Signal region detector-level distribution for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$.

Signal region detector-level distribution for the observable $m_{e\mu}$.

Signal region detector-level distribution for the observable $p_{\mathrm{T}}^{e\mu}$.

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|y_{e\mu}|$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|y_{e\mu}|$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|\Delta \phi(e \mu)|$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|\Delta \phi(e \mu)|$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $ \cos\theta^{\ast}$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $ \cos\theta^{\ast}$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $m_{e\mu}$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $m_{e\mu}$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{e\mu}$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{e\mu}$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|y_{e\mu}|$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|y_{e\mu}|$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|\Delta \phi(e \mu)|$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|\Delta \phi(e \mu)|$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $ \cos\theta^{\ast}$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $ \cos\theta^{\ast}$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $m_{e\mu}$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $m_{e\mu}$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{e\mu}$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{e\mu}$

The measured fiducial cross section vs $m(\ell\ell\gamma)$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with Sherpa 2.2.2 at NLO. The uncertainty is defined as Max(stat error, systematic difference between Sherpa LO and Sherpa 2.2.2 NLO), and cannot be considered correlated bin-to-bin. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

The measured fiducial cross section vs $p_{\mathrm{T}}^{\ell\ell\gamma}$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with Sherpa 2.2.2 at NLO. The uncertainty is defined as Max(stat error, systematic difference between Sherpa LO and Sherpa 2.2.2 NLO), and cannot be considered correlated bin-to-bin. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

The measured fiducial cross section vs $\Delta\phi(ll,\gamma)$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with Sherpa 2.2.2 at NLO. The uncertainty is defined as Max(stat error, systematic difference between Sherpa LO and Sherpa 2.2.2 NLO), and cannot be considered correlated bin-to-bin. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

The measured fiducial cross section vs $p_{\mathrm{T}}^{\ell\ell\gamma}/m(\ell\ell\gamma)$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with Sherpa 2.2.2 at NLO. The uncertainty is defined as Max(stat error, systematic difference between Sherpa LO and Sherpa 2.2.2 NLO), and cannot be considered correlated bin-to-bin. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.

Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.

Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.

Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.

Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.

Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.

Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.

Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.

Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.

Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.

Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.

Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.

Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.

Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.

Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.

Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.

Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.

Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.

Measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.

Statistical correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.

Total correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.

Measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.

Statistical correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.

Total correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.

Measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.

Statistical correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.

Total correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.

Measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.

Statistical correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.

Total correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.

Measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.

Statistical correlation between bins in data for the measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.

Total correlation between bins in data for the measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.

Measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.

Statistical correlation between bins in data for the measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.

Total correlation between bins in data for the measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.

List of experimentally considered systematic uncertainties for the WW cross section measurement.

Extrapolated unfolded fiducial cross-section of $WW\rightarrow e\mu$ production as a function of $p_\text{T}^{\text{lead }\ell}$.

Extrapolated unfolded fiducial cross-section of $WW\rightarrow e\mu$ production as a function of $m_{e\mu}$.

Extrapolated unfolded fiducial cross-section of $WW\rightarrow e\mu$ production as a function of $p_{T}^{e\mu}$.

XP distribution at c.m. energy 172.0 GeV.

XP distribution at c.m. energy 183.0 GeV.

XP distribution at c.m. energy 189.0 GeV.

XP distribution at c.m. energy 196.0 GeV.

XP distribution at c.m. energy 200.0 GeV.

XP distribution at c.m. energy 206.0 GeV.

Peak position in XI distribution for different c.m. energies.

XI distribution at c.m. energy 133.0 GeV.

XI distribution at c.m. energy 161.0 GeV.

XI distribution at c.m. energy 172.0 GeV.

XI distribution at c.m. energy 183.0 GeV.

XI distribution at c.m. energy 189.0 GeV.

XI distribution at c.m. energy 196.0 GeV.

XI distribution at c.m. energy 200.0 GeV.

XI distribution at c.m. energy 206.0 GeV.

XE distribution at c.m. energy 133.0 GeV.

XE distribution at c.m. energy 161.0 GeV.

XE distribution at c.m. energy 172.0 GeV.

XE distribution at c.m. energy 183.0 GeV.

XE distribution at c.m. energy 189.0 GeV.

XE distribution at c.m. energy 196.0 GeV.

XE distribution at c.m. energy 200.0 GeV.

XE distribution at c.m. energy 206.0 GeV.

PTIN distribution at c.m. energy 133.0 GeV.

PTIN distribution at c.m. energy 161.0 GeV.

PTIN distribution at c.m. energy 172.0 GeV.

PTIN distribution at c.m. energy 183.0 GeV.

PTIN distribution at c.m. energy 189.0 GeV.

PTIN distribution at c.m. energy 196.0 GeV.

PTIN distribution at c.m. energy 200.0 GeV.

PTIN distribution at c.m. energy 206.0 GeV.

PTOUT distribution at c.m. energy 206.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 133.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 161.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 172.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 183.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 189.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 196.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 200.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 206.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 133.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 161.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 172.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 183.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 189.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 196.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 200.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 206.0 GeV.

Combined results for ALPHAS.

Event shape means.

THRUST distribution at c.m. energy 91.20 GeV.

1-THRUST distribution at c.m. energy 133.00 GeV.

1-THRUST distribution at c.m. energy 161.00 GeV.

1-THRUST distribution at c.m. energy 172.00 GeV.

1-THRUST distribution at c.m. energy 183.00 GeV.

1-THRUST distribution at c.m. energy 189.00 GeV.

1-THRUST distribution at c.m. energy 200.00 GeV.

1-THRUST distribution at c.m. energy 206.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 91.20 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 133.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 161.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 172.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 183.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 189.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 200.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 206.00 GeV.

Total jet broadening distribution at c.m. energy 91.20 GeV.

Total jet broadening distribution at c.m. energy 133.00 GeV.

Total jet broadening distribution at c.m. energy 161.00 GeV.

Total jet broadening distribution at c.m. energy 172.00 GeV.

Total jet broadening distribution at c.m. energy 183.00 GeV.

Total jet broadening distribution at c.m. energy 189.00 GeV.

Total jet broadening distribution at c.m. energy 200.00 GeV.

Total jet broadening distribution at c.m. energy 206.00 GeV.

Wide jet broadening distribution at c.m. energy 91.20 GeV.

Wide jet broadening distribution at c.m. energy 133.00 GeV.

Wide jet broadening distribution at c.m. energy 161.00 GeV.

Wide jet broadening distribution at c.m. energy 172.00 GeV.

Wide jet broadening distribution at c.m. energy 183.00 GeV.

Wide jet broadening distribution at c.m. energy 189.00 GeV.

Wide jet broadening distribution at c.m. energy 200.00 GeV.

Wide jet broadening distribution at c.m. energy 206.00 GeV.

C-PARAMETER distribution at c.m. energy 91.20 GeV.

C-PARAMETER distribution at c.m. energy 133.00 GeV.

C-PARAMETER distribution at c.m. energy 161.00 GeV.

C-PARAMETER distribution at c.m. energy 172.00 GeV.

C-PARAMETER distribution at c.m. energy 183.00 GeV.

C-PARAMETER distribution at c.m. energy 189.00 GeV.

C-PARAMETER distribution at c.m. energy 200.00 GeV.

C-PARAMETER distribution at c.m. energy 206.00 GeV.

Thrust Major distribution at c.m. energy 91.20 GeV.

Thrust Major distribution at c.m. energy 133.00 GeV.

Thrust Major distribution at c.m. energy 161.00 GeV.

Thrust Major distribution at c.m. energy 172.00 GeV.

Thrust Major distribution at c.m. energy 183.00 GeV.

Thrust Major distribution at c.m. energy 189.00 GeV.

Thrust Major distribution at c.m. energy 200.00 GeV.

Thrust Major distribution at c.m. energy 206.00 GeV.

Thrust Minor distribution at c.m. energy 91.20 GeV.

Thrust Minor distribution at c.m. energy 133.00 GeV.

Thrust Minor distribution at c.m. energy 161.00 GeV.

Thrust Minor distribution at c.m. energy 172.00 GeV.

Thrust Minor distribution at c.m. energy 183.00 GeV.

Thrust Minor distribution at c.m. energy 189.00 GeV.

Thrust Minor distribution at c.m. energy 200.00 GeV.

Thrust Minor distribution at c.m. energy 206.00 GeV.

Jet Mass Difference distribution at c.m. energy 91.20 GeV.

Jet Mass Difference distribution at c.m. energy 133.00 GeV.

Jet Mass Difference distribution at c.m. energy 161.00 GeV.

Jet Mass Difference distribution at c.m. energy 172.00 GeV.

Jet Mass Difference distribution at c.m. energy 183.00 GeV.

Jet Mass Difference distribution at c.m. energy 189.00 GeV.

Jet Mass Difference distribution at c.m. energy 200.00 GeV.

Jet Mass Difference distribution at c.m. energy 206.00 GeV.

Aplanarity distribution at c.m. energy 91.20 GeV.

Aplanarity distribution at c.m. energy 133.00 GeV.

Aplanarity distribution at c.m. energy 161.00 GeV.

Aplanarity distribution at c.m. energy 172.00 GeV.

Aplanarity distribution at c.m. energy 183.00 GeV.

Aplanarity distribution at c.m. energy 189.00 GeV.

Aplanarity distribution at c.m. energy 200.00 GeV.

Aplanarity distribution at c.m. energy 206.00 GeV.

Planarity distribution at c.m. energy 133.00 GeV.

Planarity distribution at c.m. energy 161.00 GeV.

Planarity distribution at c.m. energy 172.00 GeV.

Planarity distribution at c.m. energy 183.00 GeV.

Planarity distribution at c.m. energy 189.00 GeV.

Planarity distribution at c.m. energy 200.00 GeV.

Planarity distribution at c.m. energy 206.00 GeV.

Oblateness distribution at c.m. energy 91.20 GeV.

Oblateness distribution at c.m. energy 133.00 GeV.

Oblateness distribution at c.m. energy 161.00 GeV.

Oblateness distribution at c.m. energy 172.00 GeV.

Oblateness distribution at c.m. energy 183.00 GeV.

Oblateness distribution at c.m. energy 189.00 GeV.

Oblateness distribution at c.m. energy 200.00 GeV.

Oblateness distribution at c.m. energy 206.00 GeV.

Sphericity distribution at c.m. energy 91.20 GeV.

Sphericity distribution at c.m. energy 133.00 GeV.

Sphericity distribution at c.m. energy 161.00 GeV.

Sphericity distribution at c.m. energy 172.00 GeV.

Sphericity distribution at c.m. energy 183.00 GeV.

Sphericity distribution at c.m. energy 189.00 GeV.

Sphericity distribution at c.m. energy 200.00 GeV.

Sphericity distribution at c.m. energy 206.00 GeV.

LN(Y12) distribution at c.m. energy 91.20 GeV.

LN(Y12) distribution at c.m. energy 133.00 GeV.

LN(Y12) distribution at c.m. energy 161.00 GeV.

LN(Y12) distribution at c.m. energy 172.00 GeV.

LN(Y12) distribution at c.m. energy 183.00 GeV.

LN(Y12) distribution at c.m. energy 189.00 GeV.

LN(Y12) distribution at c.m. energy 200.00 GeV.

LN(Y12) distribution at c.m. energy 206.00 GeV.

LN(Y23) distribution at c.m. energy 91.20 GeV.

LN(Y23) distribution at c.m. energy 133.00 GeV.

LN(Y23) distribution at c.m. energy 161.00 GeV.

LN(Y23) distribution at c.m. energy 172.00 GeV.

LN(Y23) distribution at c.m. energy 183.00 GeV.

LN(Y23) distribution at c.m. energy 189.00 GeV.

LN(Y23) distribution at c.m. energy 200.00 GeV.

LN(Y23) distribution at c.m. energy 206.00 GeV.

LN(Y34) distribution at c.m. energy 91.20 GeV.

LN(Y34) distribution at c.m. energy 133.00 GeV.

LN(Y34) distribution at c.m. energy 161.00 GeV.

LN(Y34) distribution at c.m. energy 172.00 GeV.

LN(Y34) distribution at c.m. energy 183.00 GeV.

LN(Y34) distribution at c.m. energy 189.00 GeV.

LN(Y34) distribution at c.m. energy 200.00 GeV.

LN(Y34) distribution at c.m. energy 206.00 GeV.

LN(Y45) distribution at c.m. energy 91.20 GeV.

LN(Y45) distribution at c.m. energy 133.00 GeV.

LN(Y45) distribution at c.m. energy 161.00 GeV.

LN(Y45) distribution at c.m. energy 172.00 GeV.

LN(Y45) distribution at c.m. energy 183.00 GeV.

LN(Y45) distribution at c.m. energy 189.00 GeV.

LN(Y45) distribution at c.m. energy 206.00 GeV.

LN(Y56) distribution at c.m. energy 91.20 GeV.

LN(Y56) distribution at c.m. energy 133.00 GeV.

LN(Y56) distribution at c.m. energy 161.00 GeV.

LN(Y56) distribution at c.m. energy 172.00 GeV.

LN(Y56) distribution at c.m. energy 183.00 GeV.

LN(Y56) distribution at c.m. energy 189.00 GeV.

LN(Y56) distribution at c.m. energy 206.00 GeV.

1-jet fraction at c.m. energy 91.20 GeV.

1-jet fraction at c.m. energy 133.00 GeV.

1-jet fraction at c.m. energy 161.00 GeV.

1-jet fraction at c.m. energy 172.00 GeV.

1-jet fraction at c.m. energy 183.00 GeV.

1-jet fraction at c.m. energy 189.00 GeV.

1-jet fraction at c.m. energy 200.00 GeV.

1-jet fraction at c.m. energy 206.00 GeV.

2-jet fraction at c.m. energy 91.20 GeV.

2-jet fraction at c.m. energy 133.00 GeV.

2-jet fraction at c.m. energy 161.00 GeV.

2-jet fraction at c.m. energy 172.00 GeV.

2-jet fraction at c.m. energy 183.00 GeV.

2-jet fraction at c.m. energy 189.00 GeV.

2-jet fraction at c.m. energy 200.00 GeV.

2-jet fraction at c.m. energy 206.00 GeV.

3-jet fraction at c.m. energy 91.20 GeV.

3-jet fraction at c.m. energy 133.00 GeV.

3-jet fraction at c.m. energy 161.00 GeV.

3-jet fraction at c.m. energy 172.00 GeV.

3-jet fraction at c.m. energy 183.00 GeV.

3-jet fraction at c.m. energy 189.00 GeV.

3-jet fraction at c.m. energy 200.00 GeV.

3-jet fraction at c.m. energy 206.00 GeV.

4-jet fraction at c.m. energy 91.20 GeV.

4-jet fraction at c.m. energy 133.00 GeV.

4-jet fraction at c.m. energy 161.00 GeV.

4-jet fraction at c.m. energy 172.00 GeV.

4-jet fraction at c.m. energy 183.00 GeV.

4-jet fraction at c.m. energy 189.00 GeV.

4-jet fraction at c.m. energy 200.00 GeV.

4-jet fraction at c.m. energy 206.00 GeV.

5-jet fraction at c.m. energy 91.20 GeV.

5-jet fraction at c.m. energy 133.00 GeV.

5-jet fraction at c.m. energy 161.00 GeV.

5-jet fraction at c.m. energy 172.00 GeV.

5-jet fraction at c.m. energy 183.00 GeV.

5-jet fraction at c.m. energy 189.00 GeV.

5-jet fraction at c.m. energy 200.00 GeV.

5-jet fraction at c.m. energy 206.00 GeV.

>=6-jet fraction at c.m. energy 91.20 GeV.

>=6-jet fraction at c.m. energy 133.00 GeV.

>=6-jet fraction at c.m. energy 161.00 GeV.

>=6-jet fraction at c.m. energy 172.00 GeV.

>=6-jet fraction at c.m. energy 183.00 GeV.

>=6-jet fraction at c.m. energy 189.00 GeV.

>=6-jet fraction at c.m. energy 200.00 GeV.

>=6-jet fraction at c.m. energy 206.00 GeV.

Differential cross section as a function of the ratio of the virtualities of the two photons.

Differential cross section as a function of the acolinearity angle PHI between the scattered electrons.

Differential cross section as a function of the acolinearity angle DEL(PHI) between the scattered electrons.

Differential cross section as a function of W of the hadronic system.

Differential cross section as a function of the Bjorken X.

Differential cross section as a function of the DIS Y variable.

Differential cross section as a function of LOG(S/S0).

Inclusive cross section for PI0 production in two-jet events.

Inclusive cross section for ETA production in two-jet events.

Inclusive cross section for ETAPRIME production in two-jet events.

Inclusive cross section for PI0 production in three-jet events where the PI0 comes from JET1.

Inclusive cross section for PI0 production in three-jet events where the PI0 comes from JET2.

Inclusive cross section for PI0 production in three-jet events where the PI0 comes from JET3.

Inclusive cross section for ETA production in three-jet events where the ETA comes from JET1.

Inclusive cross section for ETA production in three-jet events where the ETA comes from JET2.

Inclusive cross section for ETA production in three-jet events where the ETA comes from JET3.

Inclusive cross section for ETAPRIME production in three-jet events where the ETAPRIME comes from JET1.

Inclusive cross section for ETAPRIME production in three-jet events where the ETAPRIME comes from JET2.

Inclusive cross section for ETAPRIME production in three-jet events where the ETAPRIME comes from JET3.

Inclusive cross section for K0S production in hadronic events as a functionof 1/LN(XP).

Inclusive cross section for LAMBDA production in hadronic events as a function of 1/LN(XP).

Inclusive cross section for K0S production in two-jet events as a function of 1/LN(XP).

Inclusive cross section for LAMBDA production in two-jet events as a function of 1/LN(XP).

Inclusive cross section for K0S production in three-jet events where the K0S comes from JET1.

Inclusive cross section for K0S production in three-jet events where the K0S comes from JET2.

Inclusive cross section for K0S production in three-jet events where the K0S comes from JET3.

Inclusive cross section for LAMBDA production in three-jet events where theLAMBDA comes from JET1.

Inclusive cross section for LAMBDA production in three-jet events where theLAMBDA comes from JET2.

Inclusive cross section for LAMBDA production in three-jet events where theLAMBDA comes from JET3.

The photon structure function determined from the ECAL data in the Q**2 bin 35 to 3000 Gev**2 with a mean of 284 +- 49 GeV**2. Bin to bin correlations are given in the next table.

Bin to bin correlations in the extracted values of the photon structure function F2.

The photon structure function determined from the LCAL data in the Q**2 bin 13 to 44 GeV**2 with a mean of 20.67 +- 016 GeV**2. Bin to bin correlations are given in the next table.

Bin to bin correlations in the extracted values of the photon structure function F2.

The photon structure function determined from the LCAL data in the Q**2 bin 6 to 13 GeV**2 with a mean of 9.93 +- 0.04 GeV**2. Bin to bin correlations are given in the next table.

Bin to bin correlations in the extracted values of the photon structure function F2.

The mean values of F2 in the X range 0.1 to 0.6.

Differential cross section, as a function of pseudo-rapidity, from channel (1).

Differential cross section for two jet production with associated D* production, from channel (1). The quoted cross sections correspond to the centres of the bins. The second systematic error is that associated with the energy scale.

Differential cross section for two jet production with associated D* production, from channel (1). The quoted cross sections correspond to the centres of the bins. The second systematic error is that associated with the energy scale.