Normalized $\sigma_{\psi(2S)}/\sigma_{J/\psi}$ in $6.5<p_T<30.0\,GeV$ and $ 1 < y_{CM} < 1.935$ as functions of normalized $\text{N}^{{\text{corr.}}}_{\text{track}}$

Normalized $\sigma_{\psi(2S)}/\sigma_{J/\psi}$ in $6.5<p_T<30.0\,GeV$ and $ -2.865 < y_{CM} < 1.935$ as functions of normalized $\text{N}^{{\text{corr.}}}_{\text{track}}$

Normalized $\sigma_{\psi(2S)}/\sigma_{J/\psi}$ in $3.0<p_T<6.5\,GeV$ and $ -2.865 < y_{CM} < -2 $ as functions of normalized $\text{N}^{{\text{corr.}}}_{\text{track}}$

Normalized $\sigma_{\psi(2S)}/\sigma_{J/\psi}$ in $3.0<p_T<6.5\,GeV$ and $ 1 < y_{CM} < 1.935 $ as functions of normalized $\text{N}^{{\text{corr.}}}_{\text{track}}$

Mean $p_T$ values of the $\Upsilon(1$S$)$, $\Upsilon(2$S$)$, and $\Upsilon(3$S$)$ states with $p_T\,>\,0\,GeV$ and $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$

Ratio $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $0<p_T<5\,$GeV range

Ratio $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $5<p_T<7\,$GeV range

Ratio $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $7<p_T<9\,$GeV range

Ratio $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $9<p_T<11\,$GeV range

Ratio $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $11<p_T<15\,$GeV range

Ratio $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $15<p_T<20\,$GeV range

Ratio $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $20<p_T<50\,$GeV range

Ratio $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $0<p_T<5\,$GeV range

Ratio $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $5<p_T<7\,$GeV range

Ratio $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $7<p_T<9\,$GeV range

Ratio $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $9<p_T<11\,$GeV range

Ratio $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $11<p_T<15\,$GeV range

Ratio $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $15<p_T<20\,$GeV range

Ratio $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ with $|y|\,<\,1.2$ as a function of track multiplicity $N_{track}$ in $20<p_T<50\,$GeV range

Ratios $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ and $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ as functions of "forward" track multiplicity $N_{track}^{\Delta\phi}$ for $\Upsilon(n$S$)$ states with $p_T\,>\,7\,GeV$ and $|y|\,<\,1.2$. Forward tracks are those with momentum direction in $\Delta\phi\,<\,\pi/3$ w.r.t. the $\Upsilon(n$S$)$ momentum direction.

Ratios $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ and $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ as functions of "transverse" track multiplicity $N_{track}^{\Delta\phi}$ for $\Upsilon(n$S$)$ states with $p_T\,>\,7\,GeV$ and $|y|\,<\,1.2$. Transverse tracks are those with momentum direction in $\pi/3\,<\,\Delta\phi\,<\,2\pi/3$ w.r.t. the $\Upsilon(n$S$)$ momentum direction.

Ratios $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ and $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ as functions of "backward" track multiplicity $N_{track}^{\Delta\phi}$ for $\Upsilon(n$S$)$ states with $p_T\,>\,7\,GeV$ and $|y|\,<\,1.2$. Backward tracks are those with momentum direction in $\Delta\phi\,>\,2\pi/3$ w.r.t. the $\Upsilon(n$S$)$ momentum direction.

Ratios $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ and $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ as functions of track multiplicity $N_{track}$ for $\Upsilon(n$S$)$ states with $p_T\,>\,7\,GeV$ and $|y|\,<\,1.2$ and $N^{\Delta R}_{track}\,=\,0$ charged particles produced in $\Delta R\,<\,0.5$ cone around $\Upsilon(n$S$)$ momentum direction.

Ratios $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ and $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ as functions of track multiplicity $N_{track}$ for $\Upsilon(n$S$)$ states with $p_T\,>\,7\,GeV$ and $|y|\,<\,1.2$ and $N^{\Delta R}_{track}\,=\,1$ charged particles produced in $\Delta R\,<\,0.5$ cone around $\Upsilon(n$S$)$ momentum direction.

Ratios $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ and $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ as functions of track multiplicity $N_{track}$ for $\Upsilon(n$S$)$ states with $p_T\,>\,7\,GeV$ and $|y|\,<\,1.2$ and $N^{\Delta R}_{track}\,=\,2$ charged particles produced in $\Delta R\,<\,0.5$ cone around $\Upsilon(n$S$)$ momentum direction.

Ratios $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ and $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ as functions of track multiplicity $N_{track}$ for $\Upsilon(n$S$)$ states with $p_T\,>\,7\,GeV$ and $|y|\,<\,1.2$ and $N^{\Delta R}_{track}\,>\,2$ charged particles produced in $\Delta R\,<\,0.5$ cone around $\Upsilon(n$S$)$ momentum direction.

Ratios $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ and $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ as functions of track multiplicity $N_{track}$ in transverse sphericity bin $0.00\,<\,S_T\,<\,0.55$ for $\Upsilon(n$S$)$ states with $p_T\,>\,7\,GeV$ and $|y|\,<\,1.2$.

Ratios $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ and $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ as functions of track multiplicity $N_{track}$ in transverse sphericity bin $0.55\,<\,S_T\,<\,0.70$ for $\Upsilon(n$S$)$ states with $p_T\,>\,7\,GeV$ and $|y|\,<\,1.2$.

Ratios $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ and $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ as functions of track multiplicity $N_{track}$ in transverse sphericity bin $0.70\,<\,S_T\,<\,0.85$ for $\Upsilon(n$S$)$ states with $p_T\,>\,7\,GeV$ and $|y|\,<\,1.2$.

Ratios $\Upsilon(2$S$)\,/\,\Upsilon(1$S$)$ and $\Upsilon(3$S$)\,/\,\Upsilon(1$S$)$ as functions of track multiplicity $N_{track}$ in transverse sphericity bin $0.85\,<\,S_T\,<\,1.00$ for $\Upsilon(n$S$)$ states with $p_T\,>\,7\,GeV$ and $|y|\,<\,1.2$.

Efficiency-corrected multiplicity bins used in the $\Upsilon(n$S$)$ ratio analysis and the corresponding mean number of charged particle tracks.

Charged-particle multiplicities in proton-proton collisions at a centre-of mass energy of 13000 GeV as a function of transverse momentum for events with the number of charged particles >=2 having transverse momentum >100 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicity distribution in proton-proton collisions at a centre-of mass energy of 13000 GeV for events with the number of charged particles >=2 having transverse momentum >100 MeV and absolute(pseudorapidity) <2.5.

Average transverse momentum in proton-proton collisions at a centre-of mass energy of 13000 GeV as a function of the number of charged particles in the event for events with the number of charged particles >=2 having transverse momentum >100 MeV and absolute(pseudorapidity) <2.5.

Extrapolated ($\tau > 30$ ps) charged-particle multiplicities in proton-proton collisions at a centre-of mass energy of 13000 GeV as a function of pseudorapidity for events with the number of charged particles >=2 having transverse momentum >100 MeV and absolute(pseudorapidity) <2.5.

Extrapolated ($\tau > 30$ ps) charged-particle multiplicities in proton-proton collisions at a centre-of mass energy of 13000 GeV as a function of transverse momentum for events with the number of charged particles >=2 having transverse momentum >100 MeV and absolute(pseudorapidity) <2.5.

Extrapolated ($\tau > 30$ ps) charged-particle multiplicity distributions in proton-proton collisions at a centre-of mass energy of 13000 GeV for events with the number of charged particles >=2 having transverse momentum >100 MeV and absolute(pseudorapidity) <2.5.

Extrapolated ($\tau > 30$ ps) average transverse momentum in proton-proton collisions at a centre-of mass energy of 13000 GeV as a function of the number of charged particles in the event for events with the number of charged particles >=2 having transverse momentum >100 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicities in proton-proton collisions at a centre-of mass energy of 8000 GeV as a function of transverse momentum for events with the number of charged particles >=2 having transverse momentum >100 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicities in proton-proton collisions at a centre-of mass energy of 8000 GeV as a function of transverse momentum for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicities in proton-proton collisions at a centre-of mass energy of 8000 GeV as a function of transverse momentum for events with the number of charged particles >=6 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicities in proton-proton collisions at a centre-of mass energy of 8000 GeV as a function of transverse momentum for events with the number of charged particles >=20 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicities in proton-proton collisions at a centre-of mass energy of 8000 GeV as a function of transverse momentum for events with the number of charged particles >=50 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicities in proton-proton collisions at a centre-of mass energy of 8000 GeV as a function of pseudorapidity for events with the number of charged particles >=2 having transverse momentum >100 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicities in proton-proton collisions at a centre-of mass energy of 8000 GeV as a function of pseudorapidity for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicities in proton-proton collisions at a centre-of mass energy of 8000 GeV as a function of pseudorapidity for events with the number of charged particles >=6 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicities in proton-proton collisions at a centre-of mass energy of 8000 GeV as a function of pseudorapidity for events with the number of charged particles >=20 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicities in proton-proton collisions at a centre-of mass energy of 8000 GeV as a function of pseudorapidity for events with the number of charged particles >=50 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Average transverse momentum in proton-proton collisions at a centre-of mass energy of 8000 GeV as a function of the number of charged particles in the event for events with the number of charged particles >=2 having transverse momentum >100 MeV and absolute(pseudorapidity) <2.5.

Average transverse momentum in proton-proton collisions at a centre-of mass energy of 8000 GeV as a function of the number of charged particles in the event for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicities in proton-proton collisions at a centre-of-mass energy of 13000 GeV as a function of transverse momentum for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicity distribution in proton-proton collisions at a centre-of-mass energy of 13000 GeV for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Average transverse momentum in proton-proton collisions at a centre-of-mass energy of 13000 GeV as a function of the number of charged particles in the event for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Extrapolated charged-particle multiplicities in proton-proton collisions at a centre-of-mass energy of 13000 GeV as a function of pseudorapidity for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Extrapolated charged-particle multiplicities in proton-proton collisions at a centre-of-mass energy of 13000 GeV as a function of transverse momentum for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Extrapolated charged-particle multiplicity distributions in proton-proton collisions at a centre-of-mass energy of 13000 GeV for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Extrapolated average transverse momentum in proton-proton collisions at a centre-of-mass energy of 13000 GeV as a function of the number of charged particles in the event for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <2.5.

Charged-particle multiplicities in proton-proton collisions at a centre-of-mass energy of 13000 GeV as a function of pseudorapidity for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <0.8.

Charged-particle multiplicities in proton-proton collisions at a centre-of-mass energy of 13000 GeV as a function of transverse momentum for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <0.8.

Charged-particle multiplicity distribution in proton-proton collisions at a centre-of-mass energy of 13000 GeV for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <0.8.

Average transverse momentum in proton-proton collisions at a centre-of-mass energy of 13000 GeV as a function of the number of charged particles in the event for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <0.8.

Extrapolated charged-particle multiplicities in proton-proton collisions at a centre-of-mass energy of 13000 GeV as a function of pseudorapidity for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <0.8.

Extrapolated charged-particle multiplicities in proton-proton collisions at a centre-of-mass energy of 13000 GeV as a function of transverse momentum for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <0.8.

Extrapolated charged-particle multiplicity distributions in proton-proton collisions at a centre-of-mass energy of 13000 GeV for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <0.8.

Extrapolated average transverse momentum in proton-proton collisions at a centre-of-mass energy of 13000 GeV as a function of the number of charged particles in the event for events with the number of charged particles >=1 having transverse momentum >500 MeV and absolute(pseudorapidity) <0.8.

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.

The distribution of ratio of cross sections for successive exclusive jet multiplicities n/(n-1). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of exclusive jet multiplicity, pT(jet1) > 150 GeV. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of ratio of cross sections for successive exclusive jet multiplicities, pT(jet1) > 150 GeV. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of Exclusive jet multiplicity, M(jj)>350, Dy(jj) >3.0. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of Ratio of successive exclusive jet multiplicities, M(jj)>350, Dy(jj) >3.0. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of pT (leading jet) [GeV]. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of pT (2nd jet) [GeV]. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of pT (3rd jet) [GeV]. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of pT (4th jet) [GeV]. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of pT(jet) Z+1jet exclusive. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of pT(2nd jet)/pT(leading jet)). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of pT(Z). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of pT(Z), Z+1jet, exclusive. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of |y| (leading jet). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of |y| (2nd jet). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of |y| (3rd jet). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of |y| (4th jet). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of Dy (jj). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of M(jj). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of DPhi (jj). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of DR (jj). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of pT(3rd jet), m(jj) > 350 GeV, Dy(jj) > 3.0. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of |y| (3rd jet), m(jj) > 350 GeV, Dy(jj) > 3.0. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of HT, the scalar pT sum of the jets and leptons. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

The distribution of ST, the scalar pT sum of the jets. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

Bin averaged scaled momentum spectra in the Q**2 range 10240 to 20480 GeV**2.

Bin averaged scaled momentum spectra in the Q**2 range 20480 to 40960 GeV**2.

Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0 to 0.02.

Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.02 to 0.05.

Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.05 to 0.1.

Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.1 to 0.2.

Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.2 to 0.3.

Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.3 to 0.4.

Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.4 to 0.5.

Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.5 to 0.7.

Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.7 to 1.0.

The normalized charged particle density for the Q**2 range 5120 to 10240 GeV in three W ranges.

The normalized charged particle density for the Q**2 range 2560 to 5120 GeV in three W ranges.

The normalized charged particle density for the Q**2 range 1280 to 2560 GeV in four W ranges.

The normalized charged particle density for the Q**2 range 640 to 1280 GeV in four W ranges.

The normalized charged particle density for the Q**2 range 320 to 640GeV in three W ranges.

The normalized charged particle density for the Q**2 range 160 to 320 GeV in four W ranges.

The normalized charged particle density for the Q**2 range 60 to 160 GeV in three W ranges.

The normalized charged particle density for the Q**2 range 50 to 60 GeV in three W ranges.

The normalized charged particle density for the Q**2 range 40 to 50 GeV in three W ranges.

The normalized charged particle density for the Q**2 range 30 to 40 GeV in three W ranges.

The normalized charged particle density for the Q**2 range 20 to 30 GeV in two W ranges.

The normalized charged particle density for the Q**2 range 10 to 20 GeV in two W ranges.

Measured mean integrated jet shape corrected to the hadron level in photoproduction with -1 < ETARAP(C=JET) < 2.5.

Measured mean integrated jet shape corrected to the hadron level in photoproduction with -1 < ETARAP(C=JET) < 2.5.

Measured mean integrated jet shape corrected to the hadron level in photoproduction with -1 < ETARAP(C=JET) < 2.5.

Measured mean integrated jet shape corrected to the hadron level and for electroweak radiative effects in DIS with ET(C=JET) > 17 GeV.

Measured mean integrated jet shape corrected to the hadron level and for electroweak radiative effects in DIS with ET(C=JET) > 17 GeV.

Measured mean integrated jet shape corrected to the hadron level and for electroweak radiative effects in DIS with -1 < ETARAP(C=JET) < 2.5.

Measured mean integrated jet shape corrected to the hadron level and for electroweak radiative effects in DIS with -1 < ETARAP(C=JET) < 2.5.

Measured mean integrated jet shape corrected to the hadron level and for electroweak radiative effects in DIS with -1 < ETARAP(C=JET) < 2.5.

Measured mean integrated jet shape corrected to the hadron level and for electroweak radiative effects in DIS with -1 < ETARAP(C=JET) < 2.5.

Measured mean subject multiplicity corrected to the hadron level for photoproduction with ET(C=JET) > 17 GeV.

Measured mean subject multiplicity corrected to the hadron level for photoproduction with ET(C=JET) > 17 GeV.

Measured mean subject multiplicity corrected to the hadron level and for photoproduction with ET(C=JET) > 17 GeV.

Measured mean subject multiplicity corrected to the hadron level and for photoproduction with ET(C=JET) > 17 GeV.

Measured mean subject multiplicity corrected to the hadron level and for photoproduction with ET(C=JET) > 17 GeV.

Measured mean subject multiplicity corrected to the hadron level and for photoproduction with ET(C=JET) > 17 GeV.

Measured differential cross section DSIG/DETARAP for inclusive jet photoproduction with ET(C=JET) > 17 GeV. Jets are divided into BROAD and NARROW jets according to their shape.

Measured differential cross section DSIG/DETARAP for inclusive jet photoproduction with ET(C=JET) > 17 GeV. Jets are divided into BROAD and NARROW jets according to their subject multiplicity.

Measured differential cross section DSIG/DETARAP for inclusive jet photoproduction with ET(C=JET) > 17 GeV. Jets are divided into BROAD and NARROW jets according to the combination of shape and subject multiplicity.

Measured differential cross section DSIG/DETARAP for inclusive jet production in DIS with ET(C=JET) > 17 GeV. Jets are divided into BROAD and NARROW jets according to their shape.

Measured differential cross section DSIG/DET for inclusive jet photoproduction with -1 < ETARAP(C=JET) < 2.5. Jets are divided into BROAD and NARROW jets according to their shape.

Measured differential cross section DSIG/DET for inclusive jet photoproduction with -1 < ETARAP(C=JET) < 2.5. Jets are divided into BROAD and NARROW jets according to their subject multiplicity.

Measured differential cross section DSIG/DET for inclusive jet photoproduction with -1 < ETARAP(C=JET) < 2.5. Jets are divided into BROAD and NARROW jets according to the combination of shape and subject multiplicity.

Measured differential cross section DSIG/DET for inclusive jet production in DIS with -1 < ETARAP(C=JET) < 2.5. Jets are divided into BROAD and NARROW jets according to their shape.

Measured differential dijet cross section DSIG/DCOS(THETA) in dijet photoproduction with M(C=2JET) > 52 GeV. The data are divided into BROAD-BROAD and NARROW-NARROW jets according to the jet shapes.

Measured differential dijet cross section DSIG/DCOS(THETA) in dijet photoproduction with M(C=2JET) > 52 GeV. The data are divided into BROAD-NARROW jets according to the jet shapes.

Measured differential cross section DSIG/DM for dijet photoproduction with ABS(COS(THETA)) < 0.8. The data are divided into BROAD-BROAD and NARROW-NARROW jets according to the jet shapes.

Measured differential cross section DSIG/DX(C=GAMMA) for dijet photoproduction. The data are divided into BROAD-BROAD and NARROW-NARROW jets according to the jet shapes.

Values of ALPHAS determined for the QCD fit of the measured mean PSI value at R = 0.5 as a function of ET(C=JET) in DIS events.

Inclusive jet cross section DSIG/DETARAP for jets in the lab. frame. Data from the 1995-1997 data sample.

Inclusive jet cross section DSIG/DETARAP for jets in the lab. frame. Data from the 1999-2000 data sample.

Inclusive jet cross section DSIG/DETARAP for jets in the lab. frame. Data from the combined data sample.

Inclusive jet cross section DSIG/DET for jets in the lab. frame. Data from the 1995-1997 running period.

Inclusive jet cross section DSIG/DET for jets in the lab. frame. Data from the 1999-2000 running period.

Inclusive jet cross section DSIG/DET for jets in the lab. frame. Data from the combined running period.

Inclusive di-jet cross section DSIG/DQ**2 for jets in the lab. frame. Data from the 1995-1997 data sample.

Inclusive di-jet cross section DSIG/DQ**2 for jets in the lab. frame. Data from the 1999-2000 data sample.

Inclusive di-jet cross section DSIG/DQ**2 for jets in the lab. frame. Data from the combined data sample.

Inclusive di-jet cross section DSIG/DM for jets in the lab. frame. Data from the 1995-1997 sample.

Inclusive di-jet cross section DSIG/DM for jets in the lab. frame. Data from the 1999-2000 sample.

Inclusive di-jet cross section DSIG/DM for jets in the lab. frame. Data from the combined sample.

Mean subjet multiplicity as a function of the YCUT parameter used in defining the jet for the inclusive jet sample with ET 14 to 17 GeV and 17 to 21 GeV.

Mean subjet multiplicity as a function of the YCUT parameter used in defining the jet for the inclusive jet sample with ET 21 to 25 GeV and 25 to 35 GeV.

Mean subjet multiplicity as a function of the YCUT parameter used in defining the jet for the inclusive jet sample with ET 35 to 55 GeV and 55 to 119 GeV.

Measured values of the mean subjet multiplicity at YCUT = 0.01 as a function of Q**2.

Value of ALPHAS at the Z0 mass obtained from the data with ET(C=JET) > 25 GeV.. The second DSYS error is due to the uncertainty in the theory.