Target asymmetry T, recoil asymmetry P, and polarization observable H for $\gamma n \to \eta n$ as a function of the polar center-of-mass angle for bins at the given centroid c.m. energies.

Comparison between data and MC simulation for kinematic distributions based on events in the signal candidate sample for \Delta|y|. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC

Comparison between data and MC simulation for \Delta|y| for each of the 12 analysis channels for the low mass region prior to maximum likelihood fit. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC

Comparison between data and MC simulation for \Delta|y| for each of the 12 analysis channels for the low mass region after the maximum likelihood fit. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC

Comparison between data and MC simulation for \Delta|y| for each of the 12 analysis channels for the high mass region prior to the maximum likelihood fit. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC

Comparison between data and MC simulation for \Delta|y| for each of the 12 analysis channels for the high mass region after the maximum likelihood fit. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC

Measured A_{C}^{fid} in different mass regions after combining the two lepton channels. The vertical bars on the points show the statistical uncertainty in the data

Measured A_{C} in the full phase space in different mass regions after combining the two lepton channels. The vertical bars on the points show the statistical uncertainty in the data

The +/- standard deviation (\sigma) impacts of the nuisance parameters corresponding to the systematic uncertainties in the full phase space A_{C} measurement for mttbar > 750GeV. The red and blue bars show the effect on the unfolded AC values for up and down variations of the systematic uncertainty. The MC statistical uncertainties are omitted here.

The unfolded differential charge asymmetry as a function of the transverse momentum of the top pair system. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature.

The unfolded differential charge asymmetry as a function of the longitudinal boost of the top pair system. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature.

The unfolded inclusive leptonic asymmetry. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

The unfolded differential leptonic asymmetry as a function of the invariant mass of the di-lepton pair. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

The unfolded differential leptonic asymmetry as a function of the transverse momentum of the di-lepton pair. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

The unfolded differential leptonic asymmetry as a function of the longitudinal boost of the di-lepton pair. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

Individual 68% and 95% CL bounds on the relevant Wilson coefficients of the SM Effective Field Theory in units of $\text{TeV}^{-2}$. The bounds are derived from the $A_C^{t\bar{t}}$ inclusive measurement. The experimental uncertainties are accounted for, in the form of the complete covariance matrix that keeps track of correlations between bins for the differential measurement. The theory uncertainty from the NNLO QCD + NLO EW calculation is included by explicitly varying the renormalization and factorization scales, or the parton density functions, in the calculation and registering the variations in the intervals.

Individual 68% and 95% CL bounds on the relevant Wilson coefficients of the SM Effective Field Theory in units of $\text{TeV}^{-2}$. The bounds are derived from the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement. The experimental uncertainties are accounted for, in the form of the complete covariance matrix that keeps track of correlations between bins for the differential measurement. The theory uncertainty from the NNLO QCD + NLO EW calculation is included by explicitly varying the renormalization and factorization scales, or the parton density functions, in the calculation and registering the variations in the intervals.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ inclusive measurement. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0,0.3]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0.3,0.6]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0.6,0.8]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0.8,1]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ < 500 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ $\in$ [500,750] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ $\in$ [750,1000] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ $\in$ [1000,1500] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ > 1500 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement for $p_{T,t\bar{t}}$ < 30 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement for $p_{T,t\bar{t}}$ $\in$ [30,120] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement for $p_{T,t\bar{t}}$ > 120 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ inclusive measurement. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0,0.3]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0.3,0.6]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0.6,0.8]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0.8,1]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ < 200 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ $\in$ [200,300] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ $\in$ [300,400] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ > 400 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement for $p_{T,\ell\bar{\ell}}$ < 20 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement for $p_{T,\ell\bar{\ell}}$ $\in$ [20, 70] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement for $p_{T,\ell\bar{\ell}}$ > 70 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ inclusive measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ inclusive measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Covariance matrix for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement.

Covariance matrix for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement.

Covariance matrix for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement.

Covariance matrix for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement.

Covariance matrix for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement.

Covariance matrix for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement.

Photon beam asymmetry Sigma at W=1.2254987 GeV

Photon beam asymmetry Sigma at W=1.2290003 GeV

Photon beam asymmetry Sigma at W=1.2324995 GeV

Photon beam asymmetry Sigma at W=1.2355029 GeV

Photon beam asymmetry Sigma at W=1.2389989 GeV

Photon beam asymmetry Sigma at W=1.2425001 GeV

Photon beam asymmetry Sigma at W=1.2455020 GeV

Photon beam asymmetry Sigma at W=1.2484967 GeV

Photon beam asymmetry Sigma at W=1.2514991 GeV

Photon beam asymmetry Sigma at W=1.2550029 GeV

Photon beam asymmetry Sigma at W=1.2584969 GeV

Photon beam asymmetry Sigma at W=1.2614979 GeV

Photon beam asymmetry Sigma at W=1.2644992 GeV

Photon beam asymmetry Sigma at W=1.2675008 GeV

Photon beam asymmetry Sigma at W=1.2705027 GeV

Photon beam asymmetry Sigma at W=1.2739984 GeV

Photon beam asymmetry Sigma at W=1.2774992 GeV

Photon beam asymmetry Sigma at W=1.2804996 GeV

Photon beam asymmetry Sigma at W=1.2835003 GeV

Photon beam asymmetry Sigma at W=1.2864940 GeV

Photon beam asymmetry Sigma at W=1.2895026 GeV

Photon beam asymmetry Sigma at W=1.2924970 GeV

Photon beam asymmetry Sigma at W=1.2954989 GeV

Photon beam asymmetry Sigma at W=1.2989995 GeV

Photon beam asymmetry Sigma at W=1.3024980 GeV

Photon beam asymmetry Sigma at W=1.3054984 GeV

Photon beam asymmetry Sigma at W=1.3084992 GeV

Photon beam asymmetry Sigma at W=1.3115002 GeV

Photon beam asymmetry Sigma at W=1.3145016 GeV

Photon beam asymmetry Sigma at W=1.3175032 GeV

Photon beam asymmetry Sigma at W=1.3204980 GeV

Photon beam asymmetry Sigma at W=1.3235001 GeV

Photon beam asymmetry Sigma at W=1.3265026 GeV

Photon beam asymmetry Sigma at W=1.3294983 GeV

Photon beam asymmetry Sigma at W=1.3325013 GeV

Photon beam asymmetry Sigma at W=1.3354976 GeV

Photon beam asymmetry Sigma at W=1.3385012 GeV

Photon beam asymmetry Sigma at W=1.3414981 GeV

Photon beam asymmetry Sigma at W=1.3445022 GeV

Photon beam asymmetry Sigma at W=1.3474997 GeV

Photon beam asymmetry Sigma at W=1.3504974 GeV

Photon beam asymmetry Sigma at W=1.3535024 GeV

Photon beam asymmetry Sigma at W=1.3565007 GeV

Photon beam asymmetry Sigma at W=1.3594993 GeV

Photon beam asymmetry Sigma at W=1.3624982 GeV

Photon beam asymmetry Sigma at W=1.3654974 GeV

Photon beam asymmetry Sigma at W=1.3684968 GeV

Photon beam asymmetry Sigma at W=1.3714966 GeV

Photon beam asymmetry Sigma at W=1.3744966 GeV

Photon beam asymmetry Sigma at W=1.3774969 GeV

Photon beam asymmetry Sigma at W=1.3804974 GeV

Photon beam asymmetry Sigma at W=1.3834983 GeV

Photon beam asymmetry Sigma at W=1.3864994 GeV

Photon beam asymmetry Sigma at W=1.3890010 GeV

Photon beam asymmetry Sigma at W=1.3914981 GeV

Photon beam asymmetry Sigma at W=1.3945022 GeV

Photon beam asymmetry Sigma at W=1.3974998 GeV

Photon beam asymmetry Sigma at W=1.4004978 GeV

Photon beam asymmetry Sigma at W=1.4035026 GeV

Photon beam asymmetry Sigma at W=1.4065011 GeV

Photon beam asymmetry Sigma at W=1.4094998 GeV

Photon beam asymmetry Sigma at W=1.4119939 GeV

Photon beam asymmetry Sigma at W=1.4144969 GeV

Photon beam asymmetry Sigma at W=1.4174985 GeV

Photon beam asymmetry Sigma at W=1.4205005 GeV

Photon beam asymmetry Sigma at W=1.4235027 GeV

Photon beam asymmetry Sigma at W=1.4259986 GeV

Photon beam asymmetry Sigma at W=1.4284967 GeV

Photon beam asymmetry Sigma at W=1.4315018 GeV

Photon beam asymmetry Sigma at W=1.4345006 GeV

Photon beam asymmetry Sigma at W=1.4374997 GeV

Photon beam asymmetry Sigma at W=1.4399974 GeV

Photon beam asymmetry Sigma at W=1.4424973 GeV

Photon beam asymmetry Sigma at W=1.4454993 GeV

Photon beam asymmetry Sigma at W=1.4485015 GeV

Differential cross section at W=1.0813873 GeV

Differential cross section at W=1.0834244 GeV

Differential cross section at W=1.0854490 GeV

Differential cross section at W=1.0874871 GeV

Differential cross section at W=1.0895214 GeV

Differential cross section at W=1.0915347 GeV

Differential cross section at W=1.0935786 GeV

Differential cross section at W=1.0956101 GeV

Differential cross section at W=1.0976464 GeV

Differential cross section at W=1.0996192 GeV

Differential cross section at W=1.1016993 GeV

Differential cross section at W=1.1037073 GeV

Differential cross section at W=1.1057288 GeV

Differential cross section at W=1.1077549 GeV

Differential cross section at W=1.1097605 GeV

Differential cross section at W=1.1117962 GeV

Differential cross section at W=1.1137946 GeV

Differential cross section at W=1.1158229 GeV

Differential cross section at W=1.1178392 GeV

Differential cross section at W=1.1198602 GeV

Differential cross section at W=1.1218776 GeV

Differential cross section at W=1.1238330 GeV

Differential cross section at W=1.1258932 GeV

Differential cross section at W=1.1278915 GeV

Differential cross section at W=1.1299029 GeV

Differential cross section at W=1.1339149 GeV

Differential cross section at W=1.1359156 GeV

Photon beam asymmetry Sigma at W=1.0752268 GeV

Photon beam asymmetry Sigma at W=1.0773190 GeV

Photon beam asymmetry Sigma at W=1.0793464 GeV

Photon beam asymmetry Sigma at W=1.0813873 GeV

Photon beam asymmetry Sigma at W=1.0834244 GeV

Photon beam asymmetry Sigma at W=1.0854490 GeV

Photon beam asymmetry Sigma at W=1.0874871 GeV

Photon beam asymmetry Sigma at W=1.0895214 GeV

Photon beam asymmetry Sigma at W=1.0915347 GeV

Photon beam asymmetry Sigma at W=1.0935786 GeV

Photon beam asymmetry Sigma at W=1.0956101 GeV

Photon beam asymmetry Sigma at W=1.0976464 GeV

Photon beam asymmetry Sigma at W=1.0996192 GeV

Photon beam asymmetry Sigma at W=1.1016993 GeV

Photon beam asymmetry Sigma at W=1.1037073 GeV

Photon beam asymmetry Sigma at W=1.1057288 GeV

Photon beam asymmetry Sigma at W=1.1077549 GeV

Photon beam asymmetry Sigma at W=1.1097605 GeV

Photon beam asymmetry Sigma at W=1.1117962 GeV

Photon beam asymmetry Sigma at W=1.1137946 GeV

Photon beam asymmetry Sigma at W=1.1158229 GeV

Photon beam asymmetry Sigma at W=1.1178392 GeV

Photon beam asymmetry Sigma at W=1.1198602 GeV

Photon beam asymmetry Sigma at W=1.1218776 GeV

Photon beam asymmetry Sigma at W=1.1238330 GeV

Photon beam asymmetry Sigma at W=1.1258932 GeV

Photon beam asymmetry Sigma at W= 1.3147 GeV

Photon beam asymmetry Sigma at W= 1.3289 GeV

Photon beam asymmetry Sigma at W= 1.3430 GeV

Photon beam asymmetry Sigma at W= 1.3569 GeV

Photon beam asymmetry Sigma at W= 1.3707 GeV

Photon beam asymmetry Sigma at W= 1.3843 GeV

Photon beam asymmetry Sigma at W= 1.3978 GeV

Photon beam asymmetry Sigma at W= 1.4112 GeV

Photon beam asymmetry Sigma at W= 1.4244 GeV

Target asymmetry T for c.m. cos(Theta_pi0)= 0.819

Target asymmetry T for c.m. cos(Theta_pi0)= 0.707

Target asymmetry T for c.m. cos(Theta_pi0)= 0.574

Target asymmetry T for c.m. cos(Theta_pi0)= 0.423

Target asymmetry T for c.m. cos(Theta_pi0)= 0.259

Target asymmetry T for c.m. cos(Theta_pi0)= 0.087

Target asymmetry T for c.m. cos(Theta_pi0)= -0.087

Target asymmetry T for c.m. cos(Theta_pi0)= -0.259

Target asymmetry T for c.m. cos(Theta_pi0)= -0.423

Target asymmetry T for c.m. cos(Theta_pi0)= -0.574

Target asymmetry T for c.m. cos(Theta_pi0)= -0.707

Target asymmetry T for c.m. cos(Theta_pi0)= -0.819

Target asymmetry T for c.m. cos(Theta_pi0)= -0.906

Target asymmetry T for c.m. cos(Theta_pi0)= -0.966

Target asymmetry T for c.m. cos(Theta_pi0)= -0.996

The fraction of photon-induced background as compared with the total amount of DY signal plus photon-induced events ($N_{\gamma\gamma}/(N_{\gamma\gamma} + N_\mathrm{DY})$) in different dilepton mass bins. These numbers are averaged across the different years and channels.

Exclusion limits at 95% CL on the coupling K_L for a Z' in the sequential standard model as a function of the Z' mass.