Cross sections per nucleus for neutron production after correcting for the detector geometric acceptance.

Atomic weight dependence of the neutron cross section.

Lorentz-invariant cross section as a function of xF for pp collisions at 58 GeV.

Lorentz-invariant cross section as a function of xF for pC collisions at 58 GeV.

Lorentz-invariant cross section as a function of xF for pBi collisions at 58 GeV.

Lorentz-invariant cross section as a function of xF for pU collisions at 58 GeV.

Lorentz-invariant cross section as a function of xF for pp collisions at 84 GeV.

Lorentz-invariant cross section as a function of xF for pBe collisions at 120 GeV.

Lorentz-invariant cross section as a function of xF for pC collisions at 120 GeV.

Lorentz-invariant cross section as a function of xF for pBi collisions at 120 GeV.

dsig/dxF as a function of xF for pp collisions at 58 GeV.

dsig/dxF as a function of xF for pC collisions at 58 GeV.

dsig/dxF as a function of xF for pBi collisions at 58 GeV.

dsig/dxF as a function of xF for pU collisions at 58 GeV.

dsig/dxF as a function of xF for pp collisions at 84 GeV.

dsig/dxF as a function of xF for pBe collisions at 120 GeV.

dsig/dxF as a function of xF for pC collisions at 120 GeV.

dsig/dxF as a function of xF for pBi collisions at 120 GeV.

$p_{T}^{t,1}$ absolute differential cross-section at particle level.

$|{y}^{t,1}|$ absolute differential cross-section at particle level.

$p_{T}^{t,2}$ absolute differential cross-section at particle level.

$|{y}^{t,2}|$ absolute differential cross-section at particle level.

$m^{t\bar{t}}$ absolute differential cross-section at particle level.

$p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level.

$|y^{t\bar{t}}|$ absolute differential cross-section at particle level.

$\chi^{t\bar{t}}$ absolute differential cross-section at particle level.

$|y_{B}^{t\bar{t}}|$ absolute differential cross-section at particle level.

$|p_{out}^{t\bar{t}}|$ absolute differential cross-section at particle level.

$|\Delta \phi(t_{1}, t_{2})|$ absolute differential cross-section at particle level.

$H_{T}^{t\bar{t}}$ absolute differential cross-section at particle level.

$|\cos\theta^{*}|$ absolute differential cross-section at particle level.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t,2}|$ < 0.2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t,2}|$ < 0.5.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t,2}|$ < 1.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t,2}|$ < 2.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$p_{T}^{t}$ normalized differential cross-section at particle level.

$|y^{t}|$ normalized differential cross-section at particle level.

$p_{T}^{t,1}$ normalized differential cross-section at particle level.

$|{y}^{t,1}|$ normalized differential cross-section at particle level.

$p_{T}^{t,2}$ normalized differential cross-section at particle level.

$|{y}^{t,2}|$ normalized differential cross-section at particle level.

$m^{t\bar{t}}$ normalized differential cross-section at particle level.

$p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level.

$|y^{t\bar{t}}|$ normalized differential cross-section at particle level.

$\chi^{t\bar{t}}$ normalized differential cross-section at particle level.

$|y_{B}^{t\bar{t}}|$ normalized differential cross-section at particle level.

$|p_{out}^{t\bar{t}}|$ normalized differential cross-section at particle level.

$|\Delta \phi(t_{1}, t_{2})|$ normalized differential cross-section at particle level.

$H_{T}^{t\bar{t}}$ normalized differential cross-section at particle level.

$|\cos\theta^{*}|$ normalized differential cross-section at particle level.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t,2}|$ < 0.2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t,2}|$ < 0.5.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t,2}|$ < 1.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t,2}|$ < 2.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

Fiducial phase-space cross-section at parton level.

$p_{T}^{t}$ absolute differential cross-section at parton level.

$|y^{t}|$ absolute differential cross-section at parton level.

$p_{T}^{t,1}$ absolute differential cross-section at parton level.

$|y^{t,1}|$ absolute differential cross-section at parton level.

$p_{T}^{t,2}$ absolute differential cross-section at parton level.

$|{y}^{t,2}|$ absolute differential cross-section at parton level.

$m^{t\bar{t}}$ absolute differential cross-section at parton level.

$p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level.

$|{y}^{t\bar{t}}|$ absolute differential cross-section at parton level.

${\chi}^{t\bar{t}}$ absolute differential cross-section at parton level.

$|y_{B}^{t\bar{t}}|$ absolute differential cross-section at parton level.

$|p_{out}^{t\bar{t}}|$ absolute differential cross-section at parton level.

$|\Delta \phi(t_{1}, t_{2})|$ absolute differential cross-section at parton level.

$H_{T}^{t\bar{t}}$ absolute differential cross-section at parton level.

$|\cos\theta^{*}|$ absolute differential cross-section at parton level.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t,2}|$ < 0.2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t,2}|$ < 0.5.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t,2}|$ < 1.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t,2}|$ < 2.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$p_{T}^{t}$ normalized differential cross-section at parton level.

$|y^{t}|$ normalized differential cross-section at parton level.

$p_{T}^{t,1}$ normalized differential cross-section at parton level.

$|y^{t,1}|$ normalized differential cross-section at parton level.

$p_{T}^{t,2}$ normalized differential cross-section at parton level.

$|{y}^{t,2}|$ normalized differential cross-section at parton level.

$m^{t\bar{t}}$ normalized differential cross-section at parton level.

$p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level.

$|{y}^{t\bar{t}}|$ normalized differential cross-section at parton level.

${\chi}^{t\bar{t}}$ normalized differential cross-section at parton level.

$|y_{B}^{t\bar{t}}|$ normalized differential cross-section at parton level.

$|p_{out}^{t\bar{t}}|$ normalized differential cross-section at parton level.

$|\Delta \phi(t_{1}, t_{2})|$ normalized differential cross-section at parton level.

$H_{T}^{t\bar{t}}$ normalized differential cross-section at parton level.

$|\cos\theta^{*}|$ normalized differential cross-section at parton level.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t,2}|$ < 0.2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t,2}|$ < 0.5.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t,2}|$ < 1.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 1 < $|{y}^{t,2}|$ < 2.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2.

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.

Here THETA is the angle (in c.m. system) between the plane containing partons 1 and 3 and the plane containing partons 4 and 5: cos(theta) = [p1*p3]*[p4*p ]/(|[p1*p3]|*|[p4*p5]|). The estimated systematic uncertainty is 6 PCT.

Here M is scaled invariant mass of jet pairs. The estimated systematic uncertainty is 6 PCT.

Here M is scaled invariant mass of jet pairs. The estimated systematic uncertainty is 6 PCT.

Here M is scaled invariant mass of jet pairs. The estimated systematic uncertainty is 6 PCT.

The estimated systematic uncertainty is 6 PCT. 4-JET events in their center-of-mass system.

The estimated systematic uncertainty is 6 PCT. 4-JET events in their center-of-mass system.

The estimated systematic uncertainty is 6 PCT. 4-JET events in their center-of-mass system.

The estimated systematic uncertainty is 6 PCT. 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. The measured distribution of cosine of space angles between pairs of jets for the 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. The measured distribution of cosine of space angles between pairs of jets for the 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. The measured distribution of cosine of space angles between pairs of jets for the 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. The measured distribution of cosine of space angles between pairs of jets for the 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. The measured distribution of cosine of space angles between pairs of jets for the 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. The measured distribution of cosine of space angles between pairs of jets for the 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. The measured distribution of scaled jets pair masses for the 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. The measured distribution of scaled jets pair masses for the 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. The measured distribution of scaled jets pair masses for the 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. The measured distribution of scaled jets pair masses for the 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. The measured distribution of scaled jets pair masses for the 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. The measured distribution of scaled jets pair masses for the 4-JET events in their center-of-mass system.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. Here THETA is 'Bengtsson-Zerwas' (BZ) angle defined as COS(THETA(N=BZ)) = [p3*p4]*[p5*p6]/(|p3*p4|*|p5*p6|), where P(i) are jet momentum in the center-o f-mass frame.

Errors are statistical only. The estimated systematic uncertainty is 6 PCT. Here THETA is 'Nachtmann-Reiter' (NR) angle defined as COS(THETA(N=NR))= (p3-p4)*(p5-p6)/(|p3-p4|*|p5-p6|).

The NC cross section DSIG/DX for Q**2 > 10000 GeV**2. There is an additional 1.5 PCT normalization uncertainty.

The CC cross section DSIG/DX for Q**2 > 1000 GeV**2. There is an additional 1.5 PCT normalization uncertainty.

The NC reduced cross section and the electromagnetic structure funcion F2 derived from the data. For Q**2 > 2000 GeV**2 the extraction of F2 is restricted to Y < 0.6.

The CC double differential cross section D2SIG/DX/DQ**2 and the structure function term PHI.

The NC E- P reduced cross section for the high-y analysis. All E- P data not previously reported in EPJ C19 (2001) 269 are given.. There is an additional 1.8 PCT normalization uncertainty.

The NC structure function term PHI and the structure function FL for the E-P data.

The NC structure function term PHI and the structure function FL for the E+P data.

The generalised structure function XF3.

The structure function XF3(C=GAMMA,Z) obtained by averaging over different Q**2 values and transforming to Q**2 = 1500 GeV**2.

Breakdown of errors from table 11, F2 as a function of Q**2, X and Y. PHI(C=NC) is the NC structure function term.. Y+ = 1+(1-Y)**2. DEL(F2),DEL9F3) and DEL(FL) are the corrections to F2 as decribed in the text of the paper.

Measured cross section DSIG/DM(PI+PI-) for the W range 1475 to 1500GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1500 to 1525GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1525 to 1550GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1550 to 1575GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1575 to 1600GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1600 to 1625GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1625 to 1650GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1650 to 1675GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1675 to 1700GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1700 to 1725GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1725 to 1750GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1750 to 1775GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1775 to 1800GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1800 to 1825GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1825 to 1850GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1850 to 1875GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1875 to 1900GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1900 to 1925GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1925 to 1950GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1950 to 1975GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1975 to 2000GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 2000 to 2025GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 2025 to 2050GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 2050 to 2075GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 2075 to 2100GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1400 to 1425GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1425 to 1450GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1450 to 1475GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1475 to 1500GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1500 to 1525GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1525 to 1550GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1550 to 1575GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1575 to 1600GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1600 to 1625GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1625 to 1650GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1650 to 1675GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1675 to 1700GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1700 to 1725GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1725 to 1750GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1750 to 1775GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1775 to 1800GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1800 to 1825GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1825 to 1850GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1850 to 1875GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1875 to 1900GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1900 to 1925GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1925 to 1950GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1950 to 1975GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1975 to 2000GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 2000 to 2025GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 2025 to 2050GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 2050 to 2075GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 2075 to 2100GeV.

Measured c.m. angular distribution of the PI- for the W range 1400 to 1425GeV.

Measured c.m. angular distribution of the PI- for the W range 1425 to 1450GeV.

Measured c.m. angular distribution of the PI- for the W range 1450 to 1475GeV.

Measured c.m. angular distribution of the PI- for the W range 1475 to 1500GeV.

Measured c.m. angular distribution of the PI- for the W range 1500 to 1525GeV.

Measured c.m. angular distribution of the PI- for the W range 1525 to 1550GeV.

Measured c.m. angular distribution of the PI- for the W range 1550 to 1575GeV.

Measured c.m. angular distribution of the PI- for the W range 1575 to 1600GeV.

Measured c.m. angular distribution of the PI- for the W range 1600 to 1625GeV.

Measured c.m. angular distribution of the PI- for the W range 1625 to 1650GeV.

Measured c.m. angular distribution of the PI- for the W range 1650 to 1675GeV.

Measured c.m. angular distribution of the PI- for the W range 1675 to 1700GeV.

Measured c.m. angular distribution of the PI- for the W range 1700 to 1725GeV.

Measured c.m. angular distribution of the PI- for the W range 1725 to 1750GeV.

Measured c.m. angular distribution of the PI- for the W range 1750 to 1775GeV.

Measured c.m. angular distribution of the PI- for the W range 1775 to 1800GeV.

Measured c.m. angular distribution of the PI- for the W range 1800 to 1825GeV.

Measured c.m. angular distribution of the PI- for the W range 1825 to 1850GeV.

Measured c.m. angular distribution of the PI- for the W range 1850 to 1875GeV.

Measured c.m. angular distribution of the PI- for the W range 1875 to 1900GeV.

Measured c.m. angular distribution of the PI- for the W range 1900 to 1925GeV.

Measured c.m. angular distribution of the PI- for the W range 1925 to 1950GeV.

Measured c.m. angular distribution of the PI- for the W range 1950 to 1975GeV.

Measured c.m. angular distribution of the PI- for the W range 1975 to 2000GeV.

Measured c.m. angular distribution of the PI- for the W range 2000 to 2025GeV.

Measured c.m. angular distribution of the PI- for the W range 2025 to 2050GeV.

Measured c.m. angular distribution of the PI- for the W range 2050 to 2075GeV.

Measured c.m. angular distribution of the PI- for the W range 2075 to 2100GeV.

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Normalised distribution of (1-THRUST) where THRUST is w.r.t the axis which maximises the sum of the longitudinal momenta in the current hemisphere, for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the axis which maximises the sum of the longitudinal momenta in the current hemisphere, for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the axis which maximises the sum of the longitudinal momenta in the current hemisphere, for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the axis which maximises the sum of the longitudinal momenta in the current hemisphere, for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Normalised distribution of Jet Broadening (B), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Normalised distribution of Jet Broadening (B), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Normalised distribution of Jet Broadening (B), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Normalised distribution of Jet Broadening (B), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of Jet Broadening (B), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of Jet Broadening (B), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of Jet Broadening (B), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Normalised distribution of the C-Parameter, for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Normalised distribution of the C-Parameter, for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Normalised distribution of the C-Parameter, for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Normalised distribution of the C-Parameter, for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of the C-Parameter, for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of the C-Parameter, for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of the C-Parameter, for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Mean values of the event shape variables.

Covariance matrix for (1-THRUST(C)), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for (1-THRUST(C)), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for (1-THRUST(C)), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for (1-THRUST(C)), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for (1-THRUST(C)), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for (1-THRUST(C)), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for (1-THRUST(C)), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Covariance matrix for (1-THRUST), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for (1-THRUST), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for (1-THRUST), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for (1-THRUST), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for (1-THRUST), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for (1-THRUST), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for (1-THRUST), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Covariance matrix for the Jet Broadening (B), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for the Jet Broadening (B), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for the Jet Broadening (B), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for the Jet Broadening (B), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for the Jet Broadening (B), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for the Jet Broadening (B), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for the Jet Broadening (B), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Covariance matrix for the C-Parameter, for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for the C-Parameter, for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for the C-Parameter, for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for the C-Parameter, for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for the C-Parameter, for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for the C-Parameter, for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for the C-Parameter, for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Inclusive di-jet cross section as a function of the di-jet mass M and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of Y (inelasticity) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and ET.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETARAP(forward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETARAP(backward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive single jet cross section as a function of ET and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive dijet cross section as a function Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of ET and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of the di-jet mass M and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of Y (inelasticity) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and ET.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of ETARAP(forward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of ETARAP(backward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive dijet cross section as a function Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of ET and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of the di-jet mass M and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of Y (inelasticity) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and ET.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETARAP(forward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETARAP(backward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive dijet cross section as a function Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of ET and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of the di-jet mass M and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of Y (inelasticity) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and ET.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of ETARAP(forward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of ETARAP(backward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.