Search for supersymmetry in pp collisions at a center-of-mass energy of 8 TeV in events with a single lepton, multiple jets and b-tags

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Link to the document

The analysis is documented in arXiv:1311.4937 and submitted to Phys. Lett. B .

Abstract

Results are reported from a search for supersymmetry in pp collisions at a center-of-mass energy of 8 TeV, based on events with a single isolated lepton (e or mu) and multiple jets, at least two of which are identified as b jets. The data sample corresponds to an integrated luminosity of 19.3 fb-1 recorded by the CMS experiment at the LHC in 2012. The search is motivated by supersymmetric models that involve strong-production processes and cascade decays of new particles. The resulting final states contain multiple jets as well as missing transverse momentum from weakly interacting particles. The event yields, observed across several kinematic regions, are consistent with the expectations from standard model processes predicted from control samples in the data. The results are interpreted in the context of simplified supersymmetric scenarios with pair production of gluinos, where each gluino decays to a top quark-antiquark pair and the lightest neutralino. For the case of decays via virtual top squarks, gluinos with a mass smaller than 1.26 TeV are excluded for low neutralino masses.

Introduction

This page summarizes results from a search for supersymmetry in proton-proton collisions at a center-of-mass energy of 8 TeV in events with a single lepton (electron or muon), missing transverse momentum (MET), and multiple jets, at least two of which are tagged as originating from bottom quarks (b-tagged jets). The search focuses on gluino pair production, with subsequent gluino decay to two top quarks and the lightest supersymmetric particle (LSP) through either a virtual or an on-shell top squark: pp → g̃ g̃ with g̃ ( → t̃ t̄) → t t̄ LSP. Three variations of this scenario, denoted models A, B, and C, are considered in this analysis. In model A (models B and C), gluinos are lighter (heavier) than top squarks and gluino decay proceeds through a virtual (real) top squark. For model A, the gluino and LSP masses are allowed to vary. For model B, M(g̃) is set to 1 TeV and M(LSP) and M(t̃) are varied. For model C, M(LSP) is set to 50 GeV and M(g̃) and M(t̃) are varied.

Two approaches are used in this search. The first approach is based on the distribution of MET in exclusive intervals of the scalar sum of jet transverse momentum values (HT). The MET distribution is evaluated either by using the charged-lepton spectrum (lepton spectrum method) or by extrapolating from lower HT (MET template method). The Delta Phi method uses the azimuthal angle between the lepton and W boson directions as a discriminating variable and searches in bins of Nb (2 and ≥ 3) and STlep, which probes the total leptonic (l and ν) momentum in the event. The two methods probe complementary kinematic aspects, the hadronic and leptonic event characteristics. Together they provide a broad view of possible deviations from the standard model.

Plots and tables from the paper

FIGURE (click image for PDF) Caption

Figure 1

Observed MET distribution and the corresponding prediction from the LS method for Nb=2 and HT>500 GeV. The hatched area shows the combined statistical and systematic uncertainty of the prediction. For comparison, the distributions of SUSY model A, described in the paper, with either m(gluino)=1250 GeV and m(LSP)=0 GeV or m(gluino)=1000 GeV and m(LSP)=600 GeV are shown. The value and uncertainty for the prediction in the highest MET bin corresponds to the average for the range 450-1000 GeV.

Observed MET distributions and the corresponding predictions from the LS and MT methods for Nb=2 and HT>750 GeV. The hatched areas show the combined statistical and systematic uncertainties of the predictions. For comparison, the distributions of SUSY model A, described in the paper, with either m(gluino)=1250 GeV and m(LSP)=0 GeV or m(gluino)=1000 GeV and m(LSP)=600 GeV are shown. Values and uncertainties for the prediction in the highest MET bin correspond to the average for the range 450-1000 GeV.

Observed MET distributions and the corresponding predictions from the LS and MT methods for Nb=2 and HT>1000 GeV. The hatched areas show the combined statistical and systematic uncertainties of the predictions. For comparison, the distributions of SUSY model A, described in the paper, with either m(gluino)=1250 GeV and m(LSP)=0 GeV or m(gluino)=1000 GeV and m(LSP)=600 GeV are shown. Values and uncertainties for the prediction in the highest MET bin correspond to the average for the range 450-1000 GeV.

Observed MET distribution and the corresponding prediction from the MT method for Nb≥3 and HT>400 GeV. The hatched area shows the combined statistical and systematic uncertainty of the prediction. For comparison, the distributions of SUSY model A, described in the paper, with either m(gluino)=1250 GeV and m(LSP)=0 GeV or m(gluino)=1000 GeV and m(LSP)=600 GeV are shown. The value and uncertainty for the prediction in the highest MET bin corresponds to the average for the range 450-1000 GeV.

Observed MET distributions and the corresponding predictions from the LS and MT methods for Nb≥3 and HT>750 GeV. The hatched areas show the combined statistical and systematic uncertainties of the predictions. For comparison, the distributions of SUSY model A, described in the paper, with either m(gluino)=1250 GeV and m(LSP)=0 GeV or m(gluino)=1000 GeV and m(LSP)=600 GeV are shown. Values and uncertainties for the prediction in the highest MET bin correspond to the average for the range 450-1000 GeV.

Observed MET distributions and the corresponding predictions from the LS and MT methods for Nb≥3 and HT>1000 GeV. The hatched areas show the combined statistical and systematic uncertainties of the predictions. For comparison, the distributions of SUSY model A, described in the paper, with either m(gluino)=1250 GeV and m(LSP)=0 GeV or m(gluino)=1000 GeV and m(LSP)=600 GeV are shown. Values and uncertainties for the prediction in the highest MET bin correspond to the average for the range 450-1000 GeV.

Figure 2

The ∆φ(W,l) in simulation and data for the combined electron and muon channels with Nb≥3, Nj≥ 6. The SM simulation is normalized to the data in the control region (∆φ(W,l)>1). The simulated SM yields in the signal region (∆φ(W,l)<1) are shown only for illustration, as the actual estimate is obtained with the procedure described in the paper. The distributions expected for signal are illustrated using two mass points from model A, with masses specified as (mgluino,mLSP) in GeV. for the 250<STlep<350 GeV bin.

The ∆φ(W,l) in simulation and data for the combined electron and muon channels with Nb≥3, Nj≥6. The SM simulation is normalized to the data in the control region (∆φ(W,l)>1). The simulated SM yields in the signal region (∆φ(W,l)<1) are shown only for illustration, as the actual estimate is obtained with the procedure described in the paper. The distributions expected for signal are illustrated using two mass points from model A, with masses specified as (mgluino,mLSP) in GeV. for the 350<STlep<450 GeV bin.

The ∆φ(W,l) in simulation and data for the combined electron and muon channels with Nb≥3, Nj≥6. The SM simulation is normalized to the data in the control region (∆φ(W,l)>1). The simulated SM yields in the signal region (∆φ(W,l)<1) are shown only for illustration, as the actual estimate is obtained with the procedure described in the paper. The distributions expected for signal are illustrated using two mass points from model A, with masses specified as: (mgluino,mLSP) in GeV. for the STlep>450 GeV bin.

Figure 3

The transfer factor RCS in simulation for the combined electron and muon channels as a function of Nb for events with Nj≥6 and STlep in range: [250,350] GeV. The points correspond to o SM only and to the sum of SM background and model A signal corresponding to the mass point: (mgluino,mLSP) in GeV.

The transfer factor RCS in simulation for the combined electron and muon channels as a function of Nb for events with Nj≥6 and STlep in range: [350,450] GeV. The points correspond to o SM only and to the sum of SM background and model A signal corresponding to the mass point: (mgluino,mLSP) in GeV.

The transfer factor RCS in simulation for the combined electron and muon channels as a function of Nb for events with Nj≥6 and STlep>450 GeV. The points correspond to o SM only and to the sum of SM background and model A signal corresponding to the mass point: (mgluino,mLSP) in GeV.

Figure 4

Observed (solid lines) and expected (dashed lines) 95% C.L. limits obtained with the LS (blue) and MT (green) methods in the m(LSP) vs. m(gluino) mass plane in model A. The thick lines represent the central value and the thin lines represent the variations from the theoretical and experimental uncertainties. The uncertainties for the MT method have similar size and are not shown. The limits are obtained using a NLO+NLL reference cross section for gluino pair production and 100% BR for gluino → ttbar+LSP.

Observed (solid lines) and expected (dashed lines) 95% C.L. limits obtained with the DP method in the m(LSP) vs. m(gluino) mass plane in model A. The color shading indicates the observed limit on the cross section. The thick lines represent the central value and the thin lines represent the variations from the theoretical and experimental uncertainties. The limits are obtained using a NLO+NLL reference cross section for gluino pair production and 100% BR for gluino → ttbar+LSP. A text file containing the cross section upper limit at each point can be found here.

Observed 95% C.L. limits obtained with the DP (black), LS (blue), and MT (green) methods in the m(LSP) vs. m(gluino) mass plane in model A. The thick lines represent the central value and the thin lines represent the variations from the theoretical uncertainties. The limits are obtained using a NLO+NLL reference cross section for gluino pair production and 100% BR for gluino → ttbar+LSP.

Observed (solid lines) and expected (dashed lines) 95% C.L. limits obtained with the LS (blue) and MT (green) methods in the m(LSP) vs. m(stop) mass plane in model B. The thick lines represent the central value and the thin lines represent the variations from the theoretical and experimental uncertainties. The uncertainties for the MT method have similar size and are not shown. The limits are obtained using a NLO+NLL reference cross section for gluino pair production and 100% BR for gluino → stop+top → ttbar+LSP with m(gluino)=1 TeV.

Observed (solid lines) and expected (dashed lines) 95% C.L. limits obtained with the DP method in the m(LSP) vs. m(stop) mass plane in model B. The color shading indicates the observed limit on the cross section. The thick lines represent the central value and the thin lines represent the variations from the theoretical and experimental uncertainties. The limits are obtained using a NLO+NLL reference cross section for gluino pair production and 100% BR for gluino → stop+top → ttbar+LSP with m(gluino)=1 TeV. A text file containing the cross section upper limit at each point can be found here.

Observed 95% C.L. limits obtained with the DP (black), LS (blue), and MT (green) methods in the m(LSP) vs. m(stop) mass plane in model B. The thick lines represent the central value and the thin lines represent the variations from the theoretical uncertainties. The limits are obtained using a NLO+NLL reference cross section for gluino pair production and 100% BR for gluino → stop+top → ttbar+LSP with m(gluino)=1 TeV.

Observed (solid lines) and expected (dashed lines) 95% C.L. limits obtained with the LS (blue) and MT (green) methods in the m(stop) vs. m(gluino) mass plane in model C. The thick lines represent the central value and the thin lines represent the variations from the theoretical and experimental uncertainties. The uncertainties for the MT method have similar size and are not shown. The limits are obtained using a NLO+NLL reference cross section for gluino pair production and 100% BR for gluino → stop+top → ttbar+LSP with m(LSP)=50 GeV.

Observed (solid lines) and expected (dashed lines) 95% C.L. limits obtained with the DP method in the m(stop) vs. m(gluino) mass plane in model C. The color shading indicates the observed limit on the cross section. The thick lines represent the central value and the thin lines represent the variations from the theoretical and experimental uncertainties. The limits are obtained using a NLO+NLL reference cross section for gluino pair production and 100% BR for gluino → stop+top → ttbar+LSP with m(LSP)=50 GeV. A text file containing the cross section upper limit at each point can be found here.

Observed 95% C.L. limits obtained with the DP (black), LS (blue), and MT (green) methods in the m(stop) vs. m(gluino) mass plane in model C. The thick lines represent the central value and the thin lines represent the variations from the theoretical uncertainties. The limits are obtained using a NLO+NLL reference cross section for gluino pair production and 100% BR for gluino → stop+top → ttbar+LSP with m(LSP)=50 GeV.

Tables

Table 1: Observed yields in data and SM background predictions with their statistical and systematic uncertainties from the LS and MT methods. For the MT method, the low MET (150-250 GeV) and low HT (400-750 GeV) regions in the Nb=2 sample are used as control regions and not shown in the table.

Table 2: Event yields for the combined electron and muon channels, as predicted by simulation, for Nb≥3, Nj≥6. The RCS column lists the ratio of yields in the signal and control regions. The yields for signal benchmark points are shown for comparison, with masses: (mgluino,mLSP) in GeV. The uncertainties are statistical only.

Table 3: Data yields and the corresponding RCS for events with Nj≥6 and Nb=1.

Table 4: Closure of the background estimation method in simulation, for combined muons and electrons, comparing the yields in the signal region of events with Nb≥3 and the estimate using RCS from the Nb=1 sample. The κ factor is the ratio of the “true” and “predicted”.

Table 5: Event yields in data for the for the 3≤Nj≤5 (validation) and Nj≤6 (signal) samples. The number of events in the control regions used for the predictions are also shown. For the lower jet multiplicity validation test, only the statistical uncertainties stemming from the event counts in the control regions are given, while statistical and systematic uncertainties are listed for the signal region prediction.

Plots from the Lepton Spectrum Method

Generator-level neutrino and charged lepton pT distributions from simulated events. All background components are included and scaled to the data luminosity. The similarity between the lepton and neutrino pT is the pasis of the Lepton Spectrum method that uses the observed lepton pT spectrum to predict the MET spectrum.

Scale factors used in the lepton spectrum prediction. These scale factors are measured in MC and applied to the lepton pT spectrum to correct for polarization and acceptance effects.

Relative systematic uncertainties, in percent, on the single tau, lepton+tau→lepton, and lepton+tau→hadrons beckground predictions for Njet≥6 and Nb=2. The relative uncertainty is shown for each of the HT selections and separated by slashes, i.e. HT> 500/750/1000 GeV.

kappa factors used in the single tau prediction in the Lepton Spectrum method for Njet≥6 and Nb=2. These factors are measured in MC and are used to correct any MET dependent biases in the data driven prediction.

kappa factors used in the lepton+tau→lepton prediction in the Lepton Spectrum method for Njet≥6 and Nb=2. These factors are measured in MC and are used to correct any MET dependent biases in the data driven prediction.

kappa factors used in the lepton+tau→hadrons prediction in the Lepton Spectrum method for Njet≥6 and Nb=2. These factors are measured in MC and are used to correct any MET dependent biases in the data driven prediction.

Relative systematic uncertainties, in percent, on the lost and ignored dilepton background predictions in the Lepton Spectrum method for Njet≥6 and Nb=2. The relative uncertainty is shown for each of the HT selections and separated by slashes, i.e. HT> 500/750/1000 GeV.

Predicted MET distribution for the single tau background in the Lepton Spectrum method for Njet≥6, Nb=2, and HT> 500 GeV. The blue points are the data-driven prediction and the histogram is the prediction from MC scaled to the normalization of the data-driven prediction. The MC shapes are shown for comparison only and are not used directly.

Predicted MET distribution for the single tau background in the Lepton Spectrum method for Njet≥6, Nb=2, and HT> 750 GeV. The blue points are the data-driven prediction and the histogram is the prediction from MC scaled to the normalization of the data-driven prediction. The MC shapes are shown for comparison only and are not used directly.

Predicted MET distribution for the single tau background in the Lepton Spectrum method for Njet≥6, Nb=2, and HT> 1000 GeV. The blue points are the data-driven prediction and the histogram is the prediction from MC scaled to the normalization of the data-driven prediction. The MC shapes are shown for comparison only and are not used directly.

Predicted MET distribution for the lepton+tau→hadrons background in the Lepton Spectrum method for Njet≥6, Nb=2, and HT> 500 GeV. The blue points are the data-driven prediction and the histogram is the prediction from MC scaled to the normalization of the data-driven prediction. The MC shapes are shown for comparison only and are not used directly.

Predicted MET distribution for the lepton+tau→hadrons background in the Lepton Spectrum method for Njet≥6, Nb=2, and HT> 750 GeV. The blue points are the data-driven prediction and the histogram is the prediction from MC scaled to the normalization of the data-driven prediction. The MC shapes are shown for comparison only and are not used directly.

Predicted MET distribution for the lepton+tau→hadrons background in the Lepton Spectrum method for Njet≥6, Nb=2, and HT> 1000 GeV. The blue points are the data-driven prediction and the histogram is the prediction from MC scaled to the normalization of the data-driven prediction. The MC shapes are shown for comparison only and are not used directly.

Predicted MET distribution for the lepton+tau→lepton background in the Lepton Spectrum method for Njet≥6, Nb=2, and HT> 500 GeV. The blue points are the data-driven prediction and the histogram is the prediction from MC scaled to the normalization of the data-driven prediction. The MC shapes are shown for comparison only and are not used directly.

Predicted MET distribution for the lepton+tau→lepton background in the Lepton Spectrum method for Njet≥6, Nb=2, and HT> 750 GeV. The blue points are the data-driven prediction and the histogram is the prediction from MC scaled to the normalization of the data-driven prediction. The MC shapes are shown for comparison only and are not used directly.

Predicted MET distribution for the lepton+tau→lepton background in the Lepton Spectrum method for Njet≥6, Nb=2, and HT> 1000 GeV. The blue points are the data-driven prediction and the histogram is the prediction from MC scaled to the normalization of the data-driven prediction. The MC shapes are shown for comparison only and are not used directly.

MET distribution from simulation and data for dilepton events for Njet≥6, Nb=2, and HT> 500 GeV. The data to MC ratio of event yields for MET> 100 GeV is used to scale the predicted MET distribution from simulation for ignored and lost leptons in the Lepton Spectrum method.

MET distribution from simulation and data for dilepton events for Njet≥6, Nb=2, and HT> 750 GeV. The data to MC ratio of event yields for MET> 100 GeV is used to scale the predicted MET distribution from simulation for ignored and lost leptons in the Lepton Spectrum method.

MET distribution from simulation and data for dilepton events for Njet≥6, Nb=2, and HT> 1000 GeV. The data to MC ratio of event yields for MET> 100 GeV is used to scale the predicted MET distribution from simulation for ignored and lost leptons in the Lepton Spectrum method.

Predicted MET distribution from simulation for ignored and lost leptons in the Lepton Spectrum method, scaled to the ratio of dilepton events in data over MC for Njet≥6, Nb=2, and HT> 500 GeV.

Predicted MET distribution from simulation for ignored and lost leptons in the Lepton Spectrum method, scaled to the ratio of dilepton events in data over MC for Njet≥6, Nb=2, and HT> 750 GeV.

Predicted MET distribution from simulation for ignored and lost leptons in the Lepton Spectrum method, scaled to the ratio of dilepton events in data over MC for Njet≥6, Nb=2, and HT> 1000 GeV.

Systematic uncertainties, in percent, for the single lepton background prediction in the Lepton Spectrum method for Njet≥6, Nb=2, and HT > (500/750/1000) GeV in the search MET bins and the low MET validation region. Each uncertainty is expressed as the change in the ratio of predicted to true number of events (evaluated using simulated events). The total uncertainty is the individual uncertainties summed in quadrature.

Observed and predicted yields in the Lepton Spectrum method for HT> 500 GeV. The yields are shown as total (muon channel, electron channel). A requirement of Njet≥ 6 and Nb=2 is imposed.

Observed and predicted yields in the Lepton Spectrum method for HT> 750 GeV. The yields are shown as total (muon channel, electron channel). A requirement of Njet≥ 6 and Nb=2 is imposed.

Observed and predicted yields in the Lepton Spectrum method for HT> 1000 GeV. The yields are shown as total (muon channel, electron channel). A requirement of Njet≥ 6 and Nb=2 is imposed.

Observed and predicted yields in the Lepton Spectrum method for HT> 500 GeV. The yields are shown as total (muon channel, electron channel). A requirement of Njet≥ 6 and Nb≥3 is imposed.

Observed and predicted yields in the Lepton Spectrum method for HT> 750 GeV. The yields are shown as total (muon channel, electron channel). A requirement of Njet≥ 6 and Nb≥3 is imposed.

Observed and predicted yields in the Lepton Spectrum method for HT> 1000 GeV. The yields are shown as total (muon channel, electron channel). A requirement of Njet≥ 6 and Nb≥3 is imposed.

Observed MET distributions in the Lepton Spectrum method in data compared with predicted distributions (red bars) in the combined electron and muon channels, for events with Njet≥6, Nb=2, and HT > 500 GeV. The red-bar histogram includes the total single lepton, dilepton, and single τ background prediction, where the red (black) error band shows the uncertainty from the MET scale and MC statistics (total uncertainty) on the single lepton scale factor. The blue histogram shows the contribution from just the dilepton and single τ backgrounds. The distributions for the T1tttt SMS with (mgluino, mLSP)=(1100 GeV, 1000 GeV) is overlaid for comparison. The lower plot shows (Data-Pred)/Error.

Observed MET distributions in the Lepton Spectrum method in data compared with predicted distributions (red bars) in the combined electron and muon channels, for events with Njet≥6, Nb=2, and HT > 750 GeV. The red-bar histogram includes the total single lepton, dilepton, and single τ background prediction, where the red (black) error band shows the uncertainty from the MET scale and MC statistics (total uncertainty) on the single lepton scale factor. The blue histogram shows the contribution from just the dilepton and single τ backgrounds. The distributions for the T1tttt SMS (model A) with (mgluino, mLSP)=(1100 GeV, 1000 GeV) is overlaid for comparison. The lower plot shows (Data-Pred)/Error.

Observed MET distributions in the Lepton Spectrum method in data compared with predicted distributions (red bars) in the combined electron and muon channels, for events with Njet≥6, Nb=2, and HT > 1000 GeV. The red-bar histogram includes the total single lepton, dilepton, and single τ background prediction, where the red (black) error band shows the uncertainty from the MET scale and MC statistics (total uncertainty) on the single lepton scale factor. The blue histogram shows the contribution from just the dilepton and single τ backgrounds. The distributions for the T1tttt SMS (model A) with (mgluino, mLSP)=(1100 GeV, 1000 GeV) is overlaid for comparison. The lower plot shows (Data-Pred)/Error.

Observed MET distributions in the Lepton Spectrum method in data compared with predicted distributions (red bars) in the combined electron and muon channels, for events with 3≤Njet≤5, Nb=2, and HT > 500 GeV. The red-bar histogram includes the total single lepton, dilepton, and single τ background prediction, where the red (black) error band shows the uncertainty from the MET scale and MC statistics (total uncertainty) on the single lepton scale factor. The blue histogram shows the contribution from just the dilepton and single τ backgrounds. The distributions for the T1tttt SMS (model A) with (mgluino, mLSP)=(1100 GeV, 1000 GeV) is overlaid for comparison. The lower plot shows (Data-Pred)/Error.

Observed MET distributions in the Lepton Spectrum method in data compared with predicted distributions (red bars) in the combined electron and muon channels, for events with 3≤Njet≤5, Nb=2, and HT > 750 GeV. The red-bar histogram includes the total single lepton, dilepton, and single τ background prediction, where the red (black) error band shows the uncertainty from the MET scale and MC statistics (total uncertainty) on the single lepton scale factor. The blue histogram shows the contribution from just the dilepton and single τ backgrounds. The distributions for the T1tttt SMS (model A) with (mgluino, mLSP)=(1100 GeV, 1000 GeV) is overlaid for comparison. The lower plot shows (Data-Pred)/Error.

Observed MET distributions in the Lepton Spectrum method in data compared with predicted distributions (red bars) in the combined electron and muon channels, for events with 3≤Njet≤5, Nb=2, and HT > 1000 GeV. The red-bar histogram includes the total single lepton, dilepton, and single τ background prediction, where the red (black) error band shows the uncertainty from the MET scale and MC statistics (total uncertainty) on the single lepton scale factor. The blue histogram shows the contribution from just the dilepton and single τ backgrounds. The distributions for the T1tttt SMS (model A) with (mgluino, mLSP)=(1100 GeV, 1000 GeV) is overlaid for comparison. The lower plot shows (Data-Pred)/Error.

Observed MET distributions in the Lepton Spectrum method in data compared with predicted distributions (red bars) in the combined electron and muon channels, for events with Njet≥6, Nb≥3, and HT > 500 GeV. The red-bar histogram includes the total single lepton, dilepton, and single τ background prediction, where the red (black) error band shows the uncertainty from the MET scale and MC statistics (total uncertainty) on the single lepton scale factor. The blue histogram shows the contribution from just the dilepton and single τ backgrounds. The distributions for the T1tttt SMS (model A) with (mgluino, mLSP)=(1100 GeV, 1000 GeV) is overlaid for comparison. The lower plot shows (Data-Pred)/Error.

Observed MET distributions in the Lepton Spectrum method in data compared with predicted distributions (red bars) in the combined electron and muon channels, for events with Njet≥6, Nb≥3, and HT > 750 GeV. The red-bar histogram includes the total single lepton, dilepton, and single τ background prediction, where the red (black) error band shows the uncertainty from the MET scale and MC statistics (total uncertainty) on the single lepton scale factor. The blue histogram shows the contribution from just the dilepton and single τ backgrounds. The distributions for the T1tttt SMS (model A) with (mgluino, mLSP)=(1100 GeV, 1000 GeV) is overlaid for comparison. The lower plot shows (Data-Pred)/Error.

Observed MET distributions in the Lepton Spectrum method in data compared with predicted distributions (red bars) in the combined electron and muon channels, for events with Njet≥6, Nb≥3, and HT > 1000 GeV. The red-bar histogram includes the total single lepton, dilepton, and single τ background prediction, where the red (black) error band shows the uncertainty from the MET scale and MC statistics (total uncertainty) on the single lepton scale factor. The blue histogram shows the contribution from just the dilepton and single τ backgrounds. The distributions for the T1tttt SMS (model A) with (mgluino, mLSP)=(1100 GeV, 1000 GeV) is overlaid for comparison. The lower plot shows (Data-Pred)/Error.

Observed MET distributions in the Lepton Spectrum method in data compared with predicted distributions (red bars) in the combined electron and muon channels, for events with 3≤Njet≤5, Nb≥3, and HT > 500 GeV. The red-bar histogram includes the total single lepton, dilepton, and single τ background prediction, where the red (black) error band shows the uncertainty from the MET scale and MC statistics (total uncertainty) on the single lepton scale factor. The blue histogram shows the contribution from just the dilepton and single τ backgrounds. The distributions for the T1tttt SMS (model A) with (mgluino, mLSP)=(1100 GeV, 1000 GeV) is overlaid for comparison. The lower plot shows (Data-Pred)/Error.

Observed MET distributions in the Lepton Spectrum method in data compared with predicted distributions (red bars) in the combined electron and muon channels, for events with 3≤Njet≤5, Nb≥3, and HT > 750 GeV. The red-bar histogram includes the total single lepton, dilepton, and single τ background prediction, where the red (black) error band shows the uncertainty from the MET scale and MC statistics (total uncertainty) on the single lepton scale factor. The blue histogram shows the contribution from just the dilepton and single τ backgrounds. The distributions for the T1tttt SMS (model A) with (mgluino, mLSP)=(1100 GeV, 1000 GeV) is overlaid for comparison. The lower plot shows (Data-Pred)/Error.

Observed MET distributions in the Lepton Spectrum method in data compared with predicted distributions (red bars) in the combined electron and muon channels, for events with 3≤Njet≤5, Nb≥3, and HT > 1000 GeV. The red-bar histogram includes the total single lepton, dilepton, and single τ background prediction, where the red (black) error band shows the uncertainty from the MET scale and MC statistics (total uncertainty) on the single lepton scale factor. The blue histogram shows the contribution from just the dilepton and single τ backgrounds. The distributions for the T1tttt SMS (model A) with (mgluino, mLSP)=(1100 GeV, 1000 GeV) is overlaid for comparison. The lower plot shows (Data-Pred)/Error.

95% confidence level (C.L.) upper limits on the production cross section in the T1tttt model (model A) for the Lepton Spectrum method. Limits are extracted from a combination of results in bins in MET and Nb for a given HT selection. The final limit at each point comes from the HT selection that gives the best expected limit. The z axis corresponds to the observed limit. The observed (±1σ theory) and expected (±1σ experimental) limit contours are also shown. A text file containing the cross section upper limit at each point can be found here.

95% confidence level (C.L.) upper limits on the production cross section in the T1t1t model (model B) for the Lepton Spectrum method. Limits are extracted from a combination of results in bins in MET and Nb for a given HT selection. The final limit at each point comes from the HT selection that gives the best expected limit. The z axis corresponds to the observed limit. The observed (±1σ theory) and expected (±1σ experimental) limit contours are also shown. A text file containing the cross section upper limit at each point can be found here.

95% confidence level (C.L.) upper limits on the production cross section in the T5tttt model (model C) for the Lepton Spectrum method. Limits are extracted from a combination of results in bins in MET and Nb for a given HT selection. The final limit at each point comes from the HT selection that gives the best expected limit. The z axis corresponds to the observed limit. The observed (±1σ theory) and expected (±1σ experimental) limit contours are also shown. A text file containing the cross section upper limit at each point can be found here.

Plots of Signal Efficiency for the Lepton Spectrum and MET Templates Methods

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 500 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 500 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 500 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb=2, HT> 750 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb=2, HT> 750 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb=2, HT> 750 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 1000 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 1000 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 1000 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 500 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 500 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 500 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb≥3, HT> 750 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb≥3, HT> 750 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb≥3, HT> 750 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 1000 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 1000 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 1000 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the MET Templates method for Njet≥ 6, Nb≥3, 400<HT< 750 Gev, and 150<MET<250 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the MET Templates method for Njet≥ 6, Nb≥3, 400<HT< 750 Gev, and MET>250 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1tttt (model A) plane in the MET Templates method for Njet≥ 6, Nb≥3, HT> 750 Gev, and 150<MET<250 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 500 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 500 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 500 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb=2, HT> 750 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb=2, HT> 750 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb=2, HT> 750 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 1000 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 1000 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 1000 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 500 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 500 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 500 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb≥3, HT> 750 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb≥3, HT> 750 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb≥3, HT> 750 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 1000 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 1000 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 1000 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the MET Templates method for Njet≥ 6, Nb≥3, 400<HT< 750 Gev, and 150<MET<250 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the MET Templates method for Njet≥ 6, Nb≥3, 400<HT< 750 Gev, and MET>250 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T1t1t (model B) plane in the MET Templates method for Njet≥ 6, Nb≥3, HT> 750 Gev, and 150<MET<250 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 500 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 500 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 500 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb=2, HT> 750 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb=2, HT> 750 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb=2, HT> 750 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 1000 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 1000 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum method for Njet≥ 6, Nb=2, HT> 1000 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 500 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 500 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 500 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb≥3, HT> 750 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb≥3, HT> 750 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum and MET Templates methods for Njet≥ 6, Nb≥3, HT> 750 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 1000 Gev, and 250<MET<350 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 1000 Gev, and 350<MET<450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the Lepton Spectrum method for Njet≥ 6, Nb≥3, HT> 1000 Gev, and MET>450 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the MET Templates method for Njet≥ 6, Nb≥3, 400<HT< 750 Gev, and 150<MET<250 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the MET Templates method for Njet≥ 6, Nb≥3, 400<HT< 750 Gev, and MET>250 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.

Signal efficiency times acceptance across the T5tttt (model C) plane in the MET Templates method for Njet≥ 6, Nb≥3, HT> 750 Gev, and 150<MET<250 GeV. A .C ROOT executable to reproduce this plot can be found here. This code also contains a commented section which contains the signal efficiency times acceptance at each point.





Plots from the MET template method



Results from the fit to the MET spectrum for events with 1 b-tagged jet and HT > 400 GeV. The points represent data. The red error band reflects the statistical uncertainties and the blue error band shows the combined statistical and systematic uncertainties (with the exception of closure). The control regions used for the fit are defined by 400 < HT < 2500 GeV and 150 < MET < 1500 GeV for events with Nb=1 and 400 < HT < 750 GeV and 150 < MET < 400 GeV for events with Nb=2.

Results from the fit to the MET spectrum for events with 1 b-tagged jet and HT > 750 GeV. The points represent data. The red error band reflects the statistical uncertainties and the blue error band shows the combined statistical and systematic uncertainties (with the exception of closure). The control regions used for the fit are defined by 400 < HT < 2500 GeV and 150 < MET < 1500 GeV for events with Nb=1 and 400 < HT < 750 GeV and 150 < MET < 400 GeV for events with Nb=2.

Results from the fit to the MET spectrum for events with 1 b-tagged jet and HT > 1000 GeV. The points represent data. The red error band reflects the statistical uncertainties and the blue error band shows the combined statistical and systematic uncertainties (with the exception of closure). The control regions used for the fit are defined by 400 < HT < 2500 GeV and 150 < MET < 1500 GeV for events with Nb=1 and 400 < HT < 750 GeV and 150 < MET < 400 GeV for events with Nb=2.

Results from the fit to the MET spectrum for events with 2 b-tagged jets and HT > 400 GeV. The points represent data. The red error band reflects the statistical uncertainties and the blue error band shows the combined statistical and systematic uncertainties (with the exception of closure). The control regions used for the fit are defined by 400 < HT < 2500 GeV and 150 < MET < 1500 GeV for events with Nb=1 and 400 < HT < 750 GeV and 150 < MET < 400 GeV for events with Nb=2.

Results from the fit to the MET spectrum for events with 2 b-tagged jets and HT > 750 GeV. The points represent data. The red error band reflects the statistical uncertainties and the blue error band shows the combined statistical and systematic uncertainties (with the exception of closure). The control regions used for the fit are defined by 400 < HT < 2500 GeV and 150 < MET < 1500 GeV for events with Nb=1 and 400 < HT < 750 GeV and 150 < MET < 400 GeV for events with Nb=2.

Results from the fit to the MET spectrum for events with 2 b-tagged jets and HT > 1000 GeV. The points represent data. The red error band reflects the statistical uncertainties and the blue error band shows the combined statistical and systematic uncertainties (with the exception of closure). The control regions used for the fit are defined by 400 < HT < 2500 GeV and 150 < MET < 1500 GeV for events with Nb=1 and 400 < HT < 750 GeV and 150 < MET < 400 GeV for events with Nb=2.

95% confidence level (C.L.) upper limits on the production cross section in the T1tttt model for the MET template method. The z axis corresponds to the observed limit. The observed (±1σ theory) and expected (±1σ experimental) limit contours are also shown.

95% confidence level (C.L.) upper limits on the production cross section in the T1t1t model (model B) for the MET template method. The z axis corresponds to the observed limit. The observed (±1σ theory) and expected (±1σ experimental) limit contours are also shown.

95% confidence level (C.L.) upper limits on the production cross section in the T5tttt model (model C) for the MET template method. The z axis corresponds to the observed limit. The observed (±1σ theory) and expected (±1σ experimental) limit contours are also shown.



Plots and tables from the Delta Phi (∆φ(W,l)) Method

RCS[QCD] for QCD events in the electron channel estimated in the anti-selected sample in data for different b-tag multiplicities and STlep bins.

Binned likelihood fit in Lp for electron events with Nb=1 and 250<STlep<350 GeV. The EWK template is shown with blue, the QCD template with yellow and the fit result with red. Data are with black markers.

Systematic uncertainties of the κ factor for events with Nb≥3. The two lepton flavors are combined.

Signal efficiency times acceptance across the T1tttt plane (model A) in the ∆φ(W,l) method for Nj≥ 6, Nb=2, HT>500 GeV, and 250<ST<350 GeV. Muons on the left, electrons on the right. The stop mass is fixed at 1 TeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T1tttt_Muons_ST250_Nb2_EffxAcc_Values.txt and DPhi_Method_T1tttt_Elect_ST250_Nb2_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T1tttt (model A) plane in the ∆φ(W,l) method for Nj≥ 6, Nb=2, HT>500 GeV, and 350<ST<450 GeV. Muons on the left, electrons on the right. The stop mass is fixed at 1 TeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T1tttt_Muons_ST350_Nb2_EffxAcc_Values.txt and DPhi_Method_T1tttt_Elect_ST350_Nb2_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T1tttt (model A) plane in the ∆φ(W,l) method for Nj≥ 6, Nb=2, HT>500 GeV, and ST>450 GeV. Muons on the left, electrons on the right. The stop mass is fixed at 1 TeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T1tttt_Muons_ST450_Nb2_EffxAcc_Values.txt and DPhi_Method_T1tttt_Elect_ST450_Nb2_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T1tttt (model A) plane in the ∆φ(W,l) method for Nj≥ 6, Nb≥3, HT>500 GeV, and 250<ST<350 GeV. Muons on the left, electrons on the right. The stop mass is fixed at 1 TeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T1tttt_Muons_ST250_Nb3_EffxAcc_Values.txt and DPhi_Method_T1tttt_Elect_ST250_Nb3_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T1tttt (model A) plane in the ∆φ(W,l) method for Nj≥ 6, Nb≥3, HT>500 GeV, and 350<ST<450 GeV. Muons on the left, electrons on the right. The stop mass is fixed at 1 TeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T1tttt_Muons_ST350_Nb3_EffxAcc_Values.txt and DPhi_Method_T1tttt_Elect_ST350_Nb3_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.C script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T1tttt (model A) plane in the ∆φ(W,l) method for Nj≥ 6, Nb≥3, HT>500 GeV, and ST>450 GeV. Muons on the left, electrons on the right. The stop mass is fixed at 1 TeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T1tttt_Muons_ST450_Nb3_EffxAcc_Values.txt and DPhi_Method_T1tttt_Elect_ST450_Nb3_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T1t1t (model B) plane in the ∆φ(W,l) method for Nj≥ 6, Nb=2, HT>500 GeV, and 250<ST<350 GeV. Muons left, electrons right. The gluino mass is fixed at 1 TeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T1t1t_Muons_ST250_Nb2_EffxAcc_Values.txt and DPhi_Method_T1t1t_Elect_ST250_Nb2_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T1t1t (model B) plane in the ∆φ(W,l) method for Nj≥ 6, Nb=2, HT>500 GeV, and 350<ST<450 GeV. Muons on the left, electrons on the right. The gluino mass is fixed at 1 TeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T1t1t_Muons_ST350_Nb2_EffxAcc_Values.txt and DPhi_Method_T1t1t_Elect_ST350_Nb2_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T1t1t (model B) plane in the ∆φ(W,l) method for Nj≥ 6, Nb=2, HT>500 GeV, and ST>450 GeV. Muons on the left, electrons on the right. The gluino mass is fixed at 1 TeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T1t1t_Muons_ST450_Nb2_EffxAcc_Values.txt and DPhi_Method_T1t1t_Elect_ST450_Nb2_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T1t1t (model B) plane in the ∆φ(W,l) method for Nj≥ 6, Nb≥3, HT>500 GeV, and 250<ST<350 GeV. Muons on the left, electrons on the right. The gluino mass is fixed at 1 TeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T1t1t_Muons_ST250_Nb3_EffxAcc_Values.txt and DPhi_Method_T1t1t_Elect_ST250_Nb3_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T1t1t (model B) plane in the ∆φ(W,l) method for Nj≥ 6, Nb≥3, HT>500 GeV, and 350<ST<450 GeV. Muons on the left, electrons on the right. The gluino mass is fixed at 1 TeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T1t1t_Muons_ST350_Nb3_EffxAcc_Values.txt and DPhi_Method_T1t1t_Elect_ST350_Nb3_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T1t1t (model B) plane in the ∆φ(W,l) method for Nj≥ 6, Nb≥3, HT>500 GeV, and ST>450 GeV. Muons on the left, electrons on the right. The gluino mass is fixed at 1 TeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T1t1t_Muons_ST450_Nb3_EffxAcc_Values.txt and DPhi_Method_T1t1t_Elect_ST450_Nb3_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T5tttt (model C) plane in the ∆φ(W,l) method for Nj≥ 6, Nb=2, HT>500 GeV, and 250<ST<350 GeV. Muons on the left, electrons on the right. The LSP mass is fixed at 50 GeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T5tttt_Muons_ST250_Nb2_EffxAcc_Values.txt and DPhi_Method_T5tttt_Elect_ST250_Nb2_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T5tttt (model C) plane in the ∆φ(W,l) method for Nj≥ 6, Nb=2, HT>500 GeV, and 350<ST<450 GeV. Muons on the left, electrons on the right. The LSP mass is fixed at 50 GeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T5tttt_Muons_ST350_Nb2_EffxAcc_Values.txt and DPhi_Method_T5tttt_Elect_ST350_Nb2_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T5tttt (model C) plane in the ∆φ(W,l) method for Nj≥ 6, Nb=2, HT>500 GeV, and ST>450 GeV. Muons on the left, electrons on the right. The LSP mass is fixed at 50 GeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T5tttt_Muons_ST450_Nb2_EffxAcc_Values.txt and DPhi_Method_T5tttt_Elect_ST450_Nb2_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T5tttt (model C) plane in the ∆φ(W,l) method for Nj≥ 6, Nb≥3, HT>500 GeV, and 250<ST<350 GeV. Muons on the left, electrons on the right. The LSP mass is fixed at 50 GeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T5tttt_Muons_ST250_Nb3_EffxAcc_Values.txt and DPhi_Method_T5tttt_Elect_ST250_Nb3_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T5tttt (model C) plane in the ∆φ(W,l) method for Nj≥ 6, Nb≥3, HT>500 GeV, and 350<ST<450 GeV. Muons on the left, electrons on the right. The LSP mass is fixed at 50 GeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T5tttt_Muons_ST350_Nb3_EffxAcc_Values.txt and DPhi_Method_T5tttt_Elect_ST350_Nb3_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)

Signal efficiency times acceptance across the T5tttt (model C) plane in the ∆φ(W,l) method for Nj≥ 6, Nb≥3, HT>500 GeV, and ST>450 GeV. Muons on the left, electrons on the right. The LSP mass is fixed at 50 GeV in this model. The explicit vales of these plots are provided below in the txt files: DPhi_Method_T5tttt_Muons_ST450_Nb3_EffxAcc_Values.txt and DPhi_Method_T5tttt_Elect_ST450_Nb3_EffxAcc_Values.txt. (Plots and values can be reproduced with the Plot_EffxAcc.cpp script and the EffxAcc_Smoothed_DPhi_Paper_Dec2013.root root file which are also provided below.)
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Texttxt DPhi_Method_T1t1t_Elect_ST250_Nb2_EffxAcc_Values.txt r1 manage 9.7 K 2013-11-29 - 22:56 AntoniosAgapitos  
Texttxt DPhi_Method_T1t1t_Elect_ST250_Nb3_EffxAcc_Values.txt r1 manage 9.7 K 2013-11-29 - 22:56 AntoniosAgapitos  
Texttxt DPhi_Method_T1t1t_Elect_ST350_Nb2_EffxAcc_Values.txt r1 manage 9.7 K 2013-11-29 - 22:56 AntoniosAgapitos  
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Texttxt DPhi_Method_T1t1t_Elect_ST450_Nb2_EffxAcc_Values.txt r1 manage 9.7 K 2013-11-29 - 22:56 AntoniosAgapitos  
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Texttxt DPhi_Method_T1t1t_Muons_ST250_Nb3_EffxAcc_Values.txt r1 manage 9.7 K 2013-11-29 - 23:02 AntoniosAgapitos  
Texttxt DPhi_Method_T1t1t_Muons_ST350_Nb2_EffxAcc_Values.txt r1 manage 9.7 K 2013-11-29 - 23:02 AntoniosAgapitos  
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Texttxt DPhi_Method_T1tttt_Elect_ST250_Nb3_EffxAcc_Values.txt r1 manage 52.4 K 2013-11-29 - 23:05 AntoniosAgapitos  
Texttxt DPhi_Method_T1tttt_Elect_ST350_Nb2_EffxAcc_Values.txt r1 manage 52.5 K 2013-11-29 - 23:09 AntoniosAgapitos  
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Texttxt DPhi_Method_T5tttt_Elect_ST250_Nb3_EffxAcc_Values.txt r1 manage 39.1 K 2013-11-29 - 23:17 AntoniosAgapitos  
Texttxt DPhi_Method_T5tttt_Elect_ST350_Nb2_EffxAcc_Values.txt r1 manage 39.1 K 2013-11-29 - 23:17 AntoniosAgapitos  
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Texttxt Dphi_ExcludedXsections.txt r1 manage 53.8 K 2013-04-01 - 22:28 AntoniosAgapitos  
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Texttxt EffxAcc_El_ST450_Nb2.txt r1 manage 25.6 K 2013-04-01 - 22:27 AntoniosAgapitos  
Texttxt EffxAcc_El_ST450_Nb3.txt r1 manage 25.5 K 2013-04-01 - 22:27 AntoniosAgapitos  
Texttxt EffxAcc_Mu_ST250_Nb2.txt r1 manage 25.8 K 2013-04-01 - 22:29 AntoniosAgapitos  
Texttxt EffxAcc_Mu_ST250_Nb3.txt r1 manage 25.8 K 2013-04-01 - 22:31 AntoniosAgapitos  
Texttxt EffxAcc_Mu_ST350_Nb2.txt r1 manage 25.9 K 2013-04-01 - 22:29 AntoniosAgapitos  
Texttxt EffxAcc_Mu_ST350_Nb3.txt r1 manage 25.9 K 2013-04-01 - 22:29 AntoniosAgapitos  
Texttxt EffxAcc_Mu_ST450_Nb2.txt r1 manage 25.5 K 2013-04-01 - 22:29 AntoniosAgapitos  
Texttxt EffxAcc_Mu_ST450_Nb3.txt r1 manage 25.4 K 2013-04-01 - 22:29 AntoniosAgapitos  
Unknown file formatroot EffxAcc_Smoothed_DPhi_Paper_Dec2013.root r1 manage 708.1 K 2013-11-29 - 22:54 AntoniosAgapitos  
PDFpdf El_250_Nb2.pdf r1 manage 25.6 K 2013-04-01 - 02:17 AntoniosAgapitos  
PNGpng El_250_Nb2.png r1 manage 24.8 K 2013-04-01 - 02:17 AntoniosAgapitos  
PDFpdf El_250_Nb3.pdf r1 manage 26.0 K 2013-04-01 - 02:17 AntoniosAgapitos  
PNGpng El_250_Nb3.png r1 manage 24.9 K 2013-04-01 - 02:17 AntoniosAgapitos  
PDFpdf El_350_Nb2.pdf r1 manage 25.4 K 2013-04-01 - 02:17 AntoniosAgapitos  
PNGpng El_350_Nb2.png r1 manage 24.4 K 2013-04-01 - 02:17 AntoniosAgapitos  
PDFpdf El_350_Nb3.pdf r1 manage 25.7 K 2013-04-01 - 02:17 AntoniosAgapitos  
PNGpng El_350_Nb3.png r1 manage 24.8 K 2013-04-01 - 02:17 AntoniosAgapitos  
PDFpdf El_450_Nb2.pdf r1 manage 24.8 K 2013-04-01 - 02:50 AntoniosAgapitos  
PNGpng El_450_Nb2.png r1 manage 21.9 K 2013-04-01 - 02:50 AntoniosAgapitos  
PDFpdf El_450_Nb3.pdf r1 manage 25.2 K 2013-04-01 - 02:50 AntoniosAgapitos  
PNGpng El_450_Nb3.png r1 manage 22.1 K 2013-04-01 - 02:50 AntoniosAgapitos  
PDFpdf Fig3_RCS_250_v4.pdf r1 manage 13.9 K 2013-11-22 - 12:05 AntoniosAgapitos  
PNGpng Fig3_RCS_250_v4.png r1 manage 13.4 K 2013-11-22 - 12:59 AntoniosAgapitos  
PDFpdf Fig3_RCS_350_v4.pdf r1 manage 13.9 K 2013-11-22 - 12:05 AntoniosAgapitos  
PNGpng Fig3_RCS_350_v4.png r1 manage 13.5 K 2013-11-22 - 12:59 AntoniosAgapitos  
PDFpdf Fig3_RCS_450_v4.pdf r1 manage 13.9 K 2013-11-22 - 12:05 AntoniosAgapitos  
PNGpng Fig3_RCS_450_v4.png r1 manage 13.1 K 2013-11-22 - 12:59 AntoniosAgapitos  
PDFpdf LS_DP_combinedLimit_T1tttt.pdf r1 manage 18.9 K 2013-03-07 - 06:49 DavidStuart LS_DP_combinedLimit_T1tttt.pdf
PNGpng LS_DP_combinedLimit_T1tttt.png r1 manage 173.4 K 2013-03-07 - 06:50 DavidStuart LS_DP_combinedLimit_T1tttt.png
PDFpdf LS_MT_CombinedTable.pdf r2 r1 manage 100.8 K 2013-11-26 - 16:34 PaulGeffert  
PNGpng LS_MT_CombinedTable.png r1 manage 233.6 K 2013-11-26 - 16:28 PaulGeffert  
PDFpdf LS_T1t1t_bestlimit_observedZaxis_btagbins.pdf r1 manage 32.7 K 2013-11-22 - 19:12 PaulGeffert  
PNGpng LS_T1t1t_bestlimit_observedZaxis_btagbins.png r1 manage 161.4 K 2013-11-22 - 19:12 PaulGeffert  
Texttxt LS_T1t1t_bestlimit_observedZaxis_btagbins.txt r1 manage 17.5 K 2013-11-22 - 19:43 PaulGeffert  
PDFpdf LS_T1tttt_bestlimit_observedZaxis.pdf r1 manage 27.4 K 2013-03-07 - 06:50 DavidStuart LS_T1tttt_bestlimit_observedZaxis.pdf
PNGpng LS_T1tttt_bestlimit_observedZaxis.png r1 manage 188.1 K 2013-03-07 - 06:51 DavidStuart LS_T1tttt_bestlimit_observedZaxis.png
PDFpdf LS_T1tttt_bestlimit_observedZaxis_btagbins.pdf r1 manage 50.8 K 2013-11-22 - 19:12 PaulGeffert  
PNGpng LS_T1tttt_bestlimit_observedZaxis_btagbins.png r1 manage 205.3 K 2013-11-22 - 19:12 PaulGeffert  
Texttxt LS_T1tttt_bestlimit_observedZaxis_btagbins.txt r1 manage 58.5 K 2013-11-22 - 19:43 PaulGeffert  
PDFpdf LS_T5tttt_bestlimit_observedZaxis_btagbins.pdf r2 r1 manage 50.3 K 2013-11-27 - 13:53 PaulGeffert  
PNGpng LS_T5tttt_bestlimit_observedZaxis_btagbins.png r2 r1 manage 198.4 K 2013-11-27 - 13:53 PaulGeffert  
Texttxt LS_T5tttt_bestlimit_observedZaxis_btagbins.txt r1 manage 40.1 K 2013-11-22 - 19:43 PaulGeffert  
PDFpdf LepTauHad_kappa_Njetge6_2b.pdf r1 manage 14.9 K 2013-11-22 - 19:10 PaulGeffert  
PNGpng LepTauHad_kappa_Njetge6_2b.png r1 manage 74.3 K 2013-11-22 - 19:11 PaulGeffert  
PDFpdf LepTauHad_kappa_Njetge6_ge2b.pdf r1 manage 14.9 K 2013-03-07 - 06:45 DavidStuart LepTauHad_kappa_Njetge6_ge2b.pdf
PNGpng LepTauHad_kappa_Njetge6_ge2b.png r1 manage 76.9 K 2013-03-07 - 06:45 DavidStuart LepTauHad_kappa_Njetge6_ge2b.png
PDFpdf LepTauLep_kappa_Njetge6_2b.pdf r1 manage 14.9 K 2013-11-22 - 19:10 PaulGeffert  
PNGpng LepTauLep_kappa_Njetge6_2b.png r1 manage 74.4 K 2013-11-22 - 19:11 PaulGeffert  
PDFpdf LepTauLep_kappa_Njetge6_ge2b.pdf r1 manage 14.9 K 2013-03-07 - 06:46 DavidStuart LepTauLep_kappa_Njetge6_ge2b.pdf
PNGpng LepTauLep_kappa_Njetge6_ge2b.png r1 manage 76.8 K 2013-03-07 - 06:46 DavidStuart LepTauLep_kappa_Njetge6_ge2b.png
PDFpdf LostIgnoredPred_Dilepton_TypeIMET_EMu_HT1000_Njetge6_2b.pdf r1 manage 14.1 K 2013-11-22 - 19:10 PaulGeffert  
PNGpng LostIgnoredPred_Dilepton_TypeIMET_EMu_HT1000_Njetge6_2b.png r1 manage 79.4 K 2013-11-22 - 19:11 PaulGeffert  
PDFpdf LostIgnoredPred_Dilepton_TypeIMET_EMu_HT1000_Njetge6_ge2b.pdf r1 manage 14.2 K 2013-03-07 - 06:49 DavidStuart LostIgnoredPred_Dilepton_TypeIMET_EMu_HT1000_Njetge6_ge2b.pdf
PNGpng LostIgnoredPred_Dilepton_TypeIMET_EMu_HT1000_Njetge6_ge2b.png r1 manage 83.6 K 2013-03-07 - 06:49 DavidStuart LostIgnoredPred_Dilepton_TypeIMET_EMu_HT1000_Njetge6_ge2b.png
PDFpdf LostIgnoredPred_Dilepton_TypeIMET_EMu_HT500_Njetge6_2b.pdf r1 manage 14.1 K 2013-11-22 - 19:10 PaulGeffert  
PNGpng LostIgnoredPred_Dilepton_TypeIMET_EMu_HT500_Njetge6_2b.png r1 manage 79.8 K 2013-11-22 - 19:11 PaulGeffert  
PDFpdf LostIgnoredPred_Dilepton_TypeIMET_EMu_HT500_Njetge6_ge2b.pdf r1 manage 14.2 K 2013-03-07 - 06:47 DavidStuart LostIgnoredPred_Dilepton_TypeIMET_EMu_HT500_Njetge6_ge2b.pdf
PNGpng LostIgnoredPred_Dilepton_TypeIMET_EMu_HT500_Njetge6_ge2b.png r1 manage 82.1 K 2013-03-07 - 06:48 DavidStuart LostIgnoredPred_Dilepton_TypeIMET_EMu_HT500_Njetge6_ge2b.png
PDFpdf LostIgnoredPred_Dilepton_TypeIMET_EMu_HT750_Njetge6_2b.pdf r1 manage 14.1 K 2013-11-22 - 19:10 PaulGeffert  
PNGpng LostIgnoredPred_Dilepton_TypeIMET_EMu_HT750_Njetge6_2b.png r1 manage 79.8 K 2013-11-22 - 19:11 PaulGeffert  
PDFpdf LostIgnoredPred_Dilepton_TypeIMET_EMu_HT750_Njetge6_ge2b.pdf r1 manage 14.2 K 2013-03-07 - 06:48 DavidStuart LostIgnoredPred_Dilepton_TypeIMET_EMu_HT750_Njetge6_ge2b.pdf
PNGpng LostIgnoredPred_Dilepton_TypeIMET_EMu_HT750_Njetge6_ge2b.png r1 manage 82.9 K 2013-03-07 - 06:48 DavidStuart LostIgnoredPred_Dilepton_TypeIMET_EMu_HT750_Njetge6_ge2b.png
PDFpdf LostIgnored_syst-standalone.pdf r1 manage 42.9 K 2013-03-07 - 06:46 DavidStuart LostIgnored_syst-standalone.pdf
PNGpng LostIgnored_syst-standalone.png r1 manage 41.6 K 2013-03-07 - 06:47 DavidStuart LostIgnored_syst-standalone.png
PDFpdf LostIgnored_syst-standalone_Njetge6_2b.pdf r1 manage 64.3 K 2013-11-22 - 19:10 PaulGeffert  
PNGpng LostIgnored_syst-standalone_Njetge6_2b.png r1 manage 71.5 K 2013-11-22 - 19:11 PaulGeffert  
PDFpdf MC_PT_MET_comparison.pdf r1 manage 15.1 K 2013-03-07 - 06:51 DavidStuart MC_PT_MET_comparison.pdf
PNGpng MC_PT_MET_comparison.png r1 manage 8.0 K 2013-03-07 - 06:51 DavidStuart MC_PT_MET_comparison.png
PDFpdf Mu_250_Nb2.pdf r1 manage 25.7 K 2013-04-01 - 01:44 AntoniosAgapitos  
PNGpng Mu_250_Nb2.png r1 manage 24.8 K 2013-04-01 - 01:44 AntoniosAgapitos  
PDFpdf Mu_250_Nb3.pdf r1 manage 26.2 K 2013-04-01 - 02:01 AntoniosAgapitos  
PNGpng Mu_250_Nb3.png r1 manage 24.7 K 2013-04-01 - 02:01 AntoniosAgapitos  
PDFpdf Mu_350_Nb2.pdf r1 manage 25.5 K 2013-04-01 - 02:01 AntoniosAgapitos  
PNGpng Mu_350_Nb2.png r1 manage 24.5 K 2013-04-01 - 02:01 AntoniosAgapitos  
PDFpdf Mu_350_Nb3.pdf r1 manage 26.0 K 2013-04-01 - 02:01 AntoniosAgapitos  
PNGpng Mu_350_Nb3.png r1 manage 24.5 K 2013-04-01 - 02:01 AntoniosAgapitos  
PDFpdf Mu_450_Nb2.pdf r1 manage 25.2 K 2013-04-01 - 02:50 AntoniosAgapitos  
PNGpng Mu_450_Nb2.png r1 manage 22.0 K 2013-04-01 - 02:50 AntoniosAgapitos  
PDFpdf Mu_450_Nb3.pdf r1 manage 25.7 K 2013-04-01 - 02:50 AntoniosAgapitos  
PNGpng Mu_450_Nb3.png r1 manage 21.9 K 2013-04-01 - 02:50 AntoniosAgapitos  
PDFpdf Mu_ANplots250_NOLPsecondD500DeltaPhiMuWPT_tot_3.pdf r1 manage 16.1 K 2013-11-22 - 12:05 AntoniosAgapitos  
PNGpng Mu_ANplots250_NOLPsecondD500DeltaPhiMuWPT_tot_3.png r3 r2 r1 manage 13.6 K 2013-11-22 - 12:59 AntoniosAgapitos  
PDFpdf Mu_ANplots250_NOLPsecondD500DeltaPhiMuWPT_tot_AA.pdf r1 manage 18.5 K 2013-03-07 - 06:52 DavidStuart Mu_ANplots250_NOLPsecondD500DeltaPhiMuWPT_tot_AA.pdf
PNGpng Mu_ANplots250_NOLPsecondD500DeltaPhiMuWPT_tot_AA.png r1 manage 106.9 K 2013-03-07 - 06:52 DavidStuart Mu_ANplots250_NOLPsecondD500DeltaPhiMuWPT_tot_AA.png
PDFpdf Mu_ANplots350_NOLPsecondD500DeltaPhiMuWPT_tot_3.pdf r1 manage 15.6 K 2013-11-22 - 12:05 AntoniosAgapitos  
PNGpng Mu_ANplots350_NOLPsecondD500DeltaPhiMuWPT_tot_3.png r1 manage 13.3 K 2013-11-22 - 12:59 AntoniosAgapitos  
PDFpdf Mu_ANplots350_NOLPsecondD500DeltaPhiMuWPT_tot_AA.pdf r1 manage 18.4 K 2013-03-07 - 06:52 DavidStuart Mu_ANplots350_NOLPsecondD500DeltaPhiMuWPT_tot_AA.pdf
PNGpng Mu_ANplots350_NOLPsecondD500DeltaPhiMuWPT_tot_AA.png r1 manage 104.8 K 2013-03-07 - 06:53 DavidStuart Mu_ANplots350_NOLPsecondD500DeltaPhiMuWPT_tot_AA.png
PNGpng Mu_ANplots450_NOLPsecondD500DeltaPhiMuWPT_tot_.png r1 manage 38.8 K 2013-11-22 - 12:35 AntoniosAgapitos  
PDFpdf Mu_ANplots450_NOLPsecondD500DeltaPhiMuWPT_tot_3.pdf r1 manage 15.6 K 2013-11-22 - 12:05 AntoniosAgapitos  
PNGpng Mu_ANplots450_NOLPsecondD500DeltaPhiMuWPT_tot_3.png r1 manage 12.8 K 2013-11-22 - 12:59 AntoniosAgapitos  
PDFpdf Mu_ANplots450_NOLPsecondD500DeltaPhiMuWPT_tot_AA.pdf r1 manage 16.9 K 2013-03-07 - 06:53 DavidStuart Mu_ANplots450_NOLPsecondD500DeltaPhiMuWPT_tot_AA.pdf
PNGpng Mu_ANplots450_NOLPsecondD500DeltaPhiMuWPT_tot_AA.png r1 manage 103.5 K 2013-03-07 - 06:54 DavidStuart Mu_ANplots450_NOLPsecondD500DeltaPhiMuWPT_tot_AA.png
C source code filec Plot_EffxAcc.C r1 manage 8.3 K 2013-04-01 - 22:33 AntoniosAgapitos  
C source code filecpp Plot_EffxAcc.cpp r1 manage 9.4 K 2013-11-29 - 22:54 AntoniosAgapitos  
PDFpdf QCDest_Dphi_Rcs_AntiSelectedData.pdf r2 r1 manage 43.0 K 2013-12-01 - 23:44 LoukasGouskos  
PNGpng QCDest_Dphi_Rcs_AntiSelectedData.png r2 r1 manage 53.0 K 2013-12-01 - 23:45 LoukasGouskos RCS[QCD] for electron events in the antiselected sample in data
PDFpdf QCDfit_Lp_ST250b_Nb1_HT500.pdf r2 r1 manage 74.4 K 2013-12-01 - 23:47 LoukasGouskos  
PNGpng QCDfit_Lp_ST250b_Nb1_HT500.png r2 r1 manage 88.5 K 2013-12-01 - 23:47 LoukasGouskos Lp fit results in electrons
PDFpdf RcsVsNbtags_6Njets8_ST250.pdf r1 manage 13.8 K 2013-03-07 - 06:54 DavidStuart RcsVsNbtags_6Njets8_ST250.pdf
PNGpng RcsVsNbtags_6Njets8_ST250.png r1 manage 60.2 K 2013-03-07 - 06:54 DavidStuart RcsVsNbtags_6Njets8_ST250.png
PDFpdf RcsVsNbtags_6Njets8_ST350.pdf r1 manage 13.8 K 2013-03-07 - 06:55 DavidStuart RcsVsNbtags_6Njets8_ST350.pdf
PNGpng RcsVsNbtags_6Njets8_ST350.png r1 manage 61.3 K 2013-03-07 - 06:55 DavidStuart RcsVsNbtags_6Njets8_ST350.png
PDFpdf RcsVsNbtags_6Njets8_ST450.pdf r1 manage 13.8 K 2013-03-07 - 06:55 DavidStuart RcsVsNbtags_6Njets8_ST450.pdf
PNGpng RcsVsNbtags_6Njets8_ST450.png r1 manage 61.2 K 2013-03-07 - 06:56 DavidStuart RcsVsNbtags_6Njets8_ST450.png
PDFpdf SingleTau_kappa_Njetge6_2b.pdf r1 manage 14.9 K 2013-11-22 - 19:12 PaulGeffert  
PNGpng SingleTau_kappa_Njetge6_2b.png r1 manage 73.9 K 2013-11-22 - 19:12 PaulGeffert  
PDFpdf SingleTau_kappa_Njetge6_ge2b.pdf r1 manage 14.9 K 2013-03-07 - 06:56 DavidStuart SingleTau_kappa_Njetge6_ge2b.pdf
PNGpng SingleTau_kappa_Njetge6_ge2b.png r1 manage 76.4 K 2013-03-07 - 06:57 DavidStuart SingleTau_kappa_Njetge6_ge2b.png
PDFpdf T1t1tRA4MTXSEC.pdf r1 manage 23.0 K 2013-11-27 - 09:53 WolfgangAdam  
PNGpng T1t1tRA4MTXSEC.png r1 manage 108.1 K 2013-11-27 - 09:53 WolfgangAdam  
C source code filec T1t1t_HT1000_Njetge6_2b_efficiency_METbin1.C r1 manage 40.4 K 2013-11-22 - 19:36 PaulGeffert  
PDFpdf T1t1t_HT1000_Njetge6_2b_efficiency_METbin1.pdf r1 manage 20.4 K 2013-11-22 - 19:15 PaulGeffert  
PNGpng T1t1t_HT1000_Njetge6_2b_efficiency_METbin1.png r1 manage 45.9 K 2013-11-22 - 19:18 PaulGeffert  
C source code filec T1t1t_HT1000_Njetge6_2b_efficiency_METbin2.C r1 manage 40.5 K 2013-11-22 - 19:36 PaulGeffert  
PDFpdf T1t1t_HT1000_Njetge6_2b_efficiency_METbin2.pdf r1 manage 20.2 K 2013-11-22 - 19:15 PaulGeffert  
PNGpng T1t1t_HT1000_Njetge6_2b_efficiency_METbin2.png r1 manage 45.5 K 2013-11-22 - 19:18 PaulGeffert  
C source code filec T1t1t_HT1000_Njetge6_2b_efficiency_METbin3.C r1 manage 40.4 K 2013-11-22 - 19:36 PaulGeffert  
PDFpdf T1t1t_HT1000_Njetge6_2b_efficiency_METbin3.pdf r1 manage 20.2 K 2013-11-22 - 19:15 PaulGeffert  
PNGpng T1t1t_HT1000_Njetge6_2b_efficiency_METbin3.png r1 manage 46.7 K 2013-11-22 - 19:18 PaulGeffert  
C source code filec T1t1t_HT1000_Njetge6_ge3b_efficiency_METbin1.C r1 manage 40.4 K 2013-11-22 - 19:35 PaulGeffert  
PDFpdf T1t1t_HT1000_Njetge6_ge3b_efficiency_METbin1.pdf r1 manage 20.5 K 2013-11-22 - 19:13 PaulGeffert  
PNGpng T1t1t_HT1000_Njetge6_ge3b_efficiency_METbin1.png r1 manage 46.3 K 2013-11-22 - 19:17 PaulGeffert  
C source code filec T1t1t_HT1000_Njetge6_ge3b_efficiency_METbin2.C r1 manage 40.5 K 2013-11-22 - 19:35 PaulGeffert  
PDFpdf T1t1t_HT1000_Njetge6_ge3b_efficiency_METbin2.pdf r1 manage 20.3 K 2013-11-22 - 19:13 PaulGeffert  
PNGpng T1t1t_HT1000_Njetge6_ge3b_efficiency_METbin2.png r1 manage 45.8 K 2013-11-22 - 19:17 PaulGeffert  
C source code filec T1t1t_HT1000_Njetge6_ge3b_efficiency_METbin3.C r1 manage 40.4 K 2013-11-22 - 19:35 PaulGeffert  
PDFpdf T1t1t_HT1000_Njetge6_ge3b_efficiency_METbin3.pdf r1 manage 20.3 K 2013-11-22 - 19:13 PaulGeffert  
PNGpng T1t1t_HT1000_Njetge6_ge3b_efficiency_METbin3.png r1 manage 47.0 K 2013-11-22 - 19:17 PaulGeffert  
C source code filec T1t1t_HT400_Njetge6_ge3b_efficiency_METbin0.C r1 manage 40.4 K 2013-11-22 - 19:35 PaulGeffert  
PDFpdf T1t1t_HT400_Njetge6_ge3b_efficiency_METbin0.pdf r1 manage 20.4 K 2013-11-22 - 19:13 PaulGeffert  
PNGpng T1t1t_HT400_Njetge6_ge3b_efficiency_METbin0.png r1 manage 46.3 K 2013-11-22 - 19:16 PaulGeffert  
C source code filec T1t1t_HT400_Njetge6_ge3b_efficiency_METbin1.C r1 manage 40.3 K 2013-11-22 - 19:35 PaulGeffert  
PDFpdf T1t1t_HT400_Njetge6_ge3b_efficiency_METbin1.pdf r1 manage 20.5 K 2013-11-22 - 19:13 PaulGeffert  
PNGpng T1t1t_HT400_Njetge6_ge3b_efficiency_METbin1.png r1 manage 46.5 K 2013-11-22 - 19:16 PaulGeffert  
C source code filec T1t1t_HT500_Njetge6_2b_efficiency_METbin1.C r1 manage 39.9 K 2013-11-22 - 19:36 PaulGeffert  
PDFpdf T1t1t_HT500_Njetge6_2b_efficiency_METbin1.pdf r1 manage 20.5 K 2013-11-22 - 19:16 PaulGeffert  
PNGpng T1t1t_HT500_Njetge6_2b_efficiency_METbin1.png r1 manage 47.2 K 2013-11-22 - 19:18 PaulGeffert  
C source code filec T1t1t_HT500_Njetge6_2b_efficiency_METbin2.C r1 manage 40.1 K 2013-11-22 - 19:36 PaulGeffert  
PDFpdf T1t1t_HT500_Njetge6_2b_efficiency_METbin2.pdf r1 manage 20.4 K 2013-11-22 - 19:16 PaulGeffert  
PNGpng T1t1t_HT500_Njetge6_2b_efficiency_METbin2.png r1 manage 46.6 K 2013-11-22 - 19:18 PaulGeffert  
C source code filec T1t1t_HT500_Njetge6_2b_efficiency_METbin3.C r1 manage 40.2 K 2013-11-22 - 19:36 PaulGeffert  
PDFpdf T1t1t_HT500_Njetge6_2b_efficiency_METbin3.pdf r1 manage 20.4 K 2013-11-22 - 19:16 PaulGeffert  
PNGpng T1t1t_HT500_Njetge6_2b_efficiency_METbin3.png r1 manage 47.6 K 2013-11-22 - 19:18 PaulGeffert  
C source code filec T1t1t_HT500_Njetge6_ge3b_efficiency_METbin1.C r1 manage 39.9 K 2013-11-22 - 19:36 PaulGeffert  
PDFpdf T1t1t_HT500_Njetge6_ge3b_efficiency_METbin1.pdf r1 manage 20.7 K 2013-11-22 - 19:15 PaulGeffert  
PNGpng T1t1t_HT500_Njetge6_ge3b_efficiency_METbin1.png r1 manage 46.9 K 2013-11-22 - 19:17 PaulGeffert  
C source code filec T1t1t_HT500_Njetge6_ge3b_efficiency_METbin2.C r1 manage 40.0 K 2013-11-22 - 19:36 PaulGeffert  
PDFpdf T1t1t_HT500_Njetge6_ge3b_efficiency_METbin2.pdf r1 manage 20.5 K 2013-11-22 - 19:15 PaulGeffert  
PNGpng T1t1t_HT500_Njetge6_ge3b_efficiency_METbin2.png r1 manage 47.1 K 2013-11-22 - 19:17 PaulGeffert  
C source code filec T1t1t_HT500_Njetge6_ge3b_efficiency_METbin3.C r1 manage 40.2 K 2013-11-22 - 19:36 PaulGeffert  
PDFpdf T1t1t_HT500_Njetge6_ge3b_efficiency_METbin3.pdf r1 manage 20.5 K 2013-11-22 - 19:15 PaulGeffert  
PNGpng T1t1t_HT500_Njetge6_ge3b_efficiency_METbin3.png r1 manage 47.8 K 2013-11-22 - 19:17 PaulGeffert  
C source code filec T1t1t_HT750_Njetge6_2b_efficiency_METbin1.C r1 manage 40.0 K 2013-11-22 - 19:36 PaulGeffert  
PDFpdf T1t1t_HT750_Njetge6_2b_efficiency_METbin1.pdf r1 manage 20.4 K 2013-11-22 - 19:15 PaulGeffert  
PNGpng T1t1t_HT750_Njetge6_2b_efficiency_METbin1.png r1 manage 46.9 K 2013-11-22 - 19:18 PaulGeffert  
C source code filec T1t1t_HT750_Njetge6_2b_efficiency_METbin2.C r1 manage 40.3 K 2013-11-22 - 19:36 PaulGeffert  
PDFpdf T1t1t_HT750_Njetge6_2b_efficiency_METbin2.pdf r1 manage 20.3 K 2013-11-22 - 19:15 PaulGeffert  
PNGpng T1t1t_HT750_Njetge6_2b_efficiency_METbin2.png r1 manage 46.1 K 2013-11-22 - 19:18 PaulGeffert  
C source code filec T1t1t_HT750_Njetge6_2b_efficiency_METbin3.C r1 manage 40.2 K 2013-11-22 - 19:36 PaulGeffert  
PDFpdf T1t1t_HT750_Njetge6_2b_efficiency_METbin3.pdf r1 manage 20.4 K 2013-11-22 - 19:15 PaulGeffert  
PNGpng T1t1t_HT750_Njetge6_2b_efficiency_METbin3.png r1 manage 47.5 K 2013-11-22 - 19:18 PaulGeffert  
C source code filec T1t1t_HT750_Njetge6_ge3b_efficiency_METbin0.C r1 manage 40.0 K 2013-11-22 - 19:35 PaulGeffert  
PDFpdf T1t1t_HT750_Njetge6_ge3b_efficiency_METbin0.pdf r1 manage 20.9 K 2013-11-22 - 19:13 PaulGeffert  
PNGpng T1t1t_HT750_Njetge6_ge3b_efficiency_METbin0.png r1 manage 47.1 K 2013-11-22 - 19:16 PaulGeffert  
C source code filec T1t1t_HT750_Njetge6_ge3b_efficiency_METbin1.C r1 manage 40.0 K 2013-11-22 - 20:02 PaulGeffert  
PDFpdf T1t1t_HT750_Njetge6_ge3b_efficiency_METbin1.pdf r1 manage 20.6 K 2013-11-22 - 19:13 PaulGeffert  
PNGpng T1t1t_HT750_Njetge6_ge3b_efficiency_METbin1.png r1 manage 47.0 K 2013-11-22 - 19:17 PaulGeffert  
C source code filec T1t1t_HT750_Njetge6_ge3b_efficiency_METbin2.C r1 manage 40.1 K 2013-11-22 - 19:35 PaulGeffert  
PDFpdf T1t1t_HT750_Njetge6_ge3b_efficiency_METbin2.pdf r1 manage 20.5 K 2013-11-22 - 19:13 PaulGeffert  
PNGpng T1t1t_HT750_Njetge6_ge3b_efficiency_METbin2.png r1 manage 47.0 K 2013-11-22 - 19:17 PaulGeffert  
C source code filec T1t1t_HT750_Njetge6_ge3b_efficiency_METbin3.C r1 manage 40.2 K 2013-11-22 - 19:35 PaulGeffert  
PDFpdf T1t1t_HT750_Njetge6_ge3b_efficiency_METbin3.pdf r1 manage 20.5 K 2013-11-22 - 19:13 PaulGeffert  
PNGpng T1t1t_HT750_Njetge6_ge3b_efficiency_METbin3.png r1 manage 47.8 K 2013-11-22 - 19:17 PaulGeffert  
PDFpdf T1ttttRA4MTXSEC.pdf r1 manage 29.3 K 2013-11-27 - 09:53 WolfgangAdam  
PNGpng T1ttttRA4MTXSEC.png r1 manage 129.2 K 2013-11-27 - 09:53 WolfgangAdam  
C source code filec T1tttt_HT1000_Njetge6_2b_efficiency_METbin1.C r1 manage 100.6 K 2013-11-22 - 20:00 PaulGeffert  
PDFpdf T1tttt_HT1000_Njetge6_2b_efficiency_METbin1.pdf r1 manage 24.9 K 2013-11-22 - 19:20 PaulGeffert  
PNGpng T1tttt_HT1000_Njetge6_2b_efficiency_METbin1.png r1 manage 49.6 K 2013-11-22 - 19:23 PaulGeffert  
C source code filec T1tttt_HT1000_Njetge6_2b_efficiency_METbin2.C r1 manage 100.9 K 2013-11-22 - 19:38 PaulGeffert  
PDFpdf T1tttt_HT1000_Njetge6_2b_efficiency_METbin2.pdf r1 manage 24.8 K 2013-11-22 - 19:20 PaulGeffert  
PNGpng T1tttt_HT1000_Njetge6_2b_efficiency_METbin2.png r1 manage 49.5 K 2013-11-22 - 19:23 PaulGeffert  
C source code filec T1tttt_HT1000_Njetge6_2b_efficiency_METbin3.C r1 manage 100.4 K 2013-11-22 - 19:38 PaulGeffert  
PDFpdf T1tttt_HT1000_Njetge6_2b_efficiency_METbin3.pdf r1 manage 25.3 K 2013-11-22 - 19:20 PaulGeffert  
PNGpng T1tttt_HT1000_Njetge6_2b_efficiency_METbin3.png r1 manage 51.3 K 2013-11-22 - 19:23 PaulGeffert  
C source code filec T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin1.C r1 manage 91.0 K 2013-04-02 - 11:46 PaulGeffert  
PDFpdf T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin1.pdf r1 manage 26.0 K 2013-03-07 - 07:03 DavidStuart T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin1.pdf
PNGpng T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin1.png r1 manage 113.5 K 2013-03-07 - 07:04 DavidStuart T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin1.png
C source code filec T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin2.C r1 manage 91.3 K 2013-04-02 - 11:46 PaulGeffert  
PDFpdf T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin2.pdf r1 manage 25.9 K 2013-03-07 - 07:04 DavidStuart T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin2.pdf
PNGpng T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin2.png r1 manage 113.3 K 2013-03-07 - 07:04 DavidStuart T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin2.png
C source code filec T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin3.C r1 manage 91.3 K 2013-04-02 - 11:46 PaulGeffert  
PDFpdf T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin3.pdf r1 manage 25.9 K 2013-03-07 - 07:05 DavidStuart T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin3.pdf
PNGpng T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin3.png r1 manage 109.7 K 2013-03-07 - 07:05 DavidStuart T1tttt_HT1000_Njetge6_ge2b_efficiency_METbin3.png
C source code filec T1tttt_HT1000_Njetge6_ge3b_efficiency_METbin1.C r1 manage 100.1 K 2013-11-22 - 19:37 PaulGeffert  
PDFpdf T1tttt_HT1000_Njetge6_ge3b_efficiency_METbin1.pdf r1 manage 25.4 K 2013-11-22 - 19:19 PaulGeffert  
PNGpng T1tttt_HT1000_Njetge6_ge3b_efficiency_METbin1.png r1 manage 50.8 K 2013-11-22 - 19:22 PaulGeffert  
C source code filec T1tttt_HT1000_Njetge6_ge3b_efficiency_METbin2.C r1 manage 100.5 K 2013-11-22 - 19:37 PaulGeffert  
PDFpdf T1tttt_HT1000_Njetge6_ge3b_efficiency_METbin2.pdf r1 manage 25.1 K 2013-11-22 - 19:19 PaulGeffert  
PNGpng T1tttt_HT1000_Njetge6_ge3b_efficiency_METbin2.png r1 manage 50.3 K 2013-11-22 - 19:22 PaulGeffert  
C source code filec T1tttt_HT1000_Njetge6_ge3b_efficiency_METbin3.C r1 manage 100.4 K 2013-11-22 - 19:37 PaulGeffert  
PDFpdf T1tttt_HT1000_Njetge6_ge3b_efficiency_METbin3.pdf r1 manage 25.5 K 2013-11-22 - 19:19 PaulGeffert  
PNGpng T1tttt_HT1000_Njetge6_ge3b_efficiency_METbin3.png r1 manage 51.6 K 2013-11-22 - 19:22 PaulGeffert  
C source code filec T1tttt_HT400_Njetge6_ge3b_efficiency_METbin0.C r1 manage 99.6 K 2013-11-22 - 19:37 PaulGeffert  
PDFpdf T1tttt_HT400_Njetge6_ge3b_efficiency_METbin0.pdf r1 manage 25.7 K 2013-11-22 - 19:19 PaulGeffert  
PNGpng T1tttt_HT400_Njetge6_ge3b_efficiency_METbin0.png r1 manage 52.7 K 2013-11-22 - 19:21 PaulGeffert  
C source code filec T1tttt_HT400_Njetge6_ge3b_efficiency_METbin1.C r1 manage 100.1 K 2013-11-22 - 19:37 PaulGeffert  
PDFpdf T1tttt_HT400_Njetge6_ge3b_efficiency_METbin1.pdf r1 manage 25.3 K 2013-11-22 - 19:19 PaulGeffert  
PNGpng T1tttt_HT400_Njetge6_ge3b_efficiency_METbin1.png r1 manage 51.5 K 2013-11-22 - 19:21 PaulGeffert  
C source code filec T1tttt_HT500_Njetge6_2b_efficiency_METbin1.C r1 manage 98.6 K 2013-11-22 - 19:39 PaulGeffert  
PDFpdf T1tttt_HT500_Njetge6_2b_efficiency_METbin1.pdf r1 manage 25.8 K 2013-11-22 - 19:21 PaulGeffert  
PNGpng T1tttt_HT500_Njetge6_2b_efficiency_METbin1.png r1 manage 52.9 K 2013-11-22 - 19:23 PaulGeffert  
C source code filec T1tttt_HT500_Njetge6_2b_efficiency_METbin2.C r1 manage 99.4 K 2013-11-22 - 19:39 PaulGeffert  
PDFpdf T1tttt_HT500_Njetge6_2b_efficiency_METbin2.pdf r1 manage 25.3 K 2013-11-22 - 19:21 PaulGeffert  
PNGpng T1tttt_HT500_Njetge6_2b_efficiency_METbin2.png r1 manage 51.9 K 2013-11-22 - 19:23 PaulGeffert  
C source code filec T1tttt_HT500_Njetge6_2b_efficiency_METbin3.C r1 manage 99.9 K 2013-11-22 - 19:39 PaulGeffert  
PDFpdf T1tttt_HT500_Njetge6_2b_efficiency_METbin3.pdf r1 manage 25.6 K 2013-11-22 - 19:21 PaulGeffert  
PNGpng T1tttt_HT500_Njetge6_2b_efficiency_METbin3.png r1 manage 52.2 K 2013-11-22 - 19:23 PaulGeffert  
C source code filec T1tttt_HT500_Njetge6_ge2b_efficiency_METbin1.C r1 manage 90.1 K 2013-04-02 - 11:46 PaulGeffert  
PDFpdf T1tttt_HT500_Njetge6_ge2b_efficiency_METbin1.pdf r1 manage 26.0 K 2013-03-07 - 06:59 DavidStuart T1tttt_HT500_Njetge6_ge2b_efficiency_METbin1.pdf
PNGpng T1tttt_HT500_Njetge6_ge2b_efficiency_METbin1.png r1 manage 119.1 K 2013-03-07 - 06:59 DavidStuart T1tttt_HT500_Njetge6_ge2b_efficiency_METbin1.png
C source code filec T1tttt_HT500_Njetge6_ge2b_efficiency_METbin2.C r1 manage 90.6 K 2013-04-02 - 11:46 PaulGeffert  
PDFpdf T1tttt_HT500_Njetge6_ge2b_efficiency_METbin2.pdf r1 manage 26.0 K 2013-03-07 - 07:00 DavidStuart T1tttt_HT500_Njetge6_ge2b_efficiency_METbin2.pdf
PNGpng T1tttt_HT500_Njetge6_ge2b_efficiency_METbin2.png r1 manage 116.3 K 2013-03-07 - 07:00 DavidStuart T1tttt_HT500_Njetge6_ge2b_efficiency_METbin2.png
C source code filec T1tttt_HT500_Njetge6_ge2b_efficiency_METbin3.C r1 manage 90.9 K 2013-04-02 - 11:46 PaulGeffert  
PDFpdf T1tttt_HT500_Njetge6_ge2b_efficiency_METbin3.pdf r1 manage 26.0 K 2013-03-07 - 07:00 DavidStuart T1tttt_HT500_Njetge6_ge2b_efficiency_METbin3.pdf
PNGpng T1tttt_HT500_Njetge6_ge2b_efficiency_METbin3.png r1 manage 110.8 K 2013-03-07 - 07:01 DavidStuart T1tttt_HT500_Njetge6_ge2b_efficiency_METbin3.png
C source code filec T1tttt_HT500_Njetge6_ge3b_efficiency_METbin1.C r1 manage 98.9 K 2013-11-22 - 19:38 PaulGeffert  
PDFpdf T1tttt_HT500_Njetge6_ge3b_efficiency_METbin1.pdf r1 manage 26.2 K 2013-11-22 - 19:20 PaulGeffert  
PNGpng T1tttt_HT500_Njetge6_ge3b_efficiency_METbin1.png r1 manage 53.1 K 2013-11-22 - 19:22 PaulGeffert  
C source code filec T1tttt_HT500_Njetge6_ge3b_efficiency_METbin2.C r1 manage 99.5 K 2013-11-22 - 19:38 PaulGeffert  
PDFpdf T1tttt_HT500_Njetge6_ge3b_efficiency_METbin2.pdf r1 manage 25.6 K 2013-11-22 - 19:20 PaulGeffert  
PNGpng T1tttt_HT500_Njetge6_ge3b_efficiency_METbin2.png r1 manage 52.1 K 2013-11-22 - 19:22 PaulGeffert  
C source code filec T1tttt_HT500_Njetge6_ge3b_efficiency_METbin3.C r1 manage 100.0 K 2013-11-22 - 19:38 PaulGeffert  
PDFpdf T1tttt_HT500_Njetge6_ge3b_efficiency_METbin3.pdf r1 manage 25.9 K 2013-11-22 - 19:20 PaulGeffert  
PNGpng T1tttt_HT500_Njetge6_ge3b_efficiency_METbin3.png r1 manage 52.4 K 2013-11-22 - 19:22 PaulGeffert  
C source code filec T1tttt_HT750_Njetge6_2b_efficiency_METbin1.C r1 manage 99.2 K 2013-11-22 - 19:38 PaulGeffert  
PDFpdf T1tttt_HT750_Njetge6_2b_efficiency_METbin1.pdf r1 manage 25.7 K 2013-11-22 - 19:20 PaulGeffert  
PNGpng T1tttt_HT750_Njetge6_2b_efficiency_METbin1.png r1 manage 52.2 K 2013-11-22 - 19:23 PaulGeffert  
C source code filec T1tttt_HT750_Njetge6_2b_efficiency_METbin2.C r1 manage 99.7 K 2013-11-22 - 19:38 PaulGeffert  
PDFpdf T1tttt_HT750_Njetge6_2b_efficiency_METbin2.pdf r1 manage 25.2 K 2013-11-22 - 19:20 PaulGeffert  
PNGpng T1tttt_HT750_Njetge6_2b_efficiency_METbin2.png r1 manage 51.4 K 2013-11-22 - 19:23 PaulGeffert  
C source code filec T1tttt_HT750_Njetge6_2b_efficiency_METbin3.C r1 manage 99.9 K 2013-11-22 - 19:38 PaulGeffert  
PDFpdf T1tttt_HT750_Njetge6_2b_efficiency_METbin3.pdf r1 manage 25.6 K 2013-11-22 - 19:20 PaulGeffert  
PNGpng T1tttt_HT750_Njetge6_2b_efficiency_METbin3.png r1 manage 52.2 K 2013-11-22 - 19:23 PaulGeffert  
C source code filec T1tttt_HT750_Njetge6_ge2b_efficiency_METbin1.C r1 manage 90.4 K 2013-04-02 - 11:46 PaulGeffert  
PDFpdf T1tttt_HT750_Njetge6_ge2b_efficiency_METbin1.pdf r1 manage 26.2 K 2013-03-07 - 07:01 DavidStuart T1tttt_HT750_Njetge6_ge2b_efficiency_METbin1.pdf
PNGpng T1tttt_HT750_Njetge6_ge2b_efficiency_METbin1.png r1 manage 116.7 K 2013-03-07 - 07:01 DavidStuart T1tttt_HT750_Njetge6_ge2b_efficiency_METbin1.png
C source code filec T1tttt_HT750_Njetge6_ge2b_efficiency_METbin2.C r1 manage 90.8 K 2013-04-02 - 11:46 PaulGeffert  
PDFpdf T1tttt_HT750_Njetge6_ge2b_efficiency_METbin2.pdf r1 manage 26.1 K 2013-03-07 - 07:02 DavidStuart T1tttt_HT750_Njetge6_ge2b_efficiency_METbin2.pdf
PNGpng T1tttt_HT750_Njetge6_ge2b_efficiency_METbin2.png r1 manage 116.1 K 2013-03-07 - 07:02 DavidStuart T1tttt_HT750_Njetge6_ge2b_efficiency_METbin2.png
C source code filec T1tttt_HT750_Njetge6_ge2b_efficiency_METbin3.C r1 manage 91.0 K 2013-04-02 - 11:46 PaulGeffert  
PDFpdf T1tttt_HT750_Njetge6_ge2b_efficiency_METbin3.pdf r1 manage 26.0 K 2013-03-07 - 07:03 DavidStuart T1tttt_HT750_Njetge6_ge2b_efficiency_METbin3.pdf
PNGpng T1tttt_HT750_Njetge6_ge2b_efficiency_METbin3.png r1 manage 111.1 K 2013-03-07 - 07:03 DavidStuart T1tttt_HT750_Njetge6_ge2b_efficiency_METbin3.png
C source code filec T1tttt_HT750_Njetge6_ge3b_efficiency_METbin0.C r1 manage 99.0 K 2013-11-22 - 19:37 PaulGeffert  
PDFpdf T1tttt_HT750_Njetge6_ge3b_efficiency_METbin0.pdf r1 manage 26.0 K 2013-11-22 - 19:19 PaulGeffert  
PNGpng T1tttt_HT750_Njetge6_ge3b_efficiency_METbin0.png r1 manage 52.7 K 2013-11-22 - 19:21 PaulGeffert  
C source code filec T1tttt_HT750_Njetge6_ge3b_efficiency_METbin1.C r1 manage 99.3 K 2013-11-22 - 19:37 PaulGeffert  
PDFpdf T1tttt_HT750_Njetge6_ge3b_efficiency_METbin1.pdf r1 manage 26.0 K 2013-11-22 - 19:19 PaulGeffert  
PNGpng T1tttt_HT750_Njetge6_ge3b_efficiency_METbin1.png r1 manage 52.5 K 2013-11-22 - 19:22 PaulGeffert  
C source code filec T1tttt_HT750_Njetge6_ge3b_efficiency_METbin2.C r1 manage 99.8 K 2013-11-22 - 19:37 PaulGeffert  
PDFpdf T1tttt_HT750_Njetge6_ge3b_efficiency_METbin2.pdf r1 manage 25.5 K 2013-11-22 - 19:19 PaulGeffert  
PNGpng T1tttt_HT750_Njetge6_ge3b_efficiency_METbin2.png r1 manage 51.8 K 2013-11-22 - 19:22 PaulGeffert  
C source code filec T1tttt_HT750_Njetge6_ge3b_efficiency_METbin3.C r1 manage 100.1 K 2013-11-22 - 19:37 PaulGeffert  
PDFpdf T1tttt_HT750_Njetge6_ge3b_efficiency_METbin3.pdf r1 manage 25.8 K 2013-11-22 - 19:19 PaulGeffert  
PNGpng T1tttt_HT750_Njetge6_ge3b_efficiency_METbin3.png r1 manage 52.4 K 2013-11-22 - 19:22 PaulGeffert  
PDFpdf T5ttttRA4MTXSEC.pdf r1 manage 25.6 K 2013-11-27 - 09:53 WolfgangAdam  
PNGpng T5ttttRA4MTXSEC.png r1 manage 120.6 K 2013-11-27 - 09:53 WolfgangAdam  
C source code filec T5tttt_HT1000_Njetge6_2b_efficiency_METbin1.C r1 manage 68.9 K 2013-11-22 - 19:42 PaulGeffert  
PDFpdf T5tttt_HT1000_Njetge6_2b_efficiency_METbin1.pdf r1 manage 22.8 K 2013-11-22 - 19:25 PaulGeffert  
PNGpng T5tttt_HT1000_Njetge6_2b_efficiency_METbin1.png r1 manage 48.5 K 2013-11-22 - 19:27 PaulGeffert  
C source code filec T5tttt_HT1000_Njetge6_2b_efficiency_METbin2.C r1 manage 69.3 K 2013-11-22 - 19:42 PaulGeffert  
PDFpdf T5tttt_HT1000_Njetge6_2b_efficiency_METbin2.pdf r1 manage 22.5 K 2013-11-22 - 19:25 PaulGeffert  
PNGpng T5tttt_HT1000_Njetge6_2b_efficiency_METbin2.png r1 manage 48.0 K 2013-11-22 - 19:27 PaulGeffert  
C source code filec T5tttt_HT1000_Njetge6_2b_efficiency_METbin3.C r1 manage 68.5 K 2013-11-22 - 19:42 PaulGeffert  
PDFpdf T5tttt_HT1000_Njetge6_2b_efficiency_METbin3.pdf r1 manage 22.7 K 2013-11-22 - 19:25 PaulGeffert  
PNGpng T5tttt_HT1000_Njetge6_2b_efficiency_METbin3.png r1 manage 47.2 K 2013-11-22 - 19:27 PaulGeffert  
C source code filec T5tttt_HT1000_Njetge6_ge3b_efficiency_METbin1.C r1 manage 68.5 K 2013-11-22 - 19:41 PaulGeffert  
PDFpdf T5tttt_HT1000_Njetge6_ge3b_efficiency_METbin1.pdf r1 manage 23.1 K 2013-11-22 - 19:24 PaulGeffert  
PNGpng T5tttt_HT1000_Njetge6_ge3b_efficiency_METbin1.png r1 manage 49.6 K 2013-11-22 - 19:26 PaulGeffert  
C source code filec T5tttt_HT1000_Njetge6_ge3b_efficiency_METbin2.C r1 manage 68.7 K 2013-11-22 - 19:41 PaulGeffert  
PDFpdf T5tttt_HT1000_Njetge6_ge3b_efficiency_METbin2.pdf r1 manage 22.6 K 2013-11-22 - 19:24 PaulGeffert  
PNGpng T5tttt_HT1000_Njetge6_ge3b_efficiency_METbin2.png r1 manage 49.1 K 2013-11-22 - 19:26 PaulGeffert  
C source code filec T5tttt_HT1000_Njetge6_ge3b_efficiency_METbin3.C r1 manage 68.4 K 2013-11-22 - 19:41 PaulGeffert  
PDFpdf T5tttt_HT1000_Njetge6_ge3b_efficiency_METbin3.pdf r1 manage 22.9 K 2013-11-22 - 19:24 PaulGeffert  
PNGpng T5tttt_HT1000_Njetge6_ge3b_efficiency_METbin3.png r1 manage 47.8 K 2013-11-22 - 19:26 PaulGeffert  
C source code filec T5tttt_HT400_Njetge6_ge3b_efficiency_METbin0.C r1 manage 70.1 K 2013-11-22 - 19:41 PaulGeffert  
PDFpdf T5tttt_HT400_Njetge6_ge3b_efficiency_METbin0.pdf r1 manage 22.0 K 2013-11-22 - 19:24 PaulGeffert  
PNGpng T5tttt_HT400_Njetge6_ge3b_efficiency_METbin0.png r1 manage 47.9 K 2013-11-22 - 19:25 PaulGeffert  
C source code filec T5tttt_HT400_Njetge6_ge3b_efficiency_METbin1.C r1 manage 69.6 K 2013-11-22 - 19:41 PaulGeffert  
PDFpdf T5tttt_HT400_Njetge6_ge3b_efficiency_METbin1.pdf r1 manage 22.6 K 2013-11-22 - 19:24 PaulGeffert  
PNGpng T5tttt_HT400_Njetge6_ge3b_efficiency_METbin1.png r1 manage 47.6 K 2013-11-22 - 19:25 PaulGeffert  
C source code filec T5tttt_HT500_Njetge6_2b_efficiency_METbin1.C r1 manage 68.2 K 2013-11-22 - 19:43 PaulGeffert  
PDFpdf T5tttt_HT500_Njetge6_2b_efficiency_METbin1.pdf r1 manage 22.7 K 2013-11-22 - 19:25 PaulGeffert  
PNGpng T5tttt_HT500_Njetge6_2b_efficiency_METbin1.png r1 manage 49.7 K 2013-11-22 - 19:27 PaulGeffert  
C source code filec T5tttt_HT500_Njetge6_2b_efficiency_METbin2.C r1 manage 68.3 K 2013-11-22 - 19:43 PaulGeffert  
PDFpdf T5tttt_HT500_Njetge6_2b_efficiency_METbin2.pdf r1 manage 22.6 K 2013-11-22 - 19:25 PaulGeffert  
PNGpng T5tttt_HT500_Njetge6_2b_efficiency_METbin2.png r1 manage 49.2 K 2013-11-22 - 19:27 PaulGeffert  
C source code filec T5tttt_HT500_Njetge6_2b_efficiency_METbin3.C r1 manage 68.3 K 2013-11-22 - 19:43 PaulGeffert  
PDFpdf T5tttt_HT500_Njetge6_2b_efficiency_METbin3.pdf r1 manage 22.9 K 2013-11-22 - 19:25 PaulGeffert  
PNGpng T5tttt_HT500_Njetge6_2b_efficiency_METbin3.png r1 manage 47.6 K 2013-11-22 - 19:27 PaulGeffert  
C source code filec T5tttt_HT500_Njetge6_ge3b_efficiency_METbin1.C r1 manage 68.1 K 2013-11-22 - 19:42 PaulGeffert  
PDFpdf T5tttt_HT500_Njetge6_ge3b_efficiency_METbin1.pdf r1 manage 23.2 K 2013-11-22 - 19:25 PaulGeffert  
PNGpng T5tttt_HT500_Njetge6_ge3b_efficiency_METbin1.png r1 manage 49.8 K 2013-11-22 - 19:26 PaulGeffert  
C source code filec T5tttt_HT500_Njetge6_ge3b_efficiency_METbin2.C r1 manage 68.2 K 2013-11-22 - 19:42 PaulGeffert  
PDFpdf T5tttt_HT500_Njetge6_ge3b_efficiency_METbin2.pdf r1 manage 22.9 K 2013-11-22 - 19:25 PaulGeffert  
PNGpng T5tttt_HT500_Njetge6_ge3b_efficiency_METbin2.png r1 manage 49.8 K 2013-11-22 - 19:26 PaulGeffert  
C source code filec T5tttt_HT500_Njetge6_ge3b_efficiency_METbin3.C r1 manage 68.2 K 2013-11-22 - 19:42 PaulGeffert  
PDFpdf T5tttt_HT500_Njetge6_ge3b_efficiency_METbin3.pdf r1 manage 23.1 K 2013-11-22 - 19:25 PaulGeffert  
PNGpng T5tttt_HT500_Njetge6_ge3b_efficiency_METbin3.png r1 manage 48.1 K 2013-11-22 - 19:26 PaulGeffert  
C source code filec T5tttt_HT750_Njetge6_2b_efficiency_METbin1.C r1 manage 68.4 K 2013-11-22 - 19:42 PaulGeffert  
PDFpdf T5tttt_HT750_Njetge6_2b_efficiency_METbin1.pdf r1 manage 22.8 K 2013-11-22 - 19:25 PaulGeffert  
PNGpng T5tttt_HT750_Njetge6_2b_efficiency_METbin1.png r1 manage 49.5 K 2013-11-22 - 19:27 PaulGeffert  
C source code filec T5tttt_HT750_Njetge6_2b_efficiency_METbin2.C r1 manage 68.6 K 2013-11-22 - 19:42 PaulGeffert  
PDFpdf T5tttt_HT750_Njetge6_2b_efficiency_METbin2.pdf r1 manage 22.6 K 2013-11-22 - 19:25 PaulGeffert  
PNGpng T5tttt_HT750_Njetge6_2b_efficiency_METbin2.png r1 manage 49.0 K 2013-11-22 - 19:27 PaulGeffert  
C source code filec T5tttt_HT750_Njetge6_2b_efficiency_METbin3.C r1 manage 68.3 K 2013-11-22 - 19:42 PaulGeffert  
PDFpdf T5tttt_HT750_Njetge6_2b_efficiency_METbin3.pdf r1 manage 22.9 K 2013-11-22 - 19:25 PaulGeffert  
PNGpng T5tttt_HT750_Njetge6_2b_efficiency_METbin3.png r1 manage 47.7 K 2013-11-22 - 19:27 PaulGeffert  
C source code filec T5tttt_HT750_Njetge6_ge3b_efficiency_METbin0.C r1 manage 68.3 K 2013-11-22 - 19:41 PaulGeffert  
PDFpdf T5tttt_HT750_Njetge6_ge3b_efficiency_METbin0.pdf r1 manage 23.4 K 2013-11-22 - 19:24 PaulGeffert  
PNGpng T5tttt_HT750_Njetge6_ge3b_efficiency_METbin0.png r1 manage 50.0 K 2013-11-22 - 19:25 PaulGeffert  
C source code filec T5tttt_HT750_Njetge6_ge3b_efficiency_METbin1.C r1 manage 68.2 K 2013-11-22 - 19:41 PaulGeffert  
PDFpdf T5tttt_HT750_Njetge6_ge3b_efficiency_METbin1.pdf r1 manage 23.2 K 2013-11-22 - 19:24 PaulGeffert  
PNGpng T5tttt_HT750_Njetge6_ge3b_efficiency_METbin1.png r1 manage 50.0 K 2013-11-22 - 19:26 PaulGeffert  
C source code filec T5tttt_HT750_Njetge6_ge3b_efficiency_METbin2.C r1 manage 68.3 K 2013-11-22 - 19:41 PaulGeffert  
PDFpdf T5tttt_HT750_Njetge6_ge3b_efficiency_METbin2.pdf r1 manage 22.8 K 2013-11-22 - 19:24 PaulGeffert  
PNGpng T5tttt_HT750_Njetge6_ge3b_efficiency_METbin2.png r1 manage 49.9 K 2013-11-22 - 19:26 PaulGeffert  
C source code filec T5tttt_HT750_Njetge6_ge3b_efficiency_METbin3.C r1 manage 68.2 K 2013-11-22 - 19:41 PaulGeffert  
PDFpdf T5tttt_HT750_Njetge6_ge3b_efficiency_METbin3.pdf r1 manage 23.1 K 2013-11-22 - 19:24 PaulGeffert  
PNGpng T5tttt_HT750_Njetge6_ge3b_efficiency_METbin3.png r1 manage 48.2 K 2013-11-22 - 19:26 PaulGeffert  
PDFpdf Table10.pdf r1 manage 117.2 K 2013-03-07 - 07:06 DavidStuart  
PNGpng Table10.png r1 manage 131.5 K 2013-03-07 - 07:06 DavidStuart  
PDFpdf Table11.pdf r1 manage 91.0 K 2013-03-07 - 07:06 DavidStuart  
PNGpng Table11.png r1 manage 99.4 K 2013-03-07 - 07:06 DavidStuart  
PDFpdf Table12.pdf r1 manage 79.2 K 2013-03-07 - 07:07 DavidStuart  
PNGpng Table12.png r1 manage 101.0 K 2013-03-07 - 07:07 DavidStuart  
PDFpdf Table13.pdf r1 manage 66.0 K 2013-03-07 - 07:07 DavidStuart  
PNGpng Table13.png r1 manage 68.2 K 2013-03-07 - 07:07 DavidStuart  
PDFpdf Table7.pdf r1 manage 96.2 K 2013-03-07 - 07:06 DavidStuart  
PNGpng Table7.png r1 manage 105.5 K 2013-03-07 - 07:06 DavidStuart  
PDFpdf Table8.pdf r1 manage 102.6 K 2013-03-07 - 07:06 DavidStuart  
PNGpng Table8.png r1 manage 112.1 K 2013-03-07 - 07:06 DavidStuart  
PDFpdf Table9.pdf r1 manage 71.3 K 2013-03-07 - 07:06 DavidStuart  
PNGpng Table9.png r1 manage 73.2 K 2013-03-07 - 07:06 DavidStuart  
PDFpdf TauDataMCcompare_LepTauHad_TypeIMET_EMu_HT1000_Njetge6_2b_LepTauHad.pdf r1 manage 14.9 K 2013-11-22 - 19:05 PaulGeffert  
PNGpng TauDataMCcompare_LepTauHad_TypeIMET_EMu_HT1000_Njetge6_2b_LepTauHad.png r1 manage 78.5 K 2013-11-22 - 19:06 PaulGeffert  
PDFpdf TauDataMCcompare_LepTauHad_TypeIMET_EMu_HT1000_Njetge6_ge2b_LepTauHad.pdf r1 manage 14.9 K 2013-03-07 - 07:08 DavidStuart  
PNGpng TauDataMCcompare_LepTauHad_TypeIMET_EMu_HT1000_Njetge6_ge2b_LepTauHad.png r1 manage 80.7 K 2013-03-07 - 07:08 DavidStuart  
PDFpdf TauDataMCcompare_LepTauHad_TypeIMET_EMu_HT500_Njetge6_2b_LepTauHad.pdf r1 manage 15.1 K 2013-11-22 - 19:05 PaulGeffert  
PNGpng TauDataMCcompare_LepTauHad_TypeIMET_EMu_HT500_Njetge6_2b_LepTauHad.png r1 manage 79.8 K 2013-11-22 - 19:06 PaulGeffert  
PDFpdf TauDataMCcompare_LepTauHad_TypeIMET_EMu_HT500_Njetge6_ge2b_LepTauHad.pdf r1 manage 15.1 K 2013-03-07 - 07:08 DavidStuart  
PNGpng TauDataMCcompare_LepTauHad_TypeIMET_EMu_HT500_Njetge6_ge2b_LepTauHad.png r1 manage 82.0 K 2013-03-07 - 07:08 DavidStuart  
PDFpdf TauDataMCcompare_LepTauHad_TypeIMET_EMu_HT750_Njetge6_2b_LepTauHad.pdf r1 manage 15.0 K 2013-11-22 - 19:05 PaulGeffert  
PNGpng TauDataMCcompare_LepTauHad_TypeIMET_EMu_HT750_Njetge6_2b_LepTauHad.png r1 manage 80.4 K 2013-11-22 - 19:06 PaulGeffert  
PDFpdf TauDataMCcompare_LepTauHad_TypeIMET_EMu_HT750_Njetge6_ge2b_LepTauHad.pdf r1 manage 15.1 K 2013-03-07 - 07:08 DavidStuart  
PNGpng TauDataMCcompare_LepTauHad_TypeIMET_EMu_HT750_Njetge6_ge2b_LepTauHad.png r1 manage 82.2 K 2013-03-07 - 07:08 DavidStuart  
PDFpdf TauDataMCcompare_LepTauLep_TypeIMET_EMu_HT1000_Njetge6_2b_LepTauLep.pdf r1 manage 14.6 K 2013-11-22 - 19:05 PaulGeffert  
PNGpng TauDataMCcompare_LepTauLep_TypeIMET_EMu_HT1000_Njetge6_2b_LepTauLep.png r1 manage 76.8 K 2013-11-22 - 19:06 PaulGeffert  
PDFpdf TauDataMCcompare_LepTauLep_TypeIMET_EMu_HT1000_Njetge6_ge2b_LepTauLep.pdf r1 manage 14.8 K 2013-03-07 - 07:10 DavidStuart  
PNGpng TauDataMCcompare_LepTauLep_TypeIMET_EMu_HT1000_Njetge6_ge2b_LepTauLep.png r1 manage 79.8 K 2013-03-07 - 07:10 DavidStuart  
PDFpdf TauDataMCcompare_LepTauLep_TypeIMET_EMu_HT500_Njetge6_2b_LepTauLep.pdf r1 manage 14.8 K 2013-11-22 - 19:05 PaulGeffert  
PNGpng TauDataMCcompare_LepTauLep_TypeIMET_EMu_HT500_Njetge6_2b_LepTauLep.png r1 manage 78.1 K 2013-11-22 - 19:06 PaulGeffert  
PDFpdf TauDataMCcompare_LepTauLep_TypeIMET_EMu_HT500_Njetge6_ge2b_LepTauLep.pdf r1 manage 14.9 K 2013-03-07 - 07:09 DavidStuart  
PNGpng TauDataMCcompare_LepTauLep_TypeIMET_EMu_HT500_Njetge6_ge2b_LepTauLep.png r1 manage 80.5 K 2013-03-07 - 07:09 DavidStuart  
PDFpdf TauDataMCcompare_LepTauLep_TypeIMET_EMu_HT750_Njetge6_2b_LepTauLep.pdf r1 manage 14.8 K 2013-11-22 - 19:05 PaulGeffert  
PNGpng TauDataMCcompare_LepTauLep_TypeIMET_EMu_HT750_Njetge6_2b_LepTauLep.png r1 manage 78.6 K 2013-11-22 - 19:06 PaulGeffert  
PDFpdf TauDataMCcompare_LepTauLep_TypeIMET_EMu_HT750_Njetge6_ge2b_LepTauLep.pdf r1 manage 14.9 K 2013-03-07 - 07:10 DavidStuart  
PNGpng TauDataMCcompare_LepTauLep_TypeIMET_EMu_HT750_Njetge6_ge2b_LepTauLep.png r1 manage 80.8 K 2013-03-07 - 07:10 DavidStuart  
PDFpdf TauDataMCcompare_SingleTau_TypeIMET_EMu_HT1000_Njetge6_2b_SingleTau.pdf r1 manage 15.2 K 2013-11-22 - 19:07 PaulGeffert  
PNGpng TauDataMCcompare_SingleTau_TypeIMET_EMu_HT1000_Njetge6_2b_SingleTau.png r1 manage 79.7 K 2013-11-22 - 19:07 PaulGeffert  
PDFpdf TauDataMCcompare_SingleTau_TypeIMET_EMu_HT1000_Njetge6_ge2b_SingleTau.pdf r1 manage 15.2 K 2013-03-07 - 07:10 DavidStuart  
PNGpng TauDataMCcompare_SingleTau_TypeIMET_EMu_HT1000_Njetge6_ge2b_SingleTau.png r1 manage 81.8 K 2013-03-07 - 07:10 DavidStuart  
PDFpdf TauDataMCcompare_SingleTau_TypeIMET_EMu_HT500_Njetge6_2b_SingleTau.pdf r1 manage 15.2 K 2013-11-22 - 19:07 PaulGeffert  
PNGpng TauDataMCcompare_SingleTau_TypeIMET_EMu_HT500_Njetge6_2b_SingleTau.png r1 manage 79.9 K 2013-11-22 - 19:07 PaulGeffert  
PDFpdf TauDataMCcompare_SingleTau_TypeIMET_EMu_HT500_Njetge6_ge2b_SingleTau.pdf r1 manage 15.2 K 2013-03-07 - 07:10 DavidStuart  
PNGpng TauDataMCcompare_SingleTau_TypeIMET_EMu_HT500_Njetge6_ge2b_SingleTau.png r1 manage 82.0 K 2013-03-07 - 07:10 DavidStuart  
PDFpdf TauDataMCcompare_SingleTau_TypeIMET_EMu_HT750_Njetge6_2b_SingleTau.pdf r1 manage 15.2 K 2013-11-22 - 19:07 PaulGeffert  
PNGpng TauDataMCcompare_SingleTau_TypeIMET_EMu_HT750_Njetge6_2b_SingleTau.png r1 manage 80.4 K 2013-11-22 - 19:07 PaulGeffert  
PDFpdf TauDataMCcompare_SingleTau_TypeIMET_EMu_HT750_Njetge6_ge2b_SingleTau.pdf r1 manage 15.2 K 2013-03-07 - 07:10 DavidStuart  
PNGpng TauDataMCcompare_SingleTau_TypeIMET_EMu_HT750_Njetge6_ge2b_SingleTau.png r1 manage 82.5 K 2013-03-07 - 07:10 DavidStuart  
PDFpdf Tau_syst-standalone.pdf r1 manage 39.2 K 2013-03-07 - 07:07 DavidStuart  
PNGpng Tau_syst-standalone.png r1 manage 24.1 K 2013-03-07 - 07:07 DavidStuart  
PDFpdf Tau_syst-standalone_Njetge6_2b.pdf r1 manage 56.7 K 2013-11-22 - 19:07 PaulGeffert  
PNGpng Tau_syst-standalone_Njetge6_2b.png r1 manage 57.7 K 2013-11-22 - 19:07 PaulGeffert  
PDFpdf c_sum_model_bt1_ht_1000.pdf r1 manage 20.1 K 2013-11-29 - 10:20 WolfgangAdam  
PNGpng c_sum_model_bt1_ht_1000.png r1 manage 15.8 K 2013-11-29 - 10:20 WolfgangAdam  
PDFpdf c_sum_model_bt1_ht_400.pdf r1 manage 21.9 K 2013-11-29 - 10:20 WolfgangAdam  
PNGpng c_sum_model_bt1_ht_400.png r1 manage 15.5 K 2013-11-29 - 10:20 WolfgangAdam  
PDFpdf c_sum_model_bt1_ht_750.pdf r1 manage 21.8 K 2013-11-29 - 10:20 WolfgangAdam  
PNGpng c_sum_model_bt1_ht_750.png r1 manage 15.6 K 2013-11-29 - 10:20 WolfgangAdam  
PDFpdf c_sum_model_bt2_ht_1000.pdf r1 manage 19.7 K 2013-11-29 - 10:21 WolfgangAdam  
PNGpng c_sum_model_bt2_ht_1000.png r1 manage 15.9 K 2013-11-29 - 10:21 WolfgangAdam  
PDFpdf c_sum_model_bt2_ht_400.pdf r1 manage 20.0 K 2013-11-29 - 10:21 WolfgangAdam  
PNGpng c_sum_model_bt2_ht_400.png r1 manage 16.0 K 2013-11-29 - 10:21 WolfgangAdam  
PDFpdf c_sum_model_bt2_ht_750.pdf r1 manage 20.0 K 2013-11-29 - 10:21 WolfgangAdam  
PNGpng c_sum_model_bt2_ht_750.png r1 manage 15.9 K 2013-11-29 - 10:21 WolfgangAdam  
PDFpdf combLimit_T1t1t_a.pdf r1 manage 26.0 K 2013-11-22 - 18:56 PaulGeffert  
PNGpng combLimit_T1t1t_a.png r1 manage 168.5 K 2013-11-22 - 18:57 PaulGeffert  
PDFpdf combLimit_T1t1t_b.pdf r1 manage 28.3 K 2013-11-22 - 18:56 PaulGeffert  
PNGpng combLimit_T1t1t_b.png r1 manage 154.5 K 2013-11-22 - 18:57 PaulGeffert  
PDFpdf combLimit_T1t1t_c.pdf r1 manage 21.7 K 2013-11-22 - 18:56 PaulGeffert  
PNGpng combLimit_T1t1t_c.png r1 manage 145.1 K 2013-11-22 - 18:57 PaulGeffert  
PDFpdf combLimit_T1tttt_a.pdf r1 manage 38.0 K 2013-11-22 - 18:56 PaulGeffert  
PNGpng combLimit_T1tttt_a.png r1 manage 183.6 K 2013-11-22 - 18:57 PaulGeffert  
PDFpdf combLimit_T1tttt_b.pdf r1 manage 51.5 K 2013-11-22 - 18:56 PaulGeffert  
PNGpng combLimit_T1tttt_b.png r1 manage 192.8 K 2013-11-22 - 18:57 PaulGeffert  
PDFpdf combLimit_T1tttt_c.pdf r1 manage 31.1 K 2013-11-22 - 18:56 PaulGeffert  
PNGpng combLimit_T1tttt_c.png r1 manage 160.7 K 2013-11-22 - 18:57 PaulGeffert  
PDFpdf combLimit_T5tttt_a.pdf r1 manage 41.0 K 2013-11-22 - 18:56 PaulGeffert  
PNGpng combLimit_T5tttt_a.png r1 manage 171.2 K 2013-11-22 - 18:57 PaulGeffert  
PDFpdf combLimit_T5tttt_b.pdf r1 manage 50.5 K 2013-11-22 - 18:56 PaulGeffert  
PNGpng combLimit_T5tttt_b.png r1 manage 168.7 K 2013-11-22 - 18:57 PaulGeffert  
PDFpdf combLimit_T5tttt_c.pdf r1 manage 33.3 K 2013-11-22 - 18:56 PaulGeffert  
PNGpng combLimit_T5tttt_c.png r1 manage 144.3 K 2013-11-22 - 18:57 PaulGeffert  
PNGpng f3_1.png r1 manage 41.7 K 2013-11-22 - 12:29 AntoniosAgapitos  
PDFpdf full_prediction_Both_HT1000_2b_SixJet_log.pdf r1 manage 17.4 K 2013-11-22 - 19:04 PaulGeffert  
PNGpng full_prediction_Both_HT1000_2b_SixJet_log.png r1 manage 24.3 K 2013-11-22 - 19:04 PaulGeffert  
PDFpdf full_prediction_Both_HT1000_2b_ThreeToFiveJet_log.pdf r1 manage 17.7 K 2013-11-22 - 19:02 PaulGeffert  
PNGpng full_prediction_Both_HT1000_2b_ThreeToFiveJet_log.png r1 manage 25.6 K 2013-11-22 - 19:04 PaulGeffert  
PDFpdf full_prediction_Both_HT1000_ge2b_FourJet_log.pdf r1 manage 18.1 K 2013-03-07 - 06:42 DavidStuart full_prediction_Both_HT1000_ge2b_FourJet_log.pdf
PNGpng full_prediction_Both_HT1000_ge2b_FourJet_log.png r1 manage 105.0 K 2013-03-07 - 06:43 DavidStuart full_prediction_Both_HT1000_ge2b_FourJet_log.png
PDFpdf full_prediction_Both_HT1000_ge2b_SixJet_log.pdf r1 manage 17.7 K 2013-03-07 - 07:21 DavidStuart  
PNGpng full_prediction_Both_HT1000_ge2b_SixJet_log.png r1 manage 100.7 K 2013-03-07 - 06:44 DavidStuart full_prediction_Both_HT1000_ge2b_SixJet_log.png
PDFpdf full_prediction_Both_HT1000_ge3b_SixJet_log.pdf r1 manage 17.1 K 2013-11-22 - 19:02 PaulGeffert  
PNGpng full_prediction_Both_HT1000_ge3b_SixJet_log.png r1 manage 23.5 K 2013-11-22 - 19:04 PaulGeffert  
PDFpdf full_prediction_Both_HT1000_ge3b_ThreeToFiveJet_log.pdf r1 manage 16.8 K 2013-11-22 - 19:02 PaulGeffert  
PNGpng full_prediction_Both_HT1000_ge3b_ThreeToFiveJet_log.png r1 manage 23.3 K 2013-11-22 - 19:04 PaulGeffert  
PDFpdf full_prediction_Both_HT500_2b_SixJet_log.pdf r1 manage 17.6 K 2013-11-22 - 19:04 PaulGeffert  
PNGpng full_prediction_Both_HT500_2b_SixJet_log.png r1 manage 23.9 K 2013-11-22 - 19:04 PaulGeffert  
PDFpdf full_prediction_Both_HT500_2b_ThreeToFiveJet_log.pdf r1 manage 18.1 K 2013-11-22 - 19:02 PaulGeffert  
PNGpng full_prediction_Both_HT500_2b_ThreeToFiveJet_log.png r1 manage 26.1 K 2013-11-22 - 19:04 PaulGeffert  
PDFpdf full_prediction_Both_HT500_ge2b_FourJet_log.pdf r1 manage 18.3 K 2013-03-07 - 06:39 DavidStuart full_prediction_Both_HT500_ge2b_FourJet_log.pdf
PNGpng full_prediction_Both_HT500_ge2b_FourJet_log.png r1 manage 104.9 K 2013-03-07 - 06:39 DavidStuart full_prediction_Both_HT500_ge2b_FourJet_log.png
PDFpdf full_prediction_Both_HT500_ge2b_SixJet_log.pdf r1 manage 17.9 K 2013-03-07 - 06:40 DavidStuart full_prediction_Both_HT500_ge2b_SixJet_log.pdf
PNGpng full_prediction_Both_HT500_ge2b_SixJet_log.png r1 manage 99.7 K 2013-03-07 - 06:40 DavidStuart full_prediction_Both_HT500_ge2b_SixJet_log.png
PDFpdf full_prediction_Both_HT500_ge3b_SixJet_log.pdf r1 manage 17.4 K 2013-11-22 - 19:02 PaulGeffert  
PNGpng full_prediction_Both_HT500_ge3b_SixJet_log.png r1 manage 23.6 K 2013-11-22 - 19:04 PaulGeffert  
PDFpdf full_prediction_Both_HT500_ge3b_ThreeToFiveJet_log.pdf r1 manage 17.5 K 2013-11-22 - 19:02 PaulGeffert  
PNGpng full_prediction_Both_HT500_ge3b_ThreeToFiveJet_log.png r1 manage 24.2 K 2013-11-22 - 19:04 PaulGeffert  
PDFpdf full_prediction_Both_HT750_2b_SixJet_log.pdf r1 manage 17.6 K 2013-11-22 - 19:04 PaulGeffert  
PNGpng full_prediction_Both_HT750_2b_SixJet_log.png r1 manage 24.3 K 2013-11-22 - 19:04 PaulGeffert  
PDFpdf full_prediction_Both_HT750_2b_ThreeToFiveJet_log.pdf r1 manage 18.1 K 2013-11-22 - 19:02 PaulGeffert  
PNGpng full_prediction_Both_HT750_2b_ThreeToFiveJet_log.png r1 manage 26.5 K 2013-11-22 - 19:04 PaulGeffert  
PDFpdf full_prediction_Both_HT750_ge2b_FourJet_log.pdf r1 manage 18.2 K 2013-03-07 - 06:41 DavidStuart full_prediction_Both_HT750_ge2b_FourJet_log.pdf
PNGpng full_prediction_Both_HT750_ge2b_FourJet_log.png r1 manage 106.2 K 2013-03-07 - 06:41 DavidStuart full_prediction_Both_HT750_ge2b_FourJet_log.png
PDFpdf full_prediction_Both_HT750_ge2b_SixJet_log.pdf r1 manage 17.8 K 2013-03-07 - 06:41 DavidStuart full_prediction_Both_HT750_ge2b_SixJet_log.pdf
PNGpng full_prediction_Both_HT750_ge2b_SixJet_log.png r1 manage 100.9 K 2013-03-07 - 06:42 DavidStuart full_prediction_Both_HT750_ge2b_SixJet_log.png
PDFpdf full_prediction_Both_HT750_ge3b_SixJet_log.pdf r1 manage 17.3 K 2013-11-22 - 19:02 PaulGeffert  
PNGpng full_prediction_Both_HT750_ge3b_SixJet_log.png r1 manage 23.5 K 2013-11-22 - 19:04 PaulGeffert  
PDFpdf full_prediction_Both_HT750_ge3b_ThreeToFiveJet_log.pdf r1 manage 17.5 K 2013-11-22 - 19:53 PaulGeffert  
PNGpng full_prediction_Both_HT750_ge3b_ThreeToFiveJet_log.png r1 manage 24.8 K 2013-11-22 - 19:04 PaulGeffert  
PDFpdf kfactor_graph_sixJet.pdf r1 manage 15.4 K 2013-03-07 - 06:44 DavidStuart kfactor_graph_sixJet.pdf
PNGpng kfactor_graph_sixJet.png r1 manage 82.3 K 2013-03-07 - 06:44 DavidStuart kfactor_graph_sixJet.png
PDFpdf kfactor_graph_sixJet_new.pdf r1 manage 15.4 K 2013-11-22 - 19:12 PaulGeffert  
PNGpng kfactor_graph_sixJet_new.png r1 manage 15.2 K 2013-11-22 - 19:12 PaulGeffert  
Texttxt limits_model_A.txt r1 manage 29.9 K 2013-12-05 - 15:19 WolfgangAdam  
Texttxt limits_model_B.txt r1 manage 4.2 K 2013-12-05 - 15:19 WolfgangAdam  
Texttxt limits_model_C.txt r1 manage 16.8 K 2013-12-05 - 15:19 WolfgangAdam  
PDFpdf met_lsmt_2b_1000.pdf r1 manage 17.1 K 2013-11-26 - 16:29 PaulGeffert  
PNGpng met_lsmt_2b_1000.png r1