The expected limit contour in the GLUINO-NEUTRALINO plane.

The observed limit contour in the SQUARK-NEUTRALINO plane.

The expected limit contour in the SQUARK-NEUTRALINO plane.

95% CL observed and expected upper limits on M_* for spin-independent (D5) WIMP models. The impact of the +-1sigma theoretical uncertainty on the observed limits and the expected +-1sigma range of limits in the absence of a signal are also given.

95% CL observed and expected upper limits on M_* for spin-dependent (D8) WIMP models. The impact of the +-1sigma theoretical uncertainty on the observed limits and the expected +-1sigma range of limits in the absence of a signal are also given.

95% CL observed and expected upper limits on M_* for spin-dependent (D9) WIMP models. The impact of the +-1sigma theoretical uncertainty on the observed limits and the expected +-1sigma range of limits in the absence of a signal are also given.

95% CL observed and expected limits on the nucleon-WIMP scattering cross-section for spin-independent (D1) WIMP models. The impact of the +-1sigma theoretical uncertainty on the observed limits and the expected +-1sigma range of limits in the absence of a signal are also given.

95% CL observed and expected limits on the nucleon-WIMP scattering cross-section for spin-independent (D5) WIMP models. The impact of the +-1sigma theoretical uncertainty on the observed limits and the expected +-1sigma range of limits in the absence of a signal are also given.

95% CL observed and expected limits on the nucleon-WIMP scattering cross-section for spin-dependent (D8) WIMP models. The impact of the +-1sigma theoretical uncertainty on the observed limits and the expected +-1sigma range of limits in the absence of a signal are also given.

95% CL observed and expected limits on the nucleon-WIMP scattering cross-section for spin-dependent (D9) WIMP models. The impact of the +-1sigma theoretical uncertainty on the observed limits and the expected +-1sigma range of limits in the absence of a signal are also given.

Normalized distributions of Tranverse Thrust Minor for 5 lower limit values of leading particle PT.

Normalized distributions of Tranverse Sphericity for 4 ranges of leading particle PT.

Normalized distributions of Tranverse Sphericity for 5 lower limit values of leading particle PT.

Mean Values of Thrust, Thrust Minor and Sphericity verses Multiplicity.

Mean Values of Thrust, Thrust Minor and Sphericity verses charged particle PT scalar sum.

The meff_incl distribution in Signal Region C.

The meff_incl distribution in Signal Region D.

The meff_incl distribution in Signal Region E.

Observed and predicted dimuon invariant mass (m_mumu) distribution in the search region. The bin width is constant in log(m_mumu).

Expected and observed 95% CL limits on the cross-section times branching ratio (sigma*B) for Zprime_SSM production and the two E6-motivated Zprime models with lowest and highest sigma*B for the combination of the dielectron and dimuon channels.

Expected sigma*B for Zprime_SSM production and the two E6-motivated Zprime models with lowest and highest sigma*B.

Expected and observed 95% CL limits on sigma*B for Z* boson production for the combination of the dielectron and dimuon channels.

Expected sigma*B for Z* boson production.

Expected and observed 95% CL limits on M_{G*} versus k/Mbar_{Pl} for the combination of dielectron and dimuon channels.

Expected and observed 95% CL limits on M_{TS} versus eta_{TS} for the combination of dielectron and dimuon channels.

Expected and observed 95% CL limits on M_{pi_T} versus M_{rho_T,omega_T} for the combination of dielectron and dimuon channels.

Expected and observed 95% CL limits on M_A versus the coupling strength g-tilde for the combination of dielectron and dimuon channels.

Expected and observed 95% CL limits on g as a function of M_KK, for the combination of dielectron and dimuon channels.

Expected and observed upper limits on gammaprime within the Minimal Zprime Models parameterization, for the combination of dielectron and dimuon channels. The lower boundary corresponds to tan(theta) = 1.43 and the upper boundary to tan(theta) = -1.19. Two representative values of theta are tan(theta) = 0 and tan(theta) = -2 which correspond to the Z_{B-L} and Z_{3R} model at specific values of gammaprime respectively.

Transverse momentum distribution of the sub-leading lepton in the signal region SR1a showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the 3rd-leading lepton in the signal region SR1a showing both data points with statistical errors only and the expected standard model background.

Missing transverse energy distribution in the signal region SR1a showing both data points with statistical errors only and the expected standard model background.

Mass distribution of Same Flavour Opposite Sign lepton pairs in the signal region SR1a showing both data points with statistical errors only and the expected standard model background.

Jet multiplicity distribution in the signal region SR1a showing both data points with statistical errors only and the expected standard model background.

Transverse mass distribution in the signal region SR1a showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the leading lepton in the signal region SR2 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the sub-leading lepton in the signal region SR2 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the 3rd-leading lepton in the signal region SR2 showing both data points with statistical errors only and the expected standard model background.

Missing transverse energy distribution in the signal region SR2 showing both data points with statistical errors only and the expected standard model background.

Jet multiplicity distribution in the signal region SR2 showing both data points with statistical errors only and the expected standard model background.

Transverse mass distribution in the signal region SR2 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the leading lepton in the validation region VR1 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the sub-leading lepton in the validation region VR1 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the 3rd-leading lepton in the validation region VR1 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the leading lepton in the validation region VR2 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the sub-leading lepton in the validation region VR2 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the 3rd-leading lepton in the validation region VR2 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the leading lepton in the validation region VR3 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the sub-leading lepton in the validation region VR3 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the 3rd-leading lepton in the validation region VR3 showing both data points with statistical errors only and the expected standard model background.

The efficiencies in the different signal regions across the MSSM Direct Gaugino grid of the Higgs mass parameter MU and gaugino massess M1 and M2.

The acceptance in the different signal regions across the MSSM Direct Gaugino grid of the Higgs mass parameter MU and gaugino massess M1 and M2.

The total absolute systematic uncertainty (in number of events) in the different signal regions, not including uncertainties from Monte Carlo statistics, across the MSSM Direct Gaugino grid of the Higgs mass parameter MU and gaugino massess M1 and M2.

The observed CL_s values in the different signal regions across the MSSM Direct Gaugino grid of the Higgs mass parameter MU and gaugino massess M1 and M2.

The cross-section across the MSSM Direct Gaugino grid of the Higgs mass parameter MU and gaugino massess M1 and M2.

The number of generated events across the MSSM Direct Gaugino grid of the Higgs mass parameter MU and gaugino massess M1 and M2.

The efficiencies in the different signal regions across the simplified models with and without intermediate sleptons.

The acceptance in the different signal regions across the simplified models with and without intermediate sleptons.

The total absolute systematic uncertainty (in number of events) in the different signal regions, not including uncertainties from Monte Carlo statistics, across the simplified models with and without intermediate sleptons.

The observed CL_s values in the different signal regions across the simplified models with and without intermediate sleptons.

The cross-section across the simplified models with and without intermediate sleptons.

The number of generated events across the simplified models with and without intermediate sleptons.

The stop pair production cross section and its uncertainty due to PDF, factorization and the renormalization scales.

Cross section x BR limit for the UED model.

The measured PHI* distributions for the dimuon events corrected back to the born level. The distributions are normalised to unity inidividually for each abs(yrap) bin and channel.

The measured PHI* distributions for the dimuon events corrected back to the dress level. The distributions are normalised to unity inidividually for each abs(yrap) bin and channel.

The measured PHI* distributions for the dimuon events corrected back to the bare level. The distributions are normalised to unity inidividually for each abs(yrap) bin and channel.

The combined normalised differential PHI* distributions at the Born level in the different rapidity ranges.

The 95% CL upper limit on the production cross section for charge 5 particles.

The 95% CL upper limit on the production cross section for charge 6 particles.

Differential cross-section measurement for B+ production multiplied by the branching ratio to the J/PSI < MU+ MU- > K+ final state in B+ pT intervals in the B+ rapidity range 1.5<|y|<2.25 The first quoted uncertainty is statistical, the second uncertainty is systematic.

Differential cross-section measurement for B+ production multiplied by the branching ratio to the J/PSI < MU+ MU- > K+ final state in B+ pt intervals in the B+ rapidity (y) range 0<|y|<2.25. The first quoted uncertainty is statistical, the second uncertainty is systematic.

Differential cross-section measurement for B+ production multiplied by the branching ratio to the J/PSI < MU+ MU- > K+ final state in B+ rapidity intervals in the B+ pT range 9 GeV - 120 GeV. The first quoted uncertainty is statistical, the second uncertainty is systematic.

Results for the H_T^leptons signal regions for the >= 3 e/mu off-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the H_T^leptons signal regions for the 2 e/mu + >= 1 tau_had off-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the H_T^leptons signal regions for the >= 3 e/mu on-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the H_T^leptons signal regions for the 2 e/mu + >= 1 tau_had on-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the E_T^miss, H_T^jets<100 GeV signal regions for the >= 3 e/mu off-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the E_T^miss, H_T^jets<100 GeV signal regions for the 2 e/mu + >= 1 tau_had off-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the E_T^miss, H_T^jets<100 GeV signal regions for the >= 3 e/mu on-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the E_T^miss, H_T^jets<100 GeV signal regions for the 2 e/mu + >= 1 tau_had on-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the E_T^miss, H_T^jets>=100 GeV signal regions for the >= 3 e/mu off-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the E_T^miss, H_T^jets>=100 GeV signal regions for the 2 e/mu + >= 1 tau_had off-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the E_T^miss, H_T^jets>=100 GeV signal regions for the >= 3 e/mu on-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the E_T^miss, H_T^jets>=100 GeV signal regions for the 2 e/mu + >= 1 tau_had on-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the m_eff signal regions for the >= 3 e/mu off-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the m_eff signal regions for the 2 e/mu + >= 1 tau_had off-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the m_eff signal regions for the >= 3 e/mu on-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the m_eff signal regions for the 2 e/mu + >= 1 tau_had on-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the m_eff, E_T^miss>=75 GeV signal regions for the >= 3 e/mu off-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the m_eff, E_T^miss>=75 GeV signal regions for the 2 e/mu + >= 1 tau_had off-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the m_eff, E_T^miss>=75 GeV signal regions for the >= 3 e/mu on-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Results for the m_eff, E_T^miss>=75 GeV signal regions for the 2 e/mu + >= 1 tau_had on-Z events. Irreducible sources include all backgrounds estimated with MC simulation. Results are presented in number of expected events as N +- (statistical uncertainty) +- (systematic uncertainty).

Limits in the H_T^leptons bins, for the >= 3 e/mu off-Z events, shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the H_T^leptons bins, for the 2 e/mu + >= 1 tau_had off-Z events, shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the H_T^leptons bins, for the >= 3 e/mu on-Z events, shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the H_T^leptons bins, for the 2 e/mu + >= 1 tau_had on-Z events, shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the E_T^miss bins, for the >= 3 e/mu off-Z events, with H_T^jets<100 GeV requirement shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the E_T^miss bins, for the 2 e/mu + >= 1 tau_had off-Z events, with H_T^jets<100 GeV requirement shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the E_T^miss bins, for the >= 3 e/mu on-Z events, with H_T^jets<100 GeV requirement shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the E_T^miss bins, for the 2 e/mu + >= 1 tau_had on-Z events, with H_T^jets<100 GeV requirement shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the E_T^miss bins, for the >= 3 e/mu off-Z events, with H_T^jets>=100 GeV requirement shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the E_T^miss bins, for the 2 e/mu + >= 1 tau_had off-Z events, with H_T^jets>=100 GeV requirement shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the E_T^miss bins, for the >= 3 e/mu on-Z events, with H_T^jets>=100 GeV requirement shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the E_T^miss bins, for the 2 e/mu + >= 1 tau_had on-Z events, with H_T^jets>=100 GeV requirement shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the m_eff bins, for the >= 3 e/mu off-Z events, shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the m_eff bins, for the 2 e/mu + >= 1 tau_had off-Z events, shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the m_eff bins, for the >= 3 e/mu on-Z events, shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the m_eff bins, for the 2 e/mu + >= 1 tau_had on-Z events, shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the m_eff bins, for the >= 3 e/mu off-Z events, with E_T^miss>=75 GeV requirement shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the m_eff bins, for the 2 e/mu + >= 1 tau_had off-Z events, with E_T^miss>=75 GeV requirement shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the m_eff bins, for the >= 3 e/mu on-Z events, with E_T^miss>=75 GeV requirement shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Limits in the m_eff bins, for the 2 e/mu + >= 1 tau_had on-Z events, with E_T^miss>=75 GeV requirement shown as the upper limit on the visible cross section sigma^vis_95 = N_95/int(Ldt).

Distribution of the PT of the leading muon for E-MU events in the Signal Region, before the application of the leading lepton PT cut.

Distribution of the missing ET for all events in the Signal Region.

Distribution of MET-significnce, ie the missing ET/sqrt(scalar sum of PT of all leptons and jets), for all events in the Signal Region.

Distribution of the missing ET for E-E events in the Z Control Region.

Distribution of the missing ET for MU-MU events in the Z Control Region.

Distribution of the missing ET for E-E events in the Top Control Region.

Distribution of the missing ET for E-MU events in the Top Control Region.

Distribution of the missing ET for MU-MU events in the Top Control Region.

Distribution of the Jet Multiplicity for all events in the Top Control Region.

Distribution of the B-Jet Multiplicity for all events in the Top Control Region.

Distribution of the PT of the leading Jet for all events in the Top Control Region.

Distribution of the PT of the leading B-Jet for all events in the Top Control Region.

Observed and predicted W+W- transverse mass distribution in the E-E channel. Also tabulated are the predictions for a RS graviton of mass 1000 GeV and a bulk RS graviton with mass 600 GeV.

Observed and predicted W+W- transverse mass distribution in the E-MU channel. Also tabulated are the predictions for a RS graviton of mass 1000 GeV and a bulk RS graviton with mass 600 GeV.

Expected and observed number of events with m_ll > 1300 GeV in the dielectron and dimuon channels. Yields given for different MS values correspond to the sum of signal and background events, with the signal obtained in the GRW formalism. All yields are normalized to the Z peak control region. The errors quoted originate from systematic uncertainties and limited MC statistics.

Expected and observed 95% C.L. lower limits on MS in the dielectron and dimuon channels, as well as for the combination of those channels without and with the diphoton channel in the GRW formalism. Separate results are provided for the different choices of flat priors.

Observed 95% C.L. lower limits on MS (in units of TeV), including systematic uncertainties, for ADD signal in the GRW, Hewett and HLZ formalisms with no K-factor applied to the signal. Separate results are provided for the different choices of flat priors.

Observed 95% C.L. lower limits on of TeV), including systematic uncertainties, for in the GRW, Hewett and HLZ formalisms with K-factors of 1.6 and 1.7 applied to the signal for the dilepton and diphoton channels, respectively. Separate results are provided for the different choices of flat priors.

Fiducial Upsilon(3S) production cross-section, where pT>4 GeV and |eta|<2.3 for both muons, as a function of Upsilon(3S) pT in the Upsilon(3S) rapidity (|y|) bins 0-1.2 and 1.2-2.25. The first uncertainty is statistical, the second is systematic.

Fiducial Upsilon(nS) production cross-section, where pT>4 GeV and |eta|<2.3 for both muons, as a function of Upsilon(nS) rapidity (|y|) in Upsilon(nS) PT ranging from 0 - 70 GeV. The first uncertainty is statistical, the second is systematic.

Inclusive Upsilon(1S) production cross-section as a function of Upsilon(1S) pT in the Upsilon(1S) rapidity (|y|) bins 0-1.2 and 1.2-2.25. The first uncertainty is statistical, the second is systematic and the third encapsulates any possible variation due to spin-alignment from the unpolarised central value.

Inclusive Upsilon(2S) production cross-section as a function of Upsilon(2S) pT in the Upsilon(2S) rapidity (|y|) bins 0-1.2 and 1.2-2.25. The first uncertainty is statistical, the second is systematic and the third encapsulates any possible variation due to spin-alignment from the unpolarised central value.

Inclusive Upsilon(3S) production cross-section as a function of Upsilon(3S) pT in the Upsilon(3S) rapidity (|y|) bins 0-1.2 and 1.2-2.25. The first uncertainty is statistical, the second is systematic and the third encapsulates any possible variation due to spin-alignment from the unpolarised central value.

Inclusive Upsilon(nS) production cross-section as a function of Upsilon(nS) rapidity (|y|) in Upsilon(nS) PT ranging from 0 - 70 GeV. The first uncertainty is statistical, the second is systematic and the third encapsulates any possible variation due to spin-alignment from the unpolarised central value.

Ratio of Upsilon(2S) to Upsilon(1S) inclusive cross-section as a function of Upsilon pT in the Upsilon rapidity (|y|) bins 0-1.2 and 1.2-2.25. The first uncertainty is statistical, the second is systematic.

Ratio of Upsilon(3S) to Upsilon(1S) inclusive cross-section as a function of Upsilon pT in the Upsilon rapidity (|y|) bins 0-1.2 and 1.2-2.25. The first uncertainty is statistical, the second is systematic.

Ratio of Upsilon(2S) and Upsilon(3S) to Upsilon(1S) inclusive cross-section as a function of Upsilon rapidity (|y|) in Upsilon pT 0 - 70 GeV. The first uncertainty is statistical, the second is systematic.

Distributions of the splitting scale variable sqrt(d3) shown separately for the Electron and Muon decay modes of the W boson.

Distributions of the ratios of the splitting scale variables sqrt(d1/d0) shown separately for the Electron and Muon decay modes of the W boson.

Distributions of the ratios of the splitting scale variables sqrt(d2/d1) shown separately for the Electron and Muon decay modes of the W boson.

Distributions of the ratios of the splitting scale variables sqrt(d3/d2) shown separately for the Electron and Muon decay modes of the W boson.

The transverse momentum distribution of the 4th-leading lepton for events with at least 4 leptons and no Z-boson candidate.

Distribution of missing transverse momentum for events with at least 4 leptons and no Z-boson candidate.

Distribution of effective mass for events with at least 4 leptons and no Z-boson candidate.

Simplified Model (1) Number of generated events (2) Cross-section [pb] (3) CL_{S} [%] for SR1 (4) Acceptance [%] for SR1 (5) Efficiency [%] for SR1 (6) Uncertainty (not including MC statistics) for SR1 (7) CL_{S} [%] for SR2 (8) Acceptance [%] for SR2 (9) Efficiency [%] for SR2 (10) Uncertainty (not including MC statistics) for SR2.

MSUGRA/CMSSM Model (1) Number of generated events (2) Cross-section [pb] (3) CL_{S} [%] for SR1 (4) Acceptance [%] for SR1 (5) Efficiency [%] for SR1 (6) Uncertainty (not including MC statistics) for SR1 (7) CL_{S} [%] for SR2 (8) Acceptance [%] for SR2 (9) Efficiency [%] for SR2 (10) Uncertainty (not including MC statistics) for SR2.

Correlations in the PT distribution.

Normalised fiducial cross section in bins of the Mass of the WZ.

Correlations in the Mass distribution.

The corrected per-event transverse momentum distribution of Z bosons in the centrality region 10-20%.

The corrected per-event transverse momentum distribution of Z bosons in the centrality region 20-40%.

The corrected per-event transverse momentum distribution of Z bosons in the centrality region 40-80%.

Combined results for the centrality (Npart) dependence of Z boson yields divided by Ncoll for the PT range > 0 GeV/c. The systematic error includes the uncertainty in Ncoll.

Combined results for the centrality (Npart) dependence of Z boson yields divided by Ncoll for the PT range 0 to 10 GeV/c. The systematic error includes the uncertainty in Ncoll.

Combined results for the centrality (Npart) dependence of Z boson yields divided by Ncoll for the PT range 10 to 30 GeV/c. The systematic error includes the uncertainty in Ncoll.

Combined results for the centrality (Npart) dependence of Z boson yields divided by Ncoll for the PT range > 30 GeV/c. The systematic error includes the uncertainty in Ncoll.

The Acceptance, Efficiency and Acceptance x Efficiency for the tau+muon channel as a function of Lambda and Tan(Beta).

The Acceptance, Efficiency and Acceptance x Efficiency for the tau+electron channel as a function of Lambda and Tan(Beta).

(1) Number of generated MC events for the spin 1/2 top partner signal grid (2) Relative Cross section uncertainties for the spin 1/2 top partner signal grid.

(1) Acceptance of the same flavour selection for the spin 1/2 top partner signal grid (2) Selection efficiency of the same flavour selection for the spin 1/2 top partner signal grid (3) Product of the acceptance and efficiency of the same flavour selection for the spin 1/2 top partner signal grid (4) Relative experimental uncertainties on the acceptance times efficiency of the same flavour selection for the spin 1/2 top partner signal grid.

(1) Acceptance of the different flavour selection for the spin 1/2 top partner signal grid (2) Selection efficiency of the different flavour selection for the spin 1/2 top partner signal grid (3) Product of the acceptance and efficiency of the different flavour selection for the spin 1/2 top partner signal grid (4) Relative experimental uncertainties on the acceptance times efficiency of the different flavour selection for the spin 1/2 top partner signal grid.

(1) Observed CLs values for the scalar top signal grid (2) Expected CLs values for the scalar top signal grid.

(1) Observed CLs values for the spin 1/2 top partner signal grid (2) Expected CLs values for the spin 1/2 top partner signal grid.

Cross section limits [pb] for the scalar top signal grid.

Cross section limits [pb] for the spin 1/2 top partner signal grid.

Observed 95% CL limit for stop grid as a function of the scalar top and neutralino masses.

Observed 95% CL limit for stop grid as a function of the scalar top and neutralino masses, varying signal cross section of +1sigma.

Observed 95% CL limit for stop grid as a function of the scalar top and neutralino masses, varying signal cross section of -1sigma.

Expected 95% CL limit for stop grid as a function of the scalar top and neutralino masses.

Expected 95% CL limit for stop grid as a function of the scalar top and neutralino masses, varying the uncertainty of +1sigma.

Expected 95% CL limit for stop grid as a function of the scalar top and neutralino masses, varying the uncertainty of -1sigma.

Observed 95% CL limit for top partner grid as a function of the top partner and neutralino masses.

Observed 95% CL limit for top partner grid as a function of the top partner and neutralino masses, varying signal cross section of +1sigma.

Observed 95% CL limit for top partner grid as a function of the top partner and neutralino masses, varying signal cross section of -1sigma.

Expected 95% CL limit for top partner grid as a function of the top partner and neutralino masses.

Expected 95% CL limit for top partner grid as a function of the top partner and neutralino masses, varying the uncertainty of +1sigma.

Expected 95% CL limit for top partner grid as a function of the top partner and neutralino masses, varying the uncertainty of -1sigma.

Number of tracks in vertex vs invariant mass of vertex (DATA) The number of tracks in the vertex vs the invariant mass of the vertex, for the data, and for the MH signal sample respectively. All selection cuts are applied, with the exceptions of those on the variables in the plot (Ntrk and mass), and the offline muon requirements.

Number of tracks in vertex vs invariant mass of vertex (SIGNAL) The number of tracks in the vertex vs the invariant mass of the vertex, for the data, and for the MH signal sample respectively. All selection cuts are applied, with the exceptions of those on the variables in the plot (Ntrk and mass), and the offline muon requirements.

95% CL upper limit on sigma.BR^2 vs c*tau The observed 95% CL upper limits on the cross-section for squark production, multiplied by the branching fraction for both squarks to decay to long-lived neutralinos, which in turn decay to mu+jets, given that we observed zero events in the signal region.

Expected upper limit on sigma.BR^2 vs c*tau The expected 95% CL upper limits on the cross-section for squark production, multiplied by the branching fraction for both squarks to decay to long-lived neutralinos, which in turn decay to mu+jets.

Figure 2-a. Expected limit +1sigma.

Figure 2-a. Expected limit.

Figure 2-a. Expected limit -1sigma.

Figure 2-b. Observed limit +1sigma-th.

Figure 2-b. Observed limit.

Figure 2-b. Observed limit -1sigma-th.

Figure 2-b. Expected limit +1sigma.

Figure 2. Auxiliary material. Cross section for the Gbb and Gtt model.

Figure 3a. Auxiliary material. Theoretical uncertainty for the Gbb model.

Figure 3b. Auxiliary material. Theoretical uncertainty for the Gtt model.

Figure 4a. Auxiliary material. Number of MC events for the Gbb model.

Figure 4b. Auxiliary material. Number of MC events for the Gtt model.

Figure 5a. Auxiliary material. Acceptance for the Gbb model in the signal region SR4-L.

Figure 5b. Auxiliary material. Acceptance for the Gbb model in the signal region SR4-M.

Figure 5c. Auxiliary material. Acceptance for the Gbb model in the signal region SR4-T.

Figure 6a. Auxiliary material. Acceptance for the Gtt model in the signal region SR6-L.

Figure 6b. Auxiliary material. Acceptance for the Gtt model in the signal region SR6-T.

Figure 7a. Auxiliary material. Efficiency for the Gbb model in the signal region SR4-L.

Figure 7b. Auxiliary material. Efficiency for the Gbb model in the signal region SR4-M.

Figure 7c. Auxiliary material. Efficiency for the Gbb model in the signal region SR4-T.

Figure 8a. Auxiliary material. Efficiency for the Gtt model in the signal region SR6-L.

Figure 8b. Auxiliary material. Efficiency for the Gtt model in the signal region SR6-T.

Figure 9a. Auxiliary material. Experimental uncertainty for the Gbb model in the signal region SR4-L.

Figure 9b. Auxiliary material. Experimental uncertainty for the Gbb model in the signal region SR4-M.

Figure 9c. Auxiliary material. Experimental uncertainty for the Gbb model in the signal region SR4-T.

Figure 10a. Auxiliary material. Experimental uncertainty for the Gtt model in the signal region SR6-L.

Figure 10b. Auxiliary material. Experimental uncertainty for the Gtt model in the signal region SR6-T.

Figure 11a. Auxiliary material. Observed CLs for the Gbb model in the signal region SR4-L.

Figure 11b. Auxiliary material. Observed CLs for the Gbb model in the signal region SR4-M.

Figure 11c. Auxiliary material. Observed CLs for the Gbb model in the signal region SR4-T.

Figure 12a. Auxiliary material. Observed CLs for the Gtt model in the signal region SR6-L.

Figure 12b. Auxiliary material. Observed CLs for the Gtt model in the signal region SR6-T.

Figure 13a. Auxiliary material. Expected CLs for the Gbb model in the signal region SR4-L.

Figure 13b. Auxiliary material. Expected CLs for the Gbb model in the signal region SR4-M.

Figure 13c. Auxiliary material. Expected CLs for the Gbb model in the signal region SR4-T.

Figure 14a. Auxiliary material. Expected CLs for the Gtt model in the signal region SR6-L.

Figure 14b. Auxiliary material. Expected CLs for the Gtt model in the signal region SR6-T.

Figure 15a. Auxiliary material. Upper Limit for the Gbb model.

Figure 15b. Auxiliary material. Upper Limit for the Gtt model.

Figure 16a. Auxiliary material. Best Signal Region for the Gbb model.

Figure 16b. Auxiliary material. Best Signal Region for the Gtt model.

The measured exclusive fiducial cross section of Zgamma (l+;l-;gamma) decay channel. The first systematic (sys) error is the combined systematic uncertainty excluding that of the luminosity. The second (sys) error is the uncertainty on the luminosity.

The measured inclusive fiducial cross section of Zgamma (nu;nubar;gamma) decay channel. The first systematic (sys) error is the combined systematic uncertainty excluding that of the luminosity. The second (sys) error is the uncertainty on the luminosity.

The measured exclusive fiducial cross section of Zgamma (nu;nubar;gamma) decay channel. The first systematic (sys) error is the combined systematic uncertainty excluding that of the luminosity. The second (sys) error is the uncertainty on the luminosity.

Differential fiducial cross section of Wgamma (l;nu;gamma) decay channel in bins of the leading photon PT. Leading Photon is the photon in the final state with highest PT.

Differential fiducial cross section of Wgamma (l;nu;gamma) decay channel in bins of the leading photon PT. Leading Photon is the photon in the final state with highest PT.

Normalised fiducial cross section of Wgamma (l;nu;gamma) decay channel in bins of the leading photon PT. Leading Photon is the photon in the final state with highest PT.

Normalised fiducial cross section of Wgamma (l;nu;gamma) decay channel in bins of the leading photon PT. Leading Photon is the photon in the final state with highest PT.

Differential fiducial cross section of Zgamma (l+;l-;gamma) decay channel in bins of the leading photon PT. Leading Photon is the photon in the final state with highest PT.

Differential fiducial cross section of Wgamma (l;nu;gamma) decay channel in bins of the leading photon PT. Leading Photon is the photon in the final state with highest PT.

Normalised fiducial cross section of Zgamma (l+;l-;gamma) decay channel in bins of the leading photon PT. Leading Photon is the photon in the final state with highest PT.

Normalised fiducial cross section of Zgamma (l+;l-;gamma) decay channel in bins of the leading photon PT. Leading Photon is the photon in the final state with highest PT.

Normalised fiducial cross section of Wgamma (l;nu;gamma) decay channel in bins of the jet multiplicity with leading photon pT > 15 GeV.

Normalised fiducial cross section of Wgamma (l;nu;gamma) decay channel in bins of the jet multiplicity with leading photon pT > 60 GeV.

Normalised fiducial cross section of Zgamma (l+;l+;gamma) decay channel in bins of the jet multiplicity with leading photon pT > 15 GeV.

Normalised fiducial cross section of Zgamma (l+;l+;gamma) decay channel in bins of the jet multiplicity with leading photon pT > 60 GeV.

Normalised fiducial cross section of Wgamma (l;nu;gamma) decay channel in bins of the transverse mass of Wgamma with leading photon pT > 40 GeV.

Normalised fiducial cross section of Zgamma (l+;l+;gamma) decay channel in bins of the mass of Zgamma with leading photon pT > 40 GeV.

The reconstruction efficiency of spin 1 narrow resonance a_T in low scale technicolor model decays to Wgamma (l;nu;gamma) final state with leading photon PT > 40 GeV.

95% C.L. observed and expected upper limits on fiducial cross section of spin 1 narrow resonance decays to Wgamma (l;nu;gamma) final state.

The reconstruction efficiency of spin 1 narrow resonance rho_T in low scale technicolor model decays to Zgamma (l+;l-;gamma) final state with leading photon PT > 40 GeV.

95% C.L. observed and expected upper limits on fiducial cross section of spin 1 narrow resonance decays to Zgamma (l+;l+;gamma) final state.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 2 < pT(a) < 3 GeV and 0.5 < pT(b) < 4 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 3 < pT(a) < 4 GeV and 0.5 < pT(b) < 4 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 4 < pT(a) < 5 GeV and 0.5 < pT(b) < 4 GeV.

Integrated per-trigger yields, Yint, versus pT(a) for 0.5 < pT(b) < 4 GeV, in the SUM(ET(PB)) > 80 GeV event class, on the near-side, |Delta(phi)| < PI/3.

Integrated per-trigger yields, Yint, versus pT(a) for 0.5 < pT(b) < 4 GeV, in the SUM(ET(PB)) = 55-80 GeV event class, on the near-side, |Delta(phi)| < PI/3.

Integrated per-trigger yields, Yint, versus pT(a) for 0.5 < pT(b) < 4 GeV, in the SUM(ET(PB)) = 25-55 GeV event class, on the near-side, |Delta(phi)| < PI/3.

Integrated per-trigger yields, Yint, versus pT(a) for 0.5 < pT(b) < 4 GeV, in the SUM(ET(PB)) < 20 GeV event class, on the near-side, |Delta(phi)| < PI/3.

Difference of the yield in the SUM(ET(PB)) > 80 GeV event class from that in the SUM(ET(PB)) < 20 GeV event class, on the near-side, |Delta(phi)| < PI/3.

Difference of the yield in the SUM(ET(PB)) = 55-80 GeV event class from that in the SUM(ET(PB)) < 20 GeV event class, on the near-side, |Delta(phi)| < PI/3.

Difference of the yield in the SUM(ET(PB)) = 25-55 GeV event class from that in the SUM(ET(PB)) < 20 GeV event class, on the near-side, |Delta(phi)| < PI/3.

Integrated per-trigger yields, Yint, versus pT(a) for 0.5 < pT(b) < 4 GeV, in the SUM(ET(PB)) > 80 GeV event class, on the away-side, |Delta(phi)| > 2*PI/3.

Integrated per-trigger yields, Yint, versus pT(a) for 0.5 < pT(b) < 4 GeV, in the SUM(ET(PB)) = 55-80 GeV event class, on the away-side, |Delta(phi)| > 2*PI/3.

Integrated per-trigger yields, Yint, versus pT(a) for 0.5 < pT(b) < 4 GeV, in the SUM(ET(PB)) = 25-55 GeV event class, on the away-side, |Delta(phi)| > 2*PI/3.

Integrated per-trigger yields, Yint, versus pT(a) for 0.5 < pT(b) < 4 GeV, in the SUM(ET(PB)) < 20 GeV event class, on the away-side, |Delta(phi)| > 2*PI/3.

Difference of the yield in the SUM(ET(PB)) > 80 GeV event class from that in the SUM(ET(PB)) < 20 GeV event class, on the away-side, |Delta(phi)| > 2*PI/3.

Difference of the yield in the SUM(ET(PB)) = 55-80 GeV event class from that in the SUM(ET(PB)) < 20 GeV event class, on the away-side, |Delta(phi)| > 2*PI/3.

Difference of the yield in the SUM(ET(PB)) = 25-55 GeV event class from that in the SUM(ET(PB)) < 20 GeV event class, on the away-side, |Delta(phi)| > 2*PI/3.

The pT(a) dependence of c2 for 0.5 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of c2 for 0.5 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of c2 for 0.5 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s2 for 0.5 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s2 for 0.5 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s2 for 0.5 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of c3 for 0.5 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of c3 for 0.5 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of c3 for 0.5 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s3 for 0.5 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s3 for 0.5 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s3 for 0.5 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of c2 for 1 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of c2 for 1 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of c2 for 1 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s2 for 1 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s2 for 1 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s2 for 1 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of c3 for 1 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of c3 for 1 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of c3 for 1 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s3 for 1 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s3 for 1 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s3 for 1 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of c2 for 1.5 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of c2 for 1.5 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of c2 for 1.5 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s2 for 1.5 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s2 for 1.5 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s2 for 1.5 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of c3 for 1.5 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of c3 for 1.5 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of c3 for 1.5 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s3 for 1.5 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s3 for 1.5 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s3 for 1.5 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of c2 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of c2 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of c2 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s2 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s2 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s2 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of c3 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of c3 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of c3 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s3 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s3 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s3 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of c2 for 1 < pT(b) < 2, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of c2 for 1 < pT(b) < 2, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of c2 for 1 < pT(b) < 2, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s2 for 1 < pT(b) < 2, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s2 for 1 < pT(b) < 2, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s2 for 1 < pT(b) < 2, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of c3 for 1 < pT(b) < 2, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of c3 for 1 < pT(b) < 2, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of c3 for 1 < pT(b) < 2, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s3 for 1 < pT(b) < 2, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s3 for 1 < pT(b) < 2, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s3 for 1 < pT(b) < 2, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of c2 for 2 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of c2 for 2 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of c2 for 2 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s2 for 2 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s2 for 2 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s2 for 2 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of c3 for 2 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of c3 for 2 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of c3 for 2 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s3 for 2 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s3 for 2 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s3 for 2 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

Integrated per-trigger yield, Yint, for 0.5 < pT(a,b) < 4 GeV, measured in intervals of SUM(ET(PB)), for the near-side (|Delta(phi)| < PI/3), away-side (|Delta(phi)| > 2*PI/3) and the difference between them, DELTA(Yint).

Integrated per-trigger yield, Yint, for 1 < pT(a,b) < 4 GeV, measured in intervals of SUM(ET(PB)), for the near-side (|Delta(phi)| < PI/3), away-side (|Delta(phi)| > 2*PI/3) and the difference between them, DELTA(Yint).

Integrated per-trigger yield, Yint, for 0.5 < pT(a,b) < 4 GeV, measured in intervals of Nch, where Nch represents the charged-particle multiplicity measured over |eta| < 2.5 with pT > 0.4 GeV, for the near-side (|Delta(phi)| < PI/3), away-side (|Delta(phi)| > 2*PI/3) and the difference between them, DELTA(Yint).

Integrated per-trigger yield, Yint, for 1 < pT(a,b) < 4 GeV, measured in intervals of Nch, where Nch represents the charged-particle multiplicity measured over |eta| < 2.5 with pT > 0.4 GeV, for the near-side (|Delta(phi)| < PI/3), away-side (|Delta(phi)| > 2*PI/3) and the difference between them, DELTA(Yint).

The pT(a) dependence of s2 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s2 for 1 < pT(b) < 2, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s2 for 2 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s2 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s2 for 1 < pT(b) < 2, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s2 for 2 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s2 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s2 for 1 < pT(b) < 2, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s2 for 2 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s3 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s3 for 1 < pT(b) < 2, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s3 for 2 < pT(b) < 4, in the SUM(ET(PB)) > 80 GeV event class.

The pT(a) dependence of s3 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s3 for 1 < pT(b) < 2, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s3 for 2 < pT(b) < 4, in the SUM(ET(PB)) = 55-80 GeV event class.

The pT(a) dependence of s3 for 0.5 < pT(b) < 1, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s3 for 1 < pT(b) < 2, in the SUM(ET(PB)) = 25-55 GeV event class.

The pT(a) dependence of s3 for 2 < pT(b) < 4, in the SUM(ET(PB)) = 25-55 GeV event class.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 3 < pT(a) < 4 GeV and 0.3 < pT(b) < 0.5 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 3 < pT(a) < 4 GeV and 0.5 < pT(b) < 1 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 3 < pT(a) < 4 GeV and 1 < pT(b) < 2 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 3 < pT(a) < 4 GeV and 2 < pT(b) < 3 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 2 < pT(a) < 3 GeV and 0.3 < pT(b) < 0.5 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 2 < pT(a) < 3 GeV and 0.5 < pT(b) < 1 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 2 < pT(a) < 3 GeV and 1 < pT(b) < 2 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 2 < pT(a) < 3 GeV and 2 < pT(b) < 3 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 1 < pT(a) < 2 GeV and 0.3 < pT(b) < 0.5 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 1 < pT(a) < 2 GeV and 0.5 < pT(b) < 1 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 1 < pT(a) < 2 GeV and 1 < pT(b) < 2 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 0.5 < pT(a) < 1 GeV and 0.3 < pT(b) < 0.5 GeV.

Distribution of per-trigger yield, Y(DELTA(PHI)), in the peripheral and the central event activity classes and their differences, for 0.5 < pT(a) < 1 GeV and 0.5 < pT(b) < 1 GeV.

Measured double-differential dijet cross sections for the range 1.5 <= y* < 2.0 and jet radius parameter R = 0.4. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 2.0 <= y* < 2.5 and jet radius parameter R = 0.4. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 2.5 <= y* < 3.0 and jet radius parameter R = 0.4. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 0.0 <= y* < 0.5 and jet radius parameter R = 0.6. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 0.5 <= y* < 1.0 and jet radius parameter R = 0.6. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 1.0 <= y* < 1.5 and jet radius parameter R = 0.6. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 1.5 <= y* < 2.0 and jet radius parameter R = 0.6. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 2.0 <= y* < 2.5 and jet radius parameter R = 0.6. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 2.5 <= y* < 3.0 and jet radius parameter R = 0.6. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Observed limits on the effective theory mass scale M* as a function of the dark matter mass M(chi) at 90% confidence-level from combined mono-W-boson and mono-Z-boson signals for various operators.

Limits on chi-nucleon cross sections as a function of M(chi) at 90% confidence-level.

Limit on the Higgs boson cross section for decay to invisible particles divided by the cross section for decays to Standard Model particles as a function of M(Higgs) at 95% confidence-level.

Integrated jet shape as a function of the radius r for the PT range 40-50 GeV.

Differential jet shape as a function of the radius r for the PT range 50-70 GeV.

Integrated jet shape as a function of the radius r for the PT range 50-70 GeV.

Differential jet shape as a function of the radius r for the PT range 70-100 GeV.

Integrated jet shape as a function of the radius r for the PT range 70-100 GeV.

Differential jet shape as a function of the radius r for the PT range 100-150 GeV.

Integrated jet shape as a function of the radius r for the PT range 100-150 GeV.

The measured inclusive jet double-differential cross section in the rapidity bin 1.2 <= |y| < 2.1 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 2.1 <= |y| < 2.8 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 2.8 <= |y| < 3.6 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 3.6 <= |y| < 4.4 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin |y| < 0.3 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 0.3 <= |y| < 0.8 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 0.8 <= |y| < 1.2 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 1.2 <= |y| < 2.1 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 2.1 <= |y| < 2.8 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 2.8 <= |y| < 3.6 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 3.6 <= |y| < 4.4 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin |y| < 0.3 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.3 <= |y| < 0.8 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.8 <= |y| < 1.2 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 1.2 <= |y| < 2.1 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.1 <= |y| < 2.8 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.8 <= |y| < 3.6 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 3.6 <= |y| < 4.4 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin |y| < 0.3 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.3 <= |y| < 0.8 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.8 <= |y| < 1.2 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 1.2 <= |y| < 2.1 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.1 <= |y| < 2.8 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.8 <= |y| < 3.6 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 3.6 <= |y| < 4.4 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin |y| < 0.3 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.3 <= |y| < 0.8 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.8 <= |y| < 1.2 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 1.2 <= |y| < 2.1 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.1 <= |y| < 2.8 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.8 <= |y| < 3.6 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 3.6 <= |y| < 4.4 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin |y| < 0.3 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.3 <= |y| < 0.8 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.8 <= |y| < 1.2 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 1.2 <= |y| < 2.1 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.1 <= |y| < 2.8 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.8 <= |y| < 3.6 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 3.6 <= |y| < 4.4 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

For events in the low-ETmiss validation region, the M(l tau) distribution in VR1taua.

For events in the low-ETmiss validation region, the MT2max distribution in VR2taua.

For events in the high-ETmiss + b-tagged jet validation region, the ETmiss distribution in VR0taunoZb.

For events in the high-ETmiss + b-tagged jet validation region, the ETmiss distribution in VR0tauZb.

For events in the high-ETmiss + b-tagged jet validation region, the ETmiss distribution in VR1taub.

For events in the high-ETmiss + b-tagged jet validation region, the ETmiss distribution in VR2taub.

Expected distributions of SM background events and observed data distributions in the binned signal regions SR0taua.

The distribution of ETmiss in the summation of all SR0taua regions prior to the requirements on this variable.

The distribution of MT in the summation of all SR0taua regions prior to the requirements on this variable.

The distribution of M(SFOS) in the summation of all SR0taua regions prior to the requirements on this variable.

Expected distribution of SM background events and observed data distribution for the MIN(DELTA(PHI(ll))) variable in the SR0taub region, prior to the requirements on this variable.

Expected distribution of SM background events and observed data distribution for the ETmiss variable in the SR1tau region, prior to the requirements on this variable.

Expected distribution of SM background events and observed data distribution for the MT2max variable in the SR2taua region, prior to the requirements on this variable.

Expected distribution of SM background events and observed data distribution for the M(tau tau) variable in the SR2taub region, prior to the requirements on this variable.

Observed 95% CL exclusion contour for chargino and neutralino production in the sleptonL-mediated simplified model.

Expected 95% CL exclusion contour for chargino and neutralino production in the sleptonL-mediated simplified model.

Observed 95% CL exclusion contour for chargino and neutralino production in the WZ-mediated simplified model.

Expected 95% CL exclusion contour for chargino and neutralino production in the WZ-mediated simplified model.

Observed 95% CL exclusion contour for chargino and neutralino production in the stauL-mediated simplified model.

Expected 95% CL exclusion contour for chargino and neutralino production in the stauL-mediated simplified model.

Observed 95% CL exclusion contour for chargino and neutralino production in the Wh-mediated simplified model.

Expected 95% CL exclusion contour for chargino and neutralino production in the Wh-mediated simplified model.

Observed 95% CL exclusion contour in the pMSSM model with sleptons and M1 = 100 GeV.

Expected 95% CL exclusion contour in the pMSSM model with sleptons and M1 = 100 GeV.

Observed 95% CL exclusion contour in the pMSSM model with sleptons and M1 = 140 GeV.

Expected 95% CL exclusion contour in the pMSSM model with sleptons and M1 = 140 GeV.

Observed 95% CL exclusion contour in the pMSSM model with sleptons and M1 = 250 GeV.

Expected 95% CL exclusion contour in the pMSSM model with sleptons and M1 = 250 GeV.

Observed 95% CL exclusion contour in the pMSSM model with staus.

Expected 95% CL exclusion contour in the pMSSM model with staus.

Observed 95% CL exclusion contour in the pMSSM model with no sleptons.

Expected 95% CL exclusion contour in the pMSSM model with no sleptons.

Excluded model cross-sections at 95% confidence level for the slepL-mediated simplified model.

Excluded model cross-sections at 95% confidence level for WZ-mediated simplified model.

Excluded model cross-sections at 95% confidence level for stauL-mediated simplified model.

Excluded model cross-sections at 95% confidence level for Wh-mediated simplified model.

Number of generated signal events for slepL-mediated simplified model.

Number of generated signal events for WZ-mediated simplified model.

Number of generated signal events for stauL-mediated simplified model.

Number of generated signal events for Wh-mediated simplified model.

Cross-sections for slepL-mediated simplified model.

Cross-sections for WZ-mediated simplified model.

Cross-sections for stauL-mediated simplified model.

Cross-sections for Wh-mediated simplified model.

Acceptance for slepL-mediated simplified model using SR0taua bin 20.

Acceptance for WZ-mediated simplified model using SR0taua bin 16.

Acceptance for stauL-mediated simplified model using SR2taua.

Acceptance for Wh-mediated simplified model using SR2taub.

Efficiency for slepL-mediated simplified model using SR0taua bin 20.

Efficiency for WZ-mediated simplified model using SR0taua bin 16.

Efficiency for stauL-mediated simplified model using SR2taua.

Efficiency for Wh-mediated simplified model using SR2taub.

The total experimental uncertainty, not including Monte Carlo statistics, for the slepL-mediated simplified model using SR0taua bin 20.

The total experimental uncertainty, not including Monte Carlo statistics, for the WZ-mediated simplified model using SR0taua bin 16.

The total experimental uncertainty, not including Monte Carlo statistics, for the stauL-mediated simplified model using SR2taua.

The total experimental uncertainty, not including Monte Carlo statistics, for the Wh-mediated simplified model using SR2taub.

The expected CL for slepL-mediated simplified model using SR0taua bin 20, using pseudo-experiments.

The expected CL for WZ-mediated simplified model using SR0taua bin 16, using pseudo-experiments.

The expected CL for stauL-mediated simplified model using SR2taua, using pseudo-experiments.

The expected CL for Wh-mediated simplified model using SR2taub, using pseudo-experiments.

The observed CL for slepL-mediated simplified model using SR0taua bin 20, using pseudo-experiments.

The observed CL for WZ-mediated simplified model using SR0taua bin 16, using pseudo-experiments.

The observed CL for stauL-mediated simplified model using SR2taua, using pseudo-experiments.

The observed CL for Wh-mediated simplified model using SR2taub, using pseudo-experiments.

MET/sqrt(HT) distributions for the multi-jet + flavour stream with PTmin=50 GeV, and exactly nine jets, with the signal region selection, other than that on MET/sqrt(HT) itself. A selection of one-bjet is applied.

MET/sqrt(HT) distributions for the multi-jet + flavour stream with PTmin=50 GeV, and exactly eight jets, with the signal region selection, other than that on MET/sqrt(HT) itself. A selection of two or more b-jets is applied.

MET/sqrt(HT) distributions for the multi-jet + flavour stream with PTmin=50 GeV, and exactly nine jets, with the signal region selection, other than that on MET/sqrt(HT) itself. A selection of two or more b-jets is applied.

MET/sqrt(HT) distribution for the multi-jet + flavour stream with PTmin=50 GeV, and at least ten jets. The complete >=10j50 selection has been applied, other than the final MET/sqrt(HT) requirement.

MET/sqrt(HT) distributions for the multi-jet + flavour stream with pTmin=80 GeV, and exactly seven jets. The complete signal region selections were applied, other than the final MET/sqrts(HT) requirement. A selection of zero b-jets is applied.

MET/sqrts(HT) distributions for the multi-jet + flavour stream with pTmin=80 GeV, and at least eight jets. The complete signal region selections were applied, other than the final MET/sqrts(HT) requirement. A selection of zero b-jets is applied.

MET/(HT) distributions for the multi-jet + flavour stream with pTmin=80 GeV, and exactly seven jets. The complete signal region selections were applied, other than the final MET/sqrts(HT) requirement. A selection of one b-jet is applied.

MET/sqrts(HT) distributions for the multi-jet + flavour stream with pTmin=80 GeV, and at least eight jets. The complete signal region selections were applied, other than the final MET/sqrts(HT) requirement. A selection of one b-jet is applied.

MET/sqrts(HT) distributions for the multi-jet + flavour stream with pTmin=80 GeV, and exactly seven jets. The complete signal region selections were applied, other than the final MET/sqrts(HT) requirement. A selection of two or more b-jets is applied.

MET/sqrts(HT) distributions for the multi-jet + flavour stream with pTmin=80 GeV, and at least eight jets. The complete signal region selections were applied, other than the final MET/sqrts(HT) requirement. A selection of two or more b-jets is applied.

MET/sqrt(HT) distributions for the multi-jet + MJ(Sigma) stream with the MJ(Sigma)>340 GeV signal region selection, other than the final MET/sqrt(HT) requirement. There is a minimum multiplicity requirement of eight for the PTmin=50 GeV, R=0.4 jets.

MET/sqrt(HT) distributions for the multi-jet + MJ(Sigma) stream with the MJ(Sigma)>340 GeV signal region selection, other than the final MET/sqrt(HT) requirement. There is a minimum multiplicity requirement of nine for the PTmin=50 GeV, R=0.4 jets.

MET/sqrt(HT) distributions for the multi-jet + MJ(Sigma) stream with the MJ(Sigma)>340 GeV signal region selection, other than the final MET/sqrt(HT) requirement. There is a minimum multiplicity requirement of ten for the PTmin=50 GeV, R=0.4 jets.

MET/sqrt(HT) distributions for the multi-jet + MJ(Sigma) stream with the MJ(Sigma)>420 GeV signal region selection, other than the final MET/sqrt(HT) requirement. There is a minimum multiplicity requirement of eight for the PTmin=50 GeV, R=0.4 jets.

MET/sqrt(HT) distributions for the multi-jet + MJ(Sigma) stream with the MJ(Sigma)>420 GeV signal region selection, other than the final MET/sqrt(HT) requirement. There is a minimum multiplicity requirement of nine for the PTmin=50 GeV, R=0.4 jets.

MET/sqrt(HT) distributions for the multi-jet + MJ(Sigma) stream with the MJ(Sigma)>420 GeV signal region selection, requirement. There is a minimum multiplicity requirement of ten for the PTmin=50 GeV, R=0.4 jets.

Expected exclusion limit at 95% CL in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the sbottom pair production scenario.

Upper 1-sigma expected exclusion limit at 95% CL in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the sbottom pair production scenario.

Lower 1-sigma expected exclusion limit at 95% CL in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the sbottom pair production scenario.

Observed exclusion limit at 95% CL in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario.

Observed exclusion limit at 95% CL, when moving the nominal signal cross section up by the 1-sigma theoretical uncertainty, in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario.

Observed exclusion limit at 95% CL, when moving the nominal signal cross section down by the 1-sigma theoretical uncertainty, in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario.

Expected exclusion limit at 95% CL in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario.

Upper 1-sigma expected exclusion limit at 95% CL in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario.

Lower 1-sigma expected exclusion limit at 95% CL in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario.

Observed exclusion limit at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO) = 150 GEV for the stop pair production scenario.

Observed exclusion limit at 95% CL, when moving the nominal signal cross section up by the 1-sigma theoretical uncertainty, in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO) = 150 GEV for the stop pair production scenario.

Observed exclusion limit at 95% CL, when moving the nominal signal cross section down by the 1-sigma theoretical uncertainty, in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO) = 150 GEV for the stop pair production scenario.

Expected exclusion limit at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO) = 150 GEV for the stop pair production scenario.

Upper 1-sigma expected exclusion limit at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO) = 150 GEV for the stop pair production scenario.

Lower 1-sigma expected exclusion limit at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO) = 150 GEV for the stop pair production scenario.

Observed exclusion limit at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario.

Observed exclusion limit at 95% CL, when moving the nominal signal cross section up by the 1-sigma theoretical uncertainty, in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario.

Observed exclusion limit at 95% CL, when moving the nominal signal cross section down by the 1-sigma theoretical uncertainty, in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario.

Expected exclusion limit at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario.

Upper 1-sigma expected exclusion limit at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario.

Lower 1-sigma expected exclusion limit at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario.

Observed exclusion limit at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario.

Observed exclusion limit at 95% CL, when moving the nominal signal cross section up by the 1-sigma theoretical uncertainty, in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario.

Observed exclusion limit at 95% CL, when moving the nominal signal cross section down by the 1-sigma theoretical uncertainty, in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario.

Expected exclusion limit at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario.

Upper 1-sigma expected exclusion limit at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario.

Lower 1-sigma expected exclusion limit at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario.

Signal region (SR) providing the best expected sensitivity in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the sbottom pair production scenario. In the case of SRA, the number shown represents the contransverse mass, M(CT), threshold used.

Nominal observed excluded cross sections at 95% CL in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the sbottom pair production scenario, once corrected by the luminosity and the efficiency times acceptance of the model itself.

Impact of reducing the branching ratios of SBOTTOM --> BOTTOM NEUTRALINO, assuming no sensitivity to the other decay possibilities, in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the sbottom pair production scenario. The numbers represent the maximum branching ratio excluded at 95% CL, taking the nominal cross section as reference.

Signal region (SR) providing the best expected sensitivity in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario. In the case of SRA, the number shown represents the contransverse mass, M(CT), threshold used.

Signal region (SR) providing the best expected sensitivity in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario. In the case of SRA, the number shown represents the contransverse mass, M(CT), threshold used.

Signal region (SR) providing the best expected sensitivity in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario. In the case of SRA, the number shown represents the contransverse mass, M(CT), threshold used.

Nominal observed excluded cross sections at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario, once corrected by the luminosity and the efficiency times acceptance of the model itself.

Nominal observed excluded cross sections at 95% CL in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario, once corrected by the luminosity and the efficiency times acceptance of the model itself.

Nominal observed excluded cross sections at 95% CL in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario, once corrected by the luminosity and the efficiency times acceptance of the model itself.

Expected CLs values in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the sbottom pair production scenario.

Observed CLs values in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the sbottom pair production scenario.

Sbottom signal production cross sections in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane. These values are also used for the stop case since the differences in cross sections for these processes are negligible.

Relative theoretical uncertainties in percent on the sbottom signal production cross sections in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane coming from the usage of different PDF sets and renormalisation and factorisation scales. These values are also used for the stop case since the differences in cross sections for these processes are negligible.

Total number of generated MC events for the sbottom signal grid in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane.

Signal acceptance in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the sbottom pair production scenario. The best expected signal region selection is used per point.

Signal efficiency times acceptance in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the sbottom pair production scenario. The best expected signal region selection is used per point.

Total experimental systematic uncertainty in percent on the signal efficiency times acceptance in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the sbottom pair production scenario. All the different "up" values have been added in quadrature. The best expected signal region selection is used per point.

Total experimental systematic uncertainty in percent on the signal efficiency times acceptance in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the sbottom pair production scenario. All the different "down" values have been added in quadrature. The best expected signal region selection is used per point.

Expected CLs values in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario.

Expected CLs values in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario.

Expected CLs values in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario.

Observed CLs values in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario.

Observed CLs values in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario.

Observed CLs values in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario.

Total number of generated MC events for the stop signal grid in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV.

Signal acceptance in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario. The best expected signal region selection is used per point.

Signal efficiency times acceptance in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario. The best expected signal region selection is used per point.

Total experimental systematic uncertainty in percent on the signal efficiency times acceptance in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario. All the different "up" values have been added in quadrature. The best expected signal region selection is used per point.

Total experimental systematic uncertainty in percent on the signal efficiency times acceptance in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 5 GEV for the stop pair production scenario. All the different "down" values have been added in quadrature. The best expected signal region selection is used per point.

.

Signal acceptance in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario. The best expected signal region selection is used per point.

Signal efficiency times acceptance in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario. The best expected signal region selection is used per point.

Total experimental systematic uncertainty in percent on the signal efficiency times acceptance in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario. All the different "up" values have been added in quadrature. The best expected signal region selection is used per point.

Total experimental systematic uncertainty in percent on the signal efficiency times acceptance in the ( M(STOP), M(NEUTRALINO) ) mass plane with M(CHARGINO)-M(NEUTRALINO) = 20 GEV for the stop pair production scenario. All the different "down" values have been added in quadrature. The best expected signal region selection is used per point.

Total number of generated MC events for the stop signal grid in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV.

Signal acceptance in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario. The best expected signal region selection is used per point.

Signal efficiency times acceptance in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario. The best expected signal region selection is used per point.

Total experimental systematic uncertainty in percent on the signal efficiency times acceptance in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario. All the different "up" values have been added in quadrature. The best expected signal region selection is used per point.

Total experimental systematic uncertainty in percent on the signal efficiency times acceptance in the ( M(CHARGINO), M(NEUTRALINO) ) mass plane with M(STOP) = 300 GEV for the stop pair production scenario. All the different "down" values have been added in quadrature. The best expected signal region selection is used per point.

Measured differential cross sections as function of the lepton pseudo-rapidity of the production of a W boson with a D meson or a D* meson times the branching ratio W -> l nu in the fiducial regions together with the statistical and systematic uncertainties. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events.

Measured cross section ratios of the production of a W boson with a D meson or a D* meson and the inclusive production of a W boson in the fiducial regions together with the statistical and systematic uncertainties. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events.

Measured differential cross section ratios of the production of a W boson with a D meson or a D* meson and the inclusive production of a W boson in the fiducial regions as function of the D/D* meson pT together with the statistical and systematic uncertainties. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events.

Measured integrated cross sections of the production of a W boson in association with a single c-jet and exactly zero or one additional non-c-jets times the branching ratio W -> l nu in the fiducial regions together with the statistical and systematic uncertainties. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. The cross sections are defined for OS-SS events.

Measured integrated cross sections ratio of the production of a W+ and W- bosons in association with a single c-jet and exactly zero or one additional non-c-jets in the fiducial regions together with the statistical and systematic uncertainties. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. The cross sections are defined for OS-SS events.

Measured integrated cross sections of the production of a W boson in association with a single c-jet decaying into a soft muon in the fiducial regions together with the statistical and systematic uncertainties. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. Soft muons are associated to c-jets within a cone of DeltaR<0.5. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events.

Correlation matrix corresponding to the total uncertainties of measured integrated cross sections of the production of a W boson with a single c-jet, a D meson or a D* meson times the branching ratio W -> l nu in the fiducial regions.

Systematic uncertainties after the averaging procedure of the inclusive cross sections in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels. The luminosity is included in these correlated systematic uncertainties.

Systematic uncertainties after the averaging procedure of the differential cross sections as function of the lepton pseudo-rapidity in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels and bins. The luminosity is included in these correlated systematic uncertainties. The systematic uncertainties for the W+ + cbar-jet channel are shown in this table.

Systematic uncertainties after the averaging procedure of the differential cross sections as function of the lepton pseudo-rapidity in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels and bins. The luminosity is included in these correlated systematic uncertainties. The systematic uncertainties for the W- + c-jet channel are shown in this table.

Systematic uncertainties after the averaging procedure of the differential cross sections as function of the lepton pseudo-rapidity in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels and bins. The luminosity is included in these correlated systematic uncertainties. The systematic uncertainties for the W+ D- and W- D+ channels are shown in this table.

Systematic uncertainties after the averaging procedure of the differential cross sections as function of the lepton pseudo-rapidity in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels and bins. The luminosity is included in these correlated systematic uncertainties. The systematic uncertainties for the W+ D*- and W- D*+ channels are shown in this table.

Theoretical Predictions for the integrated cross section of the production of W+ and W- bosons associated with a single c-jet, a D meson or a D* meson in the fiducial regions together with the statistical and systematic uncertainties. For the W+c-jet cross sections events with more than one c-jet are discarded. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events. The predictions have been obtained the aMC@NLO MC simulation interfaced to the Herwig++ parton shower programme. The uncertainties on the predictions entail PDF uncertainties, parton shower, fragmentation and scale uncertainties. The predictions are reweighted using LHAPDF from the CT10nlo PDF set to the following PDF sets with the LHAPDF IDs given in brackets: CT10nlo (11000), MSTW2008nlo68cl (21100), NNPDF23_nlo_as_0119 (230000), NNPDF23_nlo_collider_as_0119 (236000), HERAPDF15NLO (EIG+VAR, 60700+60730), ATLAS-epWZ12 (EIG+VAR, 65000+65040).

PDF uncertainty for each of the used PDF sets as well as the combined parton shower, fragmentation and scale uncertainties (given in percent) for the theoretical Predictions for the integrated cross section of the production of W+ and W- bosons associated with a single c-jet, a D meson or a D* meson in the fiducial regions together with the statistical and systematic uncertainties. If added quadratically, these uncertainties represent the total uncertainty on the quoted theory prediction. For the W+c-jet cross sections events with more than one c-jet are discarded. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events. The predictions have been obtained the aMC@NLO MC simulation interfaced to the Herwig++ parton shower programme. The uncertainties on the predictions entail PDF uncertainties, FSR uncertainties and scale uncertainties. The predictions are reweighted using LHAPDF from the CT10nlo PDF set to the following PDF sets with the LHAPDF IDs given in brackets: CT10nlo (11000), MSTW2008nlo68cl (21100), NNPDF23_nlo_as_0119 (230000), NNPDF23_nlo_collider_as_0119 (236000), HERAPDF15NLO (EIG+VAR, 60700+60730), ATLAS-epWZ12 (EIG+VAR, 65000+65040). The determination of the parton shower, fragmentation and scale uncertainties is detailed in the paper.

Normalized ZZ fiducial cross section (multiplied by 10^6 for readability) in bins of the dilepton pT for the 2l2nu channel. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties.

Normalized ZZ fiducial cross section (multiplied by 10^6 for readability) in bins of deltaPhi between the two leptons of the leading dileptons for the 4l channel. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties. UPDATE (30 APR 2014): extra significant digit added for first bin.

Normalized ZZ fiducial cross section (multiplied by 10^6 for readability) in bins of deltaPhi between the two leptons for the 2l2nu channel. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties.

Normalized ZZ fiducial cross section (multiplied by 10^6 for readability) in bins of the mass of the ZZ system for the 4l channel. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties.

Normalized ZZ fiducial cross section (multiplied by 10^6 for readability) in bins of the transverse mass of the ZZ system for the 2l2nu channel. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties.

Unfolded normalised differential Z+2j cross section as a function of the rapidity separation between the leading jets in the search region.

Unfolded normalised differential cross section distribution as a function of the number of jets in the rapidity interval between the two leading jets in the high mass region.

Unfolded normalised differential cross section distribution as a function of the normalised transverse momentum balance in the high mass region.

Unfolded normalised differential cross section distribution as a function of the azimuthal angle between the two leading jets in the high mass region.

Unfolded jet veto efficiency as a function of the dijet invariant mass in the baseline region.

Unfolded jet veto efficiency as a function of the rapidity separation between the two leading jets in the baseline region.

Unfolded average number of jets in the rapidity interval between the two leading jets as a function of the dijet invariant mass in the baseline region.

Unfolded average number of jets in the rapidity interval between the two leading jets as a function of the rapidity separation between the two leading jets in the baseline region.

Unfolded transverse momentum balance veto efficiency as a function of the dijet invariant mass in the baseline region.

Unfolded transverse momentum balance veto efficiency as a function of the rapidity separation between the two leading jets in the baseline region.

Unfolded normalised differential Z+2j cross section as a function of dijet invariant mass in the high-pt region.

Unfolded normalised differential Z+2j cross section as a function of dijet invariant mass in the control region.

Unfolded normalised differential Z+2j cross section as a function of the rapidity separation between the leading jets in the high-pt region.

Unfolded normalised differential Z+2j cross section as a function of the rapidity separation between the leading jets in the control region.

Unfolded jet veto efficiency as a function of the dijet invariant mass in the high-pt region.

Unfolded jet veto efficiency as a function of the rapidity separation between the two leading jets in the high-pt region.

Unfolded average number of jets in the rapidity interval between the two leading jets as a function of the dijet invariant mass in the high-pt region.

Unfolded average number of jets in the rapidity interval between the two leading jets as a function of the rapidity separation between the two leading jets in the high-pt region.

Unfolded transverse momentum balance veto efficiency as a function of the dijet invariant mass in the high-pt region.

Unfolded transverse momentum balance veto efficiency as a function of the rapidity separation between the two leading jets in the high-pt region.

Observed CLs contour with plus 1-sigma signal cross-section uncertainty in the ( M(CHARGINO), TAU(CHARGINO) ) space for tan(beta) = 5 and mu > 0.

Expected CLs contour in the ( M(CHARGINO), TAU(CHARGINO) ) space for tan(beta) = 5 and mu > 0.

Expected CLs contour with minus 1-sigma experimental uncertainty in the ( M(CHARGINO), TAU(CHARGINO) ) space for tan(beta) = 5 and mu > 0.

Expected CLs contour with plus 1-sigma experimental uncertainty in the ( M(CHARGINO), TAU(CHARGINO) ) space for tan(beta) = 5 and mu > 0.

Observed CLs contour in the ( M(CHARGINO), M(CHARGINO)-M(NEUTRALINO) ) space of the AMSB model for tan(beta) = 5 and mu > 0.

Observed CLs contour with minus 1-sigma signal cross-section uncertainty in the ( M(CHARGINO), M(CHARGINO)-M(NEUTRALINO) ) space of the AMSB model for tan(beta) = 5 and mu > 0.

Observed CLs contour with plus 1-sigma signal cross-section uncertainty in the ( M(CHARGINO), M(CHARGINO)-M(NEUTRALINO) ) space of the AMSB model for tan(beta) = 5 and mu > 0.

Expected CLs contour in the ( M(CHARGINO), M(CHARGINO)-M(NEUTRALINO) ) space of the AMSB model for tan(beta) = 5 and mu > 0.

Expected CLs contour with minus 1-sigma experimental uncertainty in the ( M(CHARGINO), M(CHARGINO)-M(NEUTRALINO) ) space of the AMSB model for tan(beta) = 5 and mu > 0.

Expected CLs contour with plus 1-sigma experimental uncertainty in the ( M(CHARGINO), M(CHARGINO)-M(NEUTRALINO) ) space of the AMSB model for tan(beta) = 5 and mu > 0.

Acceptance (A), efficiency (EPSILON), cross-section (SIG) and limits in number of events for the excited quark benchmark model, as a function of the signal mass M(q*). Uncertainties on the cross section are on the order of 1%. The limits include statistical uncertainties only. Expected limits include the 68% uncertainty band. Acceptance was calculated using parton-level quantities by imposing criteria that apply directly to kinematic selections (photon/jet |eta|, photon/jet transverse momentum, Delta(eta), Delta(R)). All other selections, which in general correspond to event and object quality criteria, were used to calculate the efficiency based on the events included in the acceptance.

Normalised fiducial cross section in bins of the leading lepton PT. Leading Lepton is the lepton in the final state with highest PT.

Correlations in the leading Lepton PT distribution.

Experimental cross-section values per bin in PB for COS(THETA*(2GAMMA)).

Observed 95 PCT exclusion limit in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

Expected 95 PCT exclusion limit in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

Observed 95 PCT exclusion limit in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

Number of MC signal events in the M(stop), M(neutralino) plane in gaugino universality scenario.

Number of MC signal events in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

Number of MC signal events in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

Cross section in the M(stop), M(neutralino) plane in gaugino universality scenario.

Cross section in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

Cross section in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

Acceptance in the 1LSR signal region in the M(stop), M(neutralino) plane in gaugino universality scenario.

Acceptance in the 1LSR signal region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

Efficiency in the 1LSR signal region in the M(stop), M(neutralino) plane in gaugino universality scenario.

Efficiency in the 1LSR signal region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

Total PCT systematic uncertainty in the 1LSR region in the M(stop), M(neutralino) plane in gaugino universality scenario.

Total PCT systematic uncertainty in the 1LSR region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

Acceptance in the 2LSR1 signal region in the M(stop), M(neutralino) plane in gaugino universality scenario.

Acceptance in the 2LSR2 signal region in the M(stop), M(neutralino) plane in gaugino universality scenario.

Efficiency in the 2LSR1 signal region in the M(stop), M(neutralino) plane in gaugino universality scenario.

Efficiency in the 2LSR2 signal region in the M(stop), M(neutralino) plane in gaugino universality scenario.

Total PCT systematic uncertainty in the 2LSR1 region in the M(stop), M(neutralino) plane in gaugino universality scenario.

Total PCT systematic uncertainty in the 2LSR2 region in the M(stop), M(neutralino) plane in gaugino universality scenario.

Acceptance in the 2LSR1 signal region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

Acceptance in the 2LSR2 signal region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

Efficiency in the 2LSR1 signal region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

Efficiency in the 2LSR2 signal region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

Total PCT systematic uncertainty in the 2LSR1 region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

Total PCT systematic uncertainty in the 2LSR2 region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

Acceptance in the 2LSR1 signal region in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

Acceptance in the 2LSR2 signal region in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

Efficiency in the 2LSR1 signal region in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

Efficiency in the 2LSR2 signal region in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

Total PCT systematic uncertainty in the 2LSR1 region in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

Total PCT systematic uncertainty in the 2LSR2 region in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

expected CLs values for the 1LSR region in the M(stop), M(neutralino) plane in gaugino universality scenario.

observed CLs values for the 1LSR region in the M(stop), M(neutralino) plane in gaugino universality scenario.

expected CLs values for the 2LSR1 region in the M(stop), M(neutralino) plane in gaugino universality scenario.

observed CLs values for the 2LSR1 region in the M(stop), M(neutralino) plane in gaugino universality scenario.

expected CLs values for the 2LSR2 region in the M(stop), M(neutralino) plane in gaugino universality scenario.

observed CLs values for the 2LSR2 region in the M(stop), M(neutralino) plane in gaugino universality scenario.

expected CLs values combining the 1LSR and 2LSR1 regions in the M(stop), M(neutralino) plane in gaugino universality scenario.

observed CLs values combining the 1LSR and 2LSR1 regions in the M(stop), M(neutralino) plane in gaugino universality scenario.

expected CLs values combining the 1LSR and 2LSR2 regions in the M(stop), M(neutralino) plane in gaugino universality scenario.

observed CLs values combining the 1LSR and 2LSR2 regions in the M(stop), M(neutralino) plane in gaugino universality scenario.

expected CLs values for the best expected combination in the M(stop), M(neutralino) plane in gaugino universality scenario.

observed CLs values for the best expected combination in the M(stop), M(neutralino) plane in gaugino universality scenario.

expected CLs values for the 1LSR region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

observed CLs values for the 1LSR region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

expected CLs values for the 2LSR1 region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

observed CLs values for the 2LSR1 region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

expected CLs values for the 2LSR2 region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

observed CLs values for the 2LSR2 region in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

expected CLs values combining the 1LSR and 2LSR1 regions in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

observed CLs values combining the 1LSR and 2LSR1 regions in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

expected CLs values combining the 1LSR and 2LSR2 regions in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

observed CLs values combining the 1LSR and 2LSR2 regions in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

expected CLs values for the best expected combination in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

observed CLs values for the best expected combination in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.

expected CLs values for the 2LSR1 region in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

observed CLs values for the 2LSR1 region in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

expected CLs values for the 2LSR2 region in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

observed CLs values for the 2LSR2 region in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

expected CLs values for the best expected combination in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.

observed CLs values for the best expected combination in the M(stop), M(neutralino) plane in the scenario where M(chargino) = 106 GEV.