w polarization study in ttbar semi-lep decay
DESCRIPTION
W polarization study in ttbar semi-lep decay. BoLi Shandong University. W polarization in top decay. Test the top decay (in fully reconstructed tt) with W polarization. ...by measuring angular distribution of charged lepton in W rest frame. n. Angle between: - PowerPoint PPT PresentationTRANSCRIPT
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W polarization study in ttbar semi-lep decay
BoLi
Shandong University
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W polarization in top decay Test the top decay (in fully reconstructed tt) with W polarization ...
Standard Model (Mtop=175 GeV ) Longitudinal W+ (F0) Left-handed W+ (FL)
Right-handed W+ (FR)
LO 0.703 0.297 0.000
...by measuring angular distribution of charged lepton in W rest frame
222
0 2
cos1
2
cos1
2
sin
2
3
cos
1RL FFF
d
dN
N
1/2W+b t
spin
Angle between: •lepton in W rest frame and W in top rest frame
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Data
MC@NLO tt samples:mc08.105200.T1_McAtNlo_Jimmy.merge.AOD.e357_s462_s520_r809_r838
AcerMC tt samples:mc08.105205.AcerMCttbar.recon.AOD.e429_s462_s520_r808mc08.105205.AcerMCttbar.merge.AOD.e429_s462_s520_r808_r838
MC08 background samples(s520_r808_r838): w+jets (Alpgen 106280-3,107682-5,107692-5,107702-5) z+jets (Alpgen 107652-5, 107662-5,107672-5) dibosons(Herwig 105985-7) single top(AcerMC 105500,105502)
New data sample (re-reconstructed MC08 with rel. 15.3.1.6) and rel.15.6.0 for analysis
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event selection68%(64%) =1 lepton isolated |eta|<2.5pT>20GeV for μ
pT>25GeV for e
90%(90%)etmiss>20GeV
57%(57%) ≥ 4 jets pt>30GeV |eta|<2.5
33%(33%)≥ 2 bjets btagged with jetprob<0.014@eff~60%
Final kinematic cut efficiency 11.5(11.1)%
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Event reconstructionwhad = 2 jets
(mass closest to 80.4GeV)
Possible wlep = l +ν (constraint of Mw=80.4GeV)
thad = whad + bjet
(mass closest to 175GeV)
tlep = bjet + wlep
(bjet dR closest to lepton)
(mass closest to 175GeV)
reconstruction efficiency 3.39%(3.14%)
Plus quality cut ( |Mwhad-80.4 |<20 and |Mt – 175|<35 )
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DataTotal integral luminosity 700 Pb-1
After selectionProcess Run# Req x-sec (pb) Req # events
tt (non-hadronic) AcerMC 105205 218.37 152856
Signal 2686
Tau background 228
Single top Wt 105500 14.27 9986 24
Single top t-chan 105502 40.59 28414 31
Unfiltered W(e/m/t+nu)+(2/3/4/5)parton 3501.69 2451185 9
Z(ee,mm,tt)+(0/1/2/3/4/5) parton 4324.51 3027157 0
Wbb+(0/1/2/3) parton 17.86 12502.56 7
WW 105985 26.40 18478.4 0
ZZ 105986 1.93 1347.86 0
WZ 105987 8.82 6172.82 0
Total 5708100 s/b =9.0
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Selection cuts and reconstruction distort the parton lever distribution Use an independent sample to correct this distortion.
Measurement method
parton level
Reconstruction and cuts
Correction function :
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Measurement method
The tau events not correctly reconstructed as the neutrino from tau decay contaminate the neutrino from w decay
Taking e/mu/tau as signal instead of e/mu
at parton level distribution
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W polarization e/mu/tau as signal
e/mu as signal
F0 0.681 0.690
FL 0.315 0.308
FR 0.004 0.003
Truth values get from parton level distribution
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Result Function fit for w polarization
Measured value with statistical error:
FL= 0.281± 0.023
F0= 0.754± 0.042
FR=-0.034± 0.023
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Result
FL F0 FR
Theoretical error 0.02 0.02 0.01
Bjet energy scale (5%) 0.018 0.010 0.008
Btag efficiency (5%) 0.017 0.013 0.005
Systematic error
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ResultCorrection function use MC@NLO tt sample
F0 FL FR
Truth 0.697 0.301 0.002
Measured
0.614 0.332 0.054
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Summary Use new samples and software at r15 The selection efficiency increase from 11.1% to 11.5%
reconstruction efficiency increase from 3.14% to 3.39%
s/b from 8.6 to 9.0
Taking e/mu/tau as signal result matched well with theoretical value