
  • select quality muons (MuonId branch)
  • associate muons to jets ( distance lt0.7)
    ? b tagging
  • -- Invariant Mass cuts
  • 2 leading jets , p_t gt15 Gev
  • associated muon p_tgt 4 Gev
  • two associated muons ( no p_t cuts )

15
Cuts and selections ( cont)
  • Also under study
  • -- 2 leading jets back-to-back
  • -- H_t
  • -- unclustered energy
  • Energy
    corrections
  • V1.1 - January 2002
  • V2.1 - May 10 2002

16
Jets
  • Jets distributions
  • Jet Multiplicity per event eta phi Pt
    Energy MET
  • Track Multiplicity per Jet . JCCA branch, R0.7
  • Number of Good Jets gives the number of jets
    passing the standard quality cuts for jets
  • JCCA EMF gt 0.05 and lt 0.95
  • JCCA CHF gt 0.5
  • JCCA HotF lt 10
  • JCCA n90 gt 2
  • Only Good Jets are used for Inv Mass
    calculations.

17
Dimuon DATA - Jets
18
muons in Jets
  • Detected muons ( MuonId branch ) are requested
    to pass the medium quality cuts Muon Id vsn
    2.0 , Jul 2002
  • N Segments 3
  • Chisq_trk lt100
  • A Global muon is a local muon that has been
    matched to a central track.
  • Eta, phi, P and Pt distributions are given for
    the selected good muons.
  • Ptrel and R(j,mu) are also calculated.
  • A muon is associated to a jet if the distance
    from the jet axis is lt 0.7
  • In the eta,phi plane, and if it passes the
    quality cuts.
  • Multiplicities of muons per event, number of
    good muons and of muons associated to jets are
    given.

19
Dimuon DATA muons(Global) Associated to jets
20
Dimuon DATA jets and muons counts
21
Energy Corrections
  • Energy corrections ( Jet Energy Scale at D0 in
    RunII, D0Notes Jan 2002 and June 2002) have been
    applied to all the di jet Inv Mass
    distributions.
  • The jet energy is corrected for all types of
    jets.
  • In case the jet contains a muon, the energy
    correction includes the corrected muon energy and
    the neutrino energy ( muon jet en corr ).
  • Inv Mass distributions, calculated for the two
    leading jets in the event, are plotted for jets
    energies uncorrected and after correction, and
    then the plots are compared.

22
Dimuon DATA Energy Corrections V2.1
23
(Dimuon) Jets Invariant Mass Distributions
24
Dijets DATA InvMass no en corr
25
Dijet DATA Inv Mass with en corr
26
(Dimuon) Jets DATA Inv Mass
27
Conclusions
  • DATA have been (re-)analyzed from the most
    recent production vsn p11.09.00, in the TOP
    di-muon streamed sample ( p10. had bad global
    muons)
  • Invariant mass plots show clear evidences of
    peaks at the Jpsi, Ypsilon and eventually Z mass
  • No evidences of Zs on the (Dimuon) Jet Invariant
    mass
  • at this level of statistics
  • Same study to be done ( re-done!) in the TOP
    mujet streamed sample.
  • ? need more streamed data ( at present 10K in
    p11, were 500K in p10. 6.5 pb-1)

28
Appendix
  • ( Useful transparencies from my previous talks )

29
Complete B Tagging studies for Zbb
  • Started B tagging by using Impact parameter
  • and secondary vertex information.
  • Impact parameter tag
  • Select jets ( two leading jets do contribute to
    Minv plots) that are tagged by Impact parameter
    at least one of the two leading jets must be imp
    par tagged.
  • --- Study effects of imp par tagging on DATA, MC
    signal and MC background samples.
  • ---- Combine imp par tag and Pt cuts to MInv
    distributions

30
DATA bc taggings
31
DATA Impact Parameter tag
32
Zbb MC Impact Parameter tag
33
MC bb inclusive Impact Parameter tag
34
Inv Mass Pt cuts and Mass corrections
  • Pt cuts in Inv Mass ( on the two leading jets)
  • 1 improve Mass resolution
  • 2 - but- highly decrease the signal rate
  • 1 higher is the Pt cut value on the two leading
    jets and lower is the yield of events with final
    state radiation .
  • FSR events contribute to the left tail of
    the Inv Mass distribution.
  • 2 need to find a method of mass correction
    that recovers jets at lower Pt in the event so
    that they could contribute to raise the Minv
    value to the correct position so to raise the
    signal rate

35
MC Zbb Inv Mass , Pt cuts
36
MC bb inclusive Inv Mass, Pt cuts
37
Inv Mass Pt cuts and Mass corrections
  • QUESTION from where the right side tail comes
    in the DATA Invmass distribution?
  • 1 background ??
  • Study MC bb inclusive distribution ( need
    HIGH statistics, and PtGt20?? Selections )
  • 2 energy corrections ??
  • v2.1 en corr are over correcting DATA (
    en corr for MC are ok).
  • MC Zbb distributions have NO right tail in the
    Minv distribution.
  • Need to get rid of this tail too to improve Minv
    resolution.

38
Old Samples
  • Zbb Skimmed DATA
  • Prj_root/871/b_2/kazu/data/output145xxx_a.root
  • 1567 events
  • Zbb MC events
  • rAtpl_recocert_p11.08.00_lancs_pythia_hitv000326
    z-zbb-Plate_mb-none_170_02170135325.root
  • 250 events
  • bb inclusive MC events
  • rAtpl_mcp10_p10.00.01_lancs_pythia_topv000305bb
    bar-incl-ptGt10.0-Plate_mb-poisson-0.5_31100351820
    01.root
  • 500 events
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