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Top CSC Notes Figures

The ATLAS CSC book was published online at the end of 2008 as CERN-OPEN-2008-20 or hep-ex arXiv:0901.0512. The figures from the Top Chapter CSC notes can be found below.

Top Chapter Introduction (T0)

  • Figure 1 - Top-pair production at lowest order
  • Figure 2 - Three production mechanisms for single top

Top Trigger (T5)

Top Light Jets (T2)

  • Figure 1 Distributions of (Equark - Ejet )/Equark for the jets from the W-boson decay
  • Figure 2 Energy resolution for jets from light quarks
  • Figure 3 Comparison of the jet energy resolutions with respect to the Monte Carlo hadrons
  • Figure 4 Comparison of the jet energy resolutions for events simulated with and without pile-up
  • Figure 5 Relative difference between the Monte Carlo jet energy and the reconstructed jet energy
  • Figure 6 Relative difference between the quark energy and the Monte Carlo jet energy
  • Figure 7 Relative difference between the quark and the jet energy with and without pileup
  • Figure 8 Distance between the jet and the quark
  • Figure 9 Resolution on the distance between the jet and the quark
  • Figure 10 Invariant di-jet mass as an estimate of the hadronically decaying W-boson mass
  • Figure 11 Invariant mass mjj of the selected jet-jet pairs
  • Figure 12 The apparent jet energy scale due to a cut on the transverse momenta
  • Figure 13 Shift of the reconstructed W boson mass
  • Figure 14 Shift of the reconstructed top mass
  • Figure 15 Ejet/Equark for jets originating from a W-boson
  • Figure 16 (1-cos(theta jjMC ))/(1-cos(theta jj)) as function of the reconstructed cos(theta jj)
  • Figure 17 Result of the iterative rescaling method as a function of E jet , with 10 fb-1
  • Figure 18 Result of the iterative rescaling method as a function of eta jet , with 10 fb-1
  • Figure 19 Result of the iterative rescaling method as a function of E jet , with 1 fb-1
  • Figure 20 Result of the iterative rescaling method as a function of eta jet , with 1 fb-1
  • Figure 21 Jet-jet invariant mass in fully simulated events superimposed on the best template histogram
  • Figure 22 Fitted jet energy scale as a function of the top mass
  • Figure 23 Fitted jet energy scale for sixteen 48 pb-1 pseudo-experiments
  • Figure 24 Reconstructed W-boson mass distribution in datasets with different gluon radiation settings
  • Figure 25 pT distribution of the jets from the hadronic W-boson decay for datasets with different gluon radiation settings
  • Figure 26 Total number of reconstructed jets with pT > 10 GeV for datasets with different gluon radiation settings
  • Figure 27 pT of the additional jets for datasets with different gluon radiation settings

Top Cross Section (T6)

Single lepton Commissioning analysis:

  • Figure1_left: Three-jet invariant mass distribution for the electron analysis
  • Figure1_right: Same distribution after the additional W-boson mass constraint
  • Figure2_left: The di-jet combination with highest \PT for the electron analysis
  • Figure2_right: The three di-jet combinations invariant masses among the top-quark candidates for the muon analysis
  • Figure3_left: Expected distribution of the three-jet invariant mass after the standard selection for the muon analysis
  • Figure3_right: The same after the W-boson mass constraint
  • Figure4_left: Reconstructed top mass after W-boson mass constraint for the electron analysis.
  • Figure4_right: The same distribution, but in addition requiring that the three highest PT jets are at eta < 1
  • Figure5_left: Fit to the top signal.
  • Figure5_right: Distribution of the expected statistical significance of the top signal in the peak as a function of the integrated luminosity for two background scenarios
  • Figure6_left: Expected distribution of the three-jet invariant masses among the top-quark candidates after the requirement on the mass of the di-jet system in the electron channel
  • Figure6_right: Same distribution for the muon channel
  • Figure7: Number of jets tagged as coming from a b-quark in ttbar, single top and W-boson+jet events after the default electron selection
  • Figure8_left: Reconstructed three-jet mass for ttbar , single top and $W$-boson + jet events for theelectron selection, requiring one or two jets tagged as coming from a b-quark.
  • Figure8_right: Same distribution for the default selection + the W-boson mass constraint
  • Figure8_left_color: Same as Figure_8_left
  • Figure8_right_color: Same as Figure_8_right

Differential Distributions

  • Figure9_left: Momentum distribution of the reconstructed three-jet mass
  • Figure9_right: Rapidity distribution of the hadronically decaying top quark
  • Figure10_left: Normalised di-top mass distribution for the more complex (dashed line) and the simple reconstruction (dotted line)
  • Figure10_right: Expected reconstructed di-top mass distribution after all cuts
  • Figure11_left: Distribution of PT and Y of hadronically decaying top quarks from truth information
  • Figure11_right: Reconstructed distribution of PT and Y of hadronically decaying top quarks from fully simulated samples

Dilepton analyses:

  • Figure12_left: Sigma(Delta R < 0.2) E_T variable for reconstructed electrons of the semi-leptonic ttbar background: in black are electrons matched to truth electrons, in white otherwise.
  • Figure12_right: Delta(R) from a muon to the closest jet in the semi-leptonic ttbar sample. In white are muons matched to truth muons, in black are muons that are close to a b-quark
  • Figure12_left_color: Same as Figure_12_left
  • Figure12_right_color: Same as Figure_12_right
  • Figure13_left: Di-lepton mass in signal, semi-leptonic ttbar and Z events
  • Figure13_right: Distribution of missing ET for signal and various backgrounds
  • Figure13_left_color: Same as Figure_13_left
  • Figure13_right_color: Same as Figure_13_right
  • Figure14_left: Monte Carlo e-mu template spanning the plane missing ET and number of jets for ttbar
  • Figure14_center: Monte Carlo e-mu template spanning the plane missing ET and number of jets for ww
  • Figure14_right: Monte Carlo e-mu template spanning the plane missing ET and number of jets for Z in tautau
  • Figure15_left: Total composition of the inclusive di-lepton selection versus number of jets
  • Figure15_right: Projected significance from pseudo-experiments for the inclusive template fit versus integrated luminosity including all channels and all systematic uncertainties
  • Figure16: Distribution of Delta(phi) between the highest PT lepton and the missing momentum vector for (a) signal, (b) background and (c) signal/background composition according to the ratio obtained from the cut analysis

Single Top (T8)

t-channel cross-section measurement:

Event selection :

  • Figure 1-left Probability density function for signal and background of the btagged jet pT after the t-channel selection;
  • Figure 1-right Signal and background distri butions of jet multiplicity with pT above 30 geV/c after the t-channel selection for an integrated luminosity of 1 fb-1;

Systematic uncertainty :

  • Figure 2-left Variation of the t-channel jet multiplicity for loose jets (pT>15 GeV) due to ISR/FSR parameter variation;
  • Figure 2-right Variation of the t-channel jet multiplicity for tight jets (pT> 30 GeV) due to ISR/FSR parameter variation;

Event yields for an integrated luminosity of 1 fb-1:

  • Figure 3-left Boosted Decision Tree output for signal and background after the btagged jet pT cut
  • Figure 3-right Leptonic top quark mass distribution after a cut on the BDT output at 0.6

s-channel cross-section measurement:

Distributions of the likelihood functions defined against five different background types for an integrated luminosity of 1 fb-1:

  • Figure 4a Likelihood function against top pair in the lepton+jet channel
  • Figure 4b Likelihood function against top pair in the dilepton channel
  • Figure 4c Likelihood function against top pair in the tau channel
  • Figure 4d Likelihood function against W+jets background
  • Figure 4e Likelihood function against t-channel background

W+t channel cross-section measurement:

Distributions of BDT output defined in the 3-jet final state channel for an integrated luminosity of 1 fb-1:

  • Figure 5a BDT against top pair in the lepton+jet channel
  • Figure 5b BDT against the W+jet background
  • Figure 5c BDT against top pair in the dilepton channel
  • Figure 5d BDT against the t-channel background

Top Mass (T9)

  • Figure 1: b-tagging efficiency as a function of light jet rejection in ttbar events
  • Figure 2, left: Light jet multiplicity in lepton+jets events before (solid line) and after (dashed line) requiring that the jet pT be greater than 40 GeV
  • Figure 2 right: b jet multiplicity in lepton+jets events before (solid line) and after (dashed line) requiring that the jet pT be greater than 40 GeV
  • Figure 3: Invariant mass of light jet pairs for events with only two light jets
  • Figure 4: Hadronic W boson mass after chi2 minimization
  • Figure 5: Energy correction factors estimated by the chi2 minimization
  • Figure 6: Hadronic W boson mass (geometric method)
  • Figure 7: Ratio of Etmiss to the generated neutrino transverse momentum
  • Figure 8, left: Transverse W boson mass, before modification
  • Figure 8, right: Transverse W boson mass, after modification
  • Figure 9: Invariant mass of the hadronic W boson and the leptonic b-jet for events satisfying C1 cut
  • Figure 10: Invariant mass of the lepton and the leptonic b-jet for events satisfying C1 and C2 cuts
  • Figure 11: Distribution of X1 = E*(W) - E*(b had) for events passing C2 and C3 cuts
  • Figure 12: Distribution of X2 = 2E*(b had) for events passing C2, C3 and C4 cuts
  • Figure 13, left: Hadronic top quark mass reconstructed with the chi2 minimization method, after C0 cut
  • Figure 13, right: Hadronic top quark mass reconstructed with the chi2 minimization method, after C2 and C3 cuts
  • Figure 14, left: Hadronic top quark mass reconstructed with the geometric method, after C1, C2 and C3 cuts
  • Figure 14, right: Hadronic top quark mass reconstructed with the geometric method, after C2, C3, C4 and C5 cuts
  • Figure 15, left: Hadronic top quark mass reconstructed with the geometric method, with rescaling, after C1, C2 and C3 cuts
  • Figure 15, right: Hadronic top quark mass reconstructed with the geometric method, with rescaling, after C2, C3, C4 and C5 cuts
  • Figure 16: chi2 distribution (with combinatorial background) with cuts C2 and C3 applied
  • Figure 17: Top quark mass as a function of chi2.
  • Figure 18, left: Pull distribution for the top quark mass measurement, with chi2 minimization method
  • Figure 18, right: Pull distribution for the top quark mass measurement, with geometric method
  • Figure 19, left: Light jet multiplicity for several values of ISR/FSR parameters
  • Figure 19, right: b-jet multiplicity for several values of ISR/FSR parameters
  • Figure 20: Reconstructed top mass as a function of the generated top mass, with chi2 minimization method
  • Figure 21: Difference between the reconstructed and generated top mass, as a function of the latter
  • Figure 22, left: Events with only 1 b-tagged jet, with rescaling and after purification cuts (C1, C3 and C6)
  • Figure 22, right: Events with only 1 b-tagged jet, with rescaling and after purification cuts (C3, C4, C5 and C6)
  • Figure 23, left: Events without b-tagging with the geometric method and after purification cuts (C1 and C3)
  • Figure 23, right: Events without b-tagging with the geometric method and after purification cuts (C3, C4 and C5)
  • Figure 24, left: Events without b-tagging: comparison between background and event mixing samples for two jets invariant mass
  • Figure 24, right: Events without b-tagging: comparison between background and event mixing samples for three jets invariant mass

Top Properties (T7)

  • Figure 1: Invariant mass of leptons and b-jets from the same top quark (full line) and from different top quarks (dashed line)
  • Figure 2: b-jet charge associated to positive (full line) and negative (dashed line) leptons at generator level (a) and after the ℓb mass cut (b)
  • Figure 3: The b-jet Qcomb distribution from S+B (full line) and B only (dashed line) (a); the top quark charge Qcomb (full line) and its background (dashed line) (b).
  • Figure 4a: Number of b-jets (containing a non-isolated lepton) associated with positive high pT leptons vs the charge of the non-isolated lepton
  • Figure 4b: Number of b-jets (containing a non-isolated lepton) associated with negative high pT leptons vs the charge of the non-isolated lepton
  • Figure 5: Correction function (a) and reconstructed angular distribution in the W centre-of-mass system (b)
  • Figure 6a: Reconstructed distribution for the spin correlation parameter A
  • Figure 6b: Reconstructed distribution for the spin correlation parameter Ad
  • Figure 7a: Discriminant variables (normalised to L = 1 fb−1) for the analysis without b-tagging
  • Figure 7b: Discriminant variables (normalised to L = 1 fb−1) for the analysis using b-tag weights
  • Figure 8a: Expected 68% CL allowed regions on the Wtb anomalous couplings gR vs gL
  • Figure 8b: Expected 68% CL allowed regions on the Wtb anomalous couplings gR vs VR
  • Figure 9a: Normalised discriminant variables for the t→qγ channel (isolated lepton=electron)
  • Figure 9b: Normalised discriminant variables for the t→qγ channel (isolated lepton=muon)
  • Figure 9c: Normalised discriminant variables for the t→qγ channel (isolated lepton=electron+muon)
  • Figure 9d: Normalised discriminant variables for the t→qZ channel (isolated lepton=electron)
  • Figure 9e: Normalised discriminant variables for the t→qZ channel (isolated lepton=muon)
  • Figure 9f: Normalised discriminant variables for the t→qZ channel (isolated lepton=electron+muon)
  • Figure 9g: Normalised discriminant variables for the t→qgluon channel (isolated lepton=electron)
  • Figure 9h: Normalised discriminant variables for the t→qgluon channel (isolated lepton=muon)
  • Figure 9i: Normalised discriminant variables for the t→qgluon channel (isolated lepton=electron+muon)
  • Figure 10: Observed and expected 95%CL limits on BR(t→qγ) vs BR(t→qZ)
  • Figure 11: Standard Model ttbar mass spectrum
  • Figure 12: A 700 GeV Z′ reconstructed mass distribution
  • Figure 13: Reconstruction efficiency of Standard Model ttbar pairs as a function of the ttbar mass
  • Figure 14: Reconstruction efficiency of Z′→ttbar resonances as a function of the Z′ mass
  • Figure 15: Z′ mass resolution
  • Figure 16: 5σ discovery potential of a generic ttbar resonance as a function of luminosity
  • Figure 17: Expected ttbar invariant mass spectrum

Guidelines for editors

For chapter editors: Please upload your figures to this wiki page with the following conventions:

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  • Name the files T<m>_figure.eps and add a comment 'Top XYZ Figure n'
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Major updates:
-- MartineBosman - 20 Nov 2008

Responsible: MartineBosman
Last reviewed by: Never reviewed

Topic attachments
I Attachment History Action Size Date Who Comment
Postscriptps PHENO_sgtop_3graphs.ps r1 manage 274.8 K 2008-11-20 - 18:41 MartineBosman Top Introduction Figure 2
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Unknown file formateps T0_figure2.eps r1 manage 274.8 K 2008-11-21 - 15:53 RichardHawkings Top Introduction FIgure 2
Unknown file formateps T2_fig1.eps r1 manage 18.5 K 2008-11-24 - 15:00 JeromeSchwindling Light jets figure 1
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Unknown file formateps T2_fig11.eps r1 manage 11.1 K 2008-11-24 - 15:10 JeromeSchwindling Light jets figure 11
Unknown file formateps T2_fig12.eps r1 manage 10.1 K 2008-11-24 - 15:10 JeromeSchwindling Light jets figure 12
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Unknown file formateps T2_fig14.eps r1 manage 10.3 K 2008-11-24 - 15:11 JeromeSchwindling Light jets figure 14
Unknown file formateps T2_fig15.eps r1 manage 20.7 K 2008-11-24 - 15:11 JeromeSchwindling Light jets figure 15
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Unknown file formateps T2_fig17.eps r1 manage 13.9 K 2008-11-24 - 15:12 JeromeSchwindling Light jets figure 17
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Unknown file formateps T2_fig19.eps r1 manage 11.8 K 2008-11-24 - 15:13 JeromeSchwindling Light jets figure 19
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Unknown file formateps T2_fig24.eps r1 manage 24.6 K 2008-11-24 - 15:15 JeromeSchwindling Light jets figure 24
Unknown file formateps T2_fig25.eps r1 manage 14.5 K 2008-11-24 - 15:16 JeromeSchwindling Light jets figure 25
Unknown file formateps T2_fig26.eps r1 manage 10.8 K 2008-11-24 - 15:16 JeromeSchwindling Light jets figure 26
Unknown file formateps T2_fig27.eps r1 manage 14.2 K 2008-11-24 - 15:16 JeromeSchwindling Light jets figure 27
Unknown file formateps T2_fig3.eps r1 manage 13.7 K 2008-11-24 - 15:07 JeromeSchwindling Light jets figure 3
Unknown file formateps T2_fig4.eps r1 manage 15.0 K 2008-11-24 - 15:07 JeromeSchwindling Light jets figure 4
Unknown file formateps T2_fig5.eps r1 manage 14.0 K 2008-11-24 - 15:07 JeromeSchwindling Light jets figure 5
Unknown file formateps T2_fig6.eps r1 manage 13.8 K 2008-11-24 - 15:08 JeromeSchwindling Light jets figure 6
Unknown file formateps T2_fig7.eps r1 manage 11.5 K 2008-11-24 - 15:08 JeromeSchwindling Light jets figure 7
Unknown file formateps T2_fig8.eps r1 manage 16.1 K 2008-11-24 - 15:09 JeromeSchwindling Light jets figure 8
Unknown file formateps T2_fig9.eps r1 manage 13.6 K 2008-11-24 - 15:09 JeromeSchwindling Light jets figure 9
Unknown file formateps T5_figure1a.eps r1 manage 324.7 K 2008-11-21 - 16:07 RichardHawkings Top Trigger Figure 1a
Unknown file formateps T5_figure1b.eps r1 manage 396.6 K 2008-11-21 - 16:07 RichardHawkings Top Trigger Figure 1b
Unknown file formateps T5_figure2a.eps r1 manage 325.0 K 2008-11-21 - 16:11 RichardHawkings Top Trigger Figure 2a
Unknown file formateps T5_figure2b.eps r1 manage 385.3 K 2008-11-21 - 16:11 RichardHawkings Top Trigger Figure 2b
Unknown file formateps T5_figure3a.eps r1 manage 10.1 K 2008-11-21 - 16:14 RichardHawkings Top Trigger Figure 3a
Unknown file formateps T5_figure3b.eps r1 manage 13.0 K 2008-11-21 - 16:14 RichardHawkings Top Trigger Figure 3b
Unknown file formateps T5_figure3c.eps r1 manage 14.3 K 2008-11-21 - 16:15 RichardHawkings Top Trigger Figure 3c
Unknown file formateps T5_figure4a.eps r1 manage 337.6 K 2008-11-21 - 16:20 RichardHawkings Top Trigger Figure 4a
Unknown file formateps T5_figure4b.eps r1 manage 413.4 K 2008-11-21 - 16:20 RichardHawkings Top Trigger Figure 4b
Unknown file formateps T5_figure4c.eps r1 manage 364.0 K 2008-11-21 - 16:20 RichardHawkings Top Trigger Figure 4c
Unknown file formateps T5_figure5.eps r1 manage 389.0 K 2008-11-21 - 16:21 RichardHawkings Top Trigger Figure 5
Unknown file formateps T5_figure6.eps r1 manage 367.8 K 2008-11-21 - 16:21 RichardHawkings Top Trigger Figure 6
Unknown file formateps T5_figure7.eps r1 manage 386.9 K 2008-11-21 - 16:30 RichardHawkings Top Trigger Figure 7
Unknown file formateps T5_figure8a.eps r1 manage 22.6 K 2008-11-21 - 16:30 RichardHawkings Top Trigger Figure 8a
Unknown file formateps T5_figure8b.eps r1 manage 24.5 K 2008-11-21 - 16:31 RichardHawkings Top Trigger Figure 8b
Unknown file formateps T5_figure8c.eps r1 manage 18.2 K 2008-11-21 - 16:31 RichardHawkings Top Trigger Figure 8c
Unknown file formateps T5_figure8d.eps r1 manage 18.9 K 2008-11-21 - 16:31 RichardHawkings Top Trigger Figure 8d
Unknown file formateps T6_fig10_left.eps r1 manage 12.5 K 2009-01-28 - 10:00 MarinaCobal Normalised di-top mass distribution for the more complex (dashed line) and the simple reconstruction (dotted line)
Unknown file formateps T6_fig10_right.eps r1 manage 13.8 K 2009-01-28 - 10:01 MarinaCobal Expected reconstructed di-top mass distribution after all cuts
Unknown file formateps T6_fig11_left.eps r1 manage 57.2 K 2009-01-28 - 11:43 MarinaCobal Distribution of PT and Y of hadronically decaying top quarks from truth information
Unknown file formateps T6_fig11_right.eps r1 manage 49.3 K 2009-01-28 - 11:44 MarinaCobal Reconstructed distribution of PT and Y of hadronically decaying top quarks from fully simulated samples
Unknown file formateps T6_fig12_left.eps r1 manage 21.6 K 2009-01-28 - 10:14 MarinaCobal Sigma(Delta R < 0.2) E_T variable for reconstructed electrons of the semi-leptonic ttbar background: in black are electrons matched to truth electrons, in white otherwise
Unknown file formateps T6_fig12_left_color.eps r1 manage 23.0 K 2009-01-28 - 10:17 MarinaCobal Same as Figure_12_lef
Unknown file formateps T6_fig12_right.eps r1 manage 22.0 K 2009-01-28 - 10:15 MarinaCobal Delta(R) from a muon to the closest jet in the semi-leptonic ttbar sample. In white are muons matched to truth muons, in black are muons that are close to a b-quark
Unknown file formateps T6_fig12_right_color.eps r1 manage 23.3 K 2009-01-28 - 10:17 MarinaCobal Same as Figure_12_right
Unknown file formateps T6_fig13_left.eps r1 manage 25.0 K 2009-01-28 - 11:18 MarinaCobal Di-lepton mass in signal, semi-leptonic ttbar and Z events
Unknown file formateps T6_fig13_left_color.eps r1 manage 25.0 K 2009-01-28 - 11:21 MarinaCobal Same as Figure_13_left
Unknown file formateps T6_fig13_right.eps r1 manage 31.3 K 2009-01-28 - 11:19 MarinaCobal Distribution of missing ET for signal and various backgrounds
Unknown file formateps T6_fig13_right_color.eps r1 manage 31.4 K 2009-01-28 - 11:21 MarinaCobal Same as Figure_13_right
Unknown file formateps T6_fig14_center.eps r1 manage 10.3 K 2009-01-28 - 11:25 MarinaCobal Monte Carlo e-mu
Unknown file formateps T6_fig14_left.eps r1 manage 11.3 K 2009-01-28 - 11:22 MarinaCobal Monte Carlo e-mu template
Unknown file formateps T6_fig14_right.eps r1 manage 11.0 K 2009-01-28 - 11:25 MarinaCobal Monte Carlo e-mu
Unknown file formateps T6_fig15_left.eps r1 manage 22.6 K 2009-01-28 - 11:41 MarinaCobal Total composition of the inclusive di-lepton selection versus number of jets
Unknown file formateps T6_fig15_right.eps r1 manage 10.2 K 2009-01-28 - 11:42 MarinaCobal Projected significance from pseudo-experiments for the inclusive template fit versus integrated luminosity including all channels and all systematic uncertainties
Unknown file formateps T6_fig16.eps r1 manage 45.9 K 2009-01-28 - 11:42 MarinaCobal Distribution of Delta(phi) between the highest PT lepton and the missing momentum vector for (a) signal, (b) background and (c) signal/background composition according to the ratio obtained from the cut analysis
Unknown file formateps T6_fig1_left.eps r1 manage 15.7 K 2009-01-27 - 11:36 MarinaCobal Three-jet invariant mass distribution for the electron analysis
Unknown file formateps T6_fig2_left.eps r1 manage 12.8 K 2009-01-27 - 12:12 MarinaCobal The di-jet combination with highest PT for the electron analysis
Unknown file formateps T6_fig2_right.eps r1 manage 22.9 K 2009-01-27 - 12:13 MarinaCobal The three di-jet combinations invariant masses among the top-quark candidates for the muon analysis
Unknown file formateps T6_fig3_right.eps r1 manage 17.7 K 2009-01-27 - 12:20 MarinaCobal The same after the W-boson constraint
Unknown file formateps T6_fig4_left.eps r1 manage 24.9 K 2009-01-27 - 12:25 MarinaCobal Reconstructed top mass after W-boson mass constraint for the electron analysis.
Unknown file formateps T6_fig4_right.eps r1 manage 24.3 K 2009-01-27 - 12:26 MarinaCobal The same distribution, but in addition requiring that the three highest PT jets are at eta < 1
Unknown file formateps T6_fig5_left.eps r1 manage 18.1 K 2009-01-27 - 12:30 MarinaCobal Fit to the top signal.
Unknown file formateps T6_fig5_right.eps r1 manage 18.2 K 2009-01-27 - 12:31 MarinaCobal Distribution of the expected statistical significance of the top signal in the peak as a function of the integrated luminosity for two background scenarios
Unknown file formateps T6_fig6.eps r1 manage 14.3 K 2009-01-27 - 12:35 MarinaCobal Number of jets tagged as coming from a b-quark
Unknown file formateps T6_fig6_left.eps r1 manage 21.8 K 2009-01-27 - 12:50 MarinaCobal Expected distribution of the three-jet invariant masses among the top-quark candidates after the requirement on the mass of the di-jet system in the electron channel
Unknown file formateps T6_fig6_right.eps r1 manage 19.4 K 2009-01-27 - 12:50 MarinaCobal Same distribution for the muon channel
Unknown file formateps T6_fig7.eps r1 manage 14.3 K 2009-01-27 - 12:52 MarinaCobal Number of jets tagged as coming from a b-quark in ttbar, single top and W-boson+jet events after the default electron selection
Unknown file formateps T6_fig8_left.eps r1 manage 24.3 K 2009-01-27 - 12:58 MarinaCobal Reconstructed three-jet mass for ttbar , single top and $W$-boson + jet events for theelectron selection, requiring one or two jets tagged as coming from a b-quark.
Unknown file formateps T6_fig8_left__colour.eps r1 manage 24.0 K 2009-01-27 - 13:01 MarinaCobal Same as Figure_8_lef
Unknown file formateps T6_fig8_right.eps r1 manage 23.0 K 2009-01-27 - 13:00 MarinaCobal Same distribution for the default selection + the W-boson mass constraint
Unknown file formateps T6_fig8_right_colour.eps r1 manage 22.7 K 2009-01-27 - 13:02 MarinaCobal Same as Figure_8_right
Unknown file formateps T6_fig9_left.eps r1 manage 22.7 K 2009-01-27 - 13:08 MarinaCobal Momentum distribution of the reconstructed three-jet mass
Unknown file formateps T6_fig9_right.eps r1 manage 18.5 K 2009-01-27 - 13:08 MarinaCobal Rapidity distribution of the hadronically decaying top quark
Unknown file formateps T7_fig1.eps r1 manage 13.7 K 2008-11-24 - 20:27 AntonioOnofre Top Properties Figure 1
Unknown file formateps T7_fig10.eps r1 manage 44.7 K 2008-11-24 - 20:55 AntonioOnofre Top Properties Figure 10
Unknown file formateps T7_fig11.eps r1 manage 12.9 K 2008-11-24 - 20:56 AntonioOnofre Top Properties Figure 11
Unknown file formateps T7_fig12.eps r1 manage 12.6 K 2008-11-24 - 20:56 AntonioOnofre Top Properties Figure 12
Unknown file formateps T7_fig13.eps r1 manage 10.0 K 2008-11-24 - 20:57 AntonioOnofre Top Properties Figure 13
Unknown file formateps T7_fig14.eps r1 manage 11.1 K 2008-11-24 - 20:57 AntonioOnofre Top Properties Figure 14
Unknown file formateps T7_fig15.eps r1 manage 11.7 K 2008-11-24 - 21:01 AntonioOnofre Top Properties Figure 15
Unknown file formateps T7_fig16.eps r1 manage 14.0 K 2008-11-24 - 21:01 AntonioOnofre Top Properties Figure 16
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Unknown file formateps T9_fig1.eps r1 manage 10.8 K 2008-12-12 - 12:33 AnneisabelleEtienvre T9_fig1
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PDFpdf t9.pdf r1 manage 306.3 K 2008-09-25 - 16:58 AnneisabelleEtienvre CSC note
Unknown file formateps toppair.eps r1 manage 484.9 K 2008-11-20 - 18:36 MartineBosman Top Introduction Figure 1
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Topic revision: r16 - 2010-12-06 - PatrickJussel
 
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