Inclusive Jet Cross Section for |rapidity| 1.5 TO 2.0 as a function of the jet transverse momentum. The (sys) error is the total systematic error, including the luminosity uncertainty of 2.2%.

Inclusive Jet Cross Section for |rapidity| 2.0 TO 2.5 as a function of the jet transverse momentum. The (sys) error is the total systematic error, including the luminosity uncertainty of 2.2%.

DiJet Cross Section for |rapidity| < 0.5 as a function of the dijet invariant mass. The (sys) error is the total systematic error, including the luminosity uncertainty of 2.2%.

DiJet Cross Section for |rapidity| 0.5 TO 1.0 as a function of the dijet invariant mass. The (sys) error is the total systematic error, including the luminosity uncertainty of 2.2%.

DiJet Cross Section for |rapidity| 1.0 TO 1.5 as a function of the dijet invariant mass. The (sys) error is the total systematic error, including the luminosity uncertainty of 2.2%.

DiJet Cross Section for |rapidity| 1.5 TO 2.0 as a function of the dijet invariant mass. The (sys) error is the total systematic error, including the luminosity uncertainty of 2.2%.

DiJet Cross Section for |rapidity| 2.0 TO 2.5 as a function of the dijet invariant mass. The (sys) error is the total systematic error, including the luminosity uncertainty of 2.2%.

Correlation coefficients for the differential cross-section of $Z \to e^+ e^-$ at 7 TeV between bins of $Z$ rapidity, $y_{Z}$. Both statistical and systematic contributions are included.

Correlation coefficients for the differential cross-section of $Z \to e^+ e^-$ at 7 TeV between bins of $\phi^*$. Both statistical and systematic contributions are included.

The measured differential cross sections for $P_T(\gamma\gamma)$ , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for $P_T(\gamma\gamma)$, when $P_T(\gamma\gamma) > M(\gamma\gamma)$ , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for $P_T(\gamma\gamma)$, when $P_T(\gamma\gamma) < M(\gamma\gamma)$ , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for $\Delta\Phi(\gamma\gamma)$ , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for $\Delta\Phi(\gamma\gamma)$, when $P_T(\gamma\gamma) > M(\gamma\gamma)$ , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for $\Delta\Phi(\gamma\gamma)$, when $P_T(\gamma\gamma) < M(\gamma\gamma)$ , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for $y(\gamma\gamma)$, the rapidity of the diphoton system , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for $y(\gamma\gamma)$, the rapidity of the diphoton system, when $P_T(\gamma\gamma) > M(\gamma\gamma)$ , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for $y(\gamma\gamma)$, the rapidity of the diphoton system, when $P_T(\gamma\gamma) < M(\gamma\gamma)$ , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for $E_T^{\gamma 2}/E_T^{\gamma 1}$ , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for $E_T^{\gamma 2}/E_T^{\gamma 1}$, when $P_T(\gamma\gamma) > M(\gamma\gamma)$ , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for $E_T^{\gamma 2}/E_T^{\gamma 1}$, when $P_T(\gamma\gamma) < M(\gamma\gamma)$ , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for the cosine of the polar angle of the leading photon in the Collins-Soper frame , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for the cosine of the polar angle of the leading photon in the Collins-Soper frame, when $P_T(\gamma\gamma) > M(\gamma\gamma)$ , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for the cosine of the polar angle of the leading photon in the Collins-Soper frame, when $P_T(\gamma\gamma) < M(\gamma\gamma)$ , together with the predictions from the Sherpa and NNLO Monte Carlos.

The measured differential cross sections for $\eta_1-\eta_2$, the diffrence in photon pseudorapidities , together with the predictions from the Sherpa Monte Carlo.

The measured differential cross sections for log$_{10}$ ($P_T(\gamma\gamma)/M(\gamma\gamma))$ , together with the predictions from the Sherpa Monte Carlo.

The measured differential cross sections for $\Delta R(\gamma\gamma)$ where $\Delta R(\gamma\gamma)^2 = \Delta \Phi(\gamma\gamma)^2 + (\eta_1-\eta_2)^2$ , together with the predictions from the Sherpa Monte Carlo.

The measured differential cross sections for the photon $E_T$ (two entries per event) , together with the predictions from the Sherpa Monte Carlo.

The measured differential cross sections for the photon $\eta$ (two entries per event) , together with the predictions from the Sherpa Monte Carlo.

Charged energy flow for non-diffractive enriched events, requiring at least one charged particle in the pseudorapidity range -3.5 < eta < -1.5 and at least one charged particle in the pseudorapidity range 1.9 < eta < 4.9.

Total energy flow for inclusive mininum bias events, requiring at least one charged particle in the pseudorapidity range 1.9 < eta < 4.9.

Total energy flow for hard scattering events, requiring at least one charged particle with transverse momentum > 3 GeV and in the pseudorapidity range 1.9 < eta < 4.9.

Total energy flow for diffractive enriched events, requiring no charged particles in the pseudorapidity range -3.5 < eta < -1.5 and at least one charged particle in the pseudorapidity range 1.9 < eta < 4.9.

Total energy flow for non-diffractive enriched events, requiring at least one charged particle in the pseudorapidity range -3.5 < eta < -1.5 and at least one charged particle in the pseudorapidity range 1.9 < eta < 4.9.

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 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.

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.

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).

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.