Showing 10 of 464 results
Measurements of single-, double-, and triple-differential cross-sections are presented for boosted top-quark pair-production in 13 $\text{TeV}$ proton-proton collisions recorded by the ATLAS detector at the LHC. The top quarks are observed through their hadronic decay and reconstructed as large-radius jets with the leading jet having transverse momentum ($p_{\text{T}}$) greater than 500 GeV. The observed data are unfolded to remove detector effects. The particle-level cross-section, multiplied by the $t\bar{t} \rightarrow W W b \bar{b}$ branching fraction and measured in a fiducial phase space defined by requiring the leading and second-leading jets to have $p_{\text{T}} > 500$ GeV and $p_{\text{T}} > 350$ GeV, respectively, is $331 \pm 3 \text{(stat.)} \pm 39 \text{(syst.)}$ fb. This is approximately 20$\%$ lower than the prediction of $398^{+48}_{-49}$ fb by Powheg+Pythia 8 with next-to-leading-order (NLO) accuracy but consistent within the theoretical uncertainties. Results are also presented at the parton level, where the effects of top-quark decay, parton showering, and hadronization are removed such that they can be compared with fixed-order next-to-next-to-leading-order (NNLO) calculations. The parton-level cross-section, measured in a fiducial phase space similar to that at particle level, is $1.94 \pm 0.02 \text{(stat.)} \pm 0.25 \text{(syst.)}$ pb. This agrees with the NNLO prediction of $1.96^{+0.02}_{-0.17}$ pb. Reasonable agreement with the differential cross-sections is found for most NLO models, while the NNLO calculations are generally in better agreement with the data. The differential cross-sections are interpreted using a Standard Model effective field-theory formalism and limits are set on Wilson coefficients of several four-fermion operators.
Fiducial phase-space cross-section at particle level.
$p_{T}^{t}$ absolute differential cross-section at particle level.
$|y^{t}|$ absolute differential cross-section at particle level.
$p_{T}^{t,1}$ 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.
A new method is employed to measure the neutral current cross section up to Bjorken-x values of one with the ZEUS detector at HERA using an integrated luminosity of 65.1 pb-1 for e+p collisions and 16.7 pb-1 for e-p collisions at sqrt{s}=318 GeV and 38.6 pb-1 for e+p collisions at sqrt{s}=300 GeV. Cross sections have been extracted for Q2 >= 648 GeV2 and are compared to predictions using different parton density functions. For the highest x bins, the data have a tendency to lie above the expectations using recent parton density function parametrizations.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The double differential cross section for the 96-97 E+ P NC scattering data.
The integral cross section for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 96-97 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the integrated 96-97 E+ P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The double differential cross section for the 98-99 E- P NC scattering data.
The integral cross section for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 98-99 E- P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the integrated 98-99 E- P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The double differential cross section for the 99-00 E+ P NC scattering data.
The integral cross section for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
Breakdown of the uncorrelated and correlated systematic errors for the integrated 99-00 E+ P NC scattering data.
Mean values and differential distributions of event-shape variables have been studied in neutral current deep inelastic scattering using an integrated {luminosity} of 82.2 pb$^{-1}$ collected with the ZEUS detector at HERA. The kinematic range was $80 < Q^2 < 20 480\gev^2$ and $0.0024 < x < 0.6$, where $Q^2$ is the virtuality of the exchanged boson and $x$ is the Bjorken variable. The data are compared with a model based on a combination of next-to-leading-order QCD calculations with next-to-leading-logarithm corrections and the Dokshitzer-Webber non-perturbative power corrections. The power-correction method provides a reasonable description of the data for all event-shape variables studied. Nevertheless, the lack of consistency of the determination of $\alpha_s$ and of the non-perturbative parameter of the model, $\albar$, suggests the importance of higher-order processes that are not yet included in the model.
Mean value of the event shape variable 1-THRUST(C=T).
Mean value of the event shape variable B(C=T).
Mean value of the event shape variable RHO**2.
Mean value of the event shape variable C-PARAM.
Mean value of the event shape variable 1-THRUST(C=G).
Mean value of the event shape variable B(C=G).
Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.
Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.
Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.
Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.
Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.
Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.
Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.
Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.
Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.
Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.
Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.
Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.
Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.
Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.
Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.
Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.
Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.
Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.
Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.
Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.
Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.
Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.
Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.
Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.
Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.
Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.
Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.
Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.
Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.
Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.
Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.
Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.
Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.
Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.
Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.
Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.
Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.
Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.
Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.
Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.
Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.
Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.
Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.
Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.
Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.
Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.
Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.
Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.
Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.
Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.
Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.
Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.
Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.
Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.
Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.
Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.
Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.
Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.
Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.
Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.
Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.
Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.
Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.
Deep inelastic scattering and its diffractive component, ep -> e'gamma*p ->e'XN, have been studied at HERA with the ZEUS detector using an integrated luminosity of 4.2 pb-1. The measurement covers a wide range in the gamma*p c.m. energy W (37 - 245 GeV), photon virtuality Q2 (2.2 - 80 GeV2) and mass Mx. The diffractive cross section for Mx > 2 GeV rises strongly with W: the rise is steeper with increasing Q2. The latter observation excludes the description of diffractive deep inelastic scattering in terms of the exchange of a single Pomeron. The ratio of diffractive to total cross section is constant as a function of W, in contradiction to the expectation of Regge phenomenology combined with a naive extension of the optical theorem to gamma*p scattering. Above Mx of 8 GeV, the ratio is flat with Q2, indicating a leading-twist behaviour of the diffractive cross section. The data are also presented in terms of the diffractive structure function, F2D(3)(beta,xpom,Q2), of the proton. For fixed beta, the Q2 dependence of xpom F2D(3) changes with xpom in violation of Regge factorisation. For fixed xpom, xpom F2D(3) rises as beta -> 0, the rise accelerating with increasing Q2. These positive scaling violations suggest substantial contributions of perturbative effects in the diffractive DIS cross section.
Measurement of the proton structure function F2 at Q**2 = 2.7 GeV**2.
Measurement of the proton structure function F2 at Q**2 = 4.0 GeV**2.
Measurement of the proton structure function F2 at Q**2 = 6.0 GeV**2.
Measurement of the proton structure function F2 at Q**2 = 8.0 GeV**2.
Measurement of the proton structure function F2 at Q**2 = 14.0 GeV**2.
Measurement of the proton structure function F2 at Q**2 = 27.0 GeV**2.
Measurement of the proton structure function F2 at Q**2 = 55.0 GeV**2.
Measurement of the proton total cross section for GAMMA* P scattering at Q**2 = 2.7 GeV.
Measurement of the proton total cross section for GAMMA* P scattering at Q**2 = 4.0 GeV.
Measurement of the proton total cross section for GAMMA* P scattering at Q**2 = 6.0 GeV.
Measurement of the proton total cross section for GAMMA* P scattering at Q**2 = 8.0 GeV.
Measurement of the proton total cross section for GAMMA* P scattering at Q**2 = 14.0 GeV.
Measurement of the proton total cross section for GAMMA* P scattering at Q**2 = 27.0 GeV.
Measurement of the proton total cross section for GAMMA* P scattering at Q**2 = 55.0 GeV.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 1.2 GeV and Q**2 = 2.7 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 1.2 GeV and Q**2 = 4.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 1.2 GeV and Q**2 = 6.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 1.2 GeV and Q**2 = 8.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 1.2 GeV and Q**2 = 14.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 1.2 GeV and Q**2 = 27.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 1.2 GeV and Q**2 = 55.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 3.0 GeV and Q**2 = 2.7 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 3.0 GeV and Q**2 = 4.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 3.0 GeV and Q**2 = 6.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 3.0 GeV and Q**2 = 8.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 3.0 GeV and Q**2 = 14.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 3.0 GeV and Q**2 = 27.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 3.0 GeV and Q**2 = 55.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 6.0 GeV and Q**2 = 2.7 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 6.0 GeV and Q**2 = 4.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 6.0 GeV and Q**2 = 6.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 6.0 GeV and Q**2 = 8.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 6.0 GeV and Q**2 = 14.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 6.0 GeV and Q**2 = 27.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 6.0 GeV and Q**2 = 55.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 11.0 GeV and Q**2 = 2.7 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 11.0 GeV and Q**2 = 4.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 11.0 GeV and Q**2 = 6.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 11.0 GeV and Q**2 = 8.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 11.0 GeV and Q**2 = 14.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 11.0 GeV and Q**2 = 27.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 11.0 GeV and Q**2 = 55.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 20.0 GeV and Q**2 = 2.7 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 20.0 GeV and Q**2 = 4.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 20.0 GeV and Q**2 = 6.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 20.0 GeV and Q**2 = 8.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 20.0 GeV and Q**2 = 14.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 20.0 GeV and Q**2 = 27.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 20.0 GeV and Q**2 = 55.0 GeV**2.
Cross section for the diffractive scattering process GAMMA* P --> DD X for a diffractive mass of 30.0 GeV and Q**2 = 2.7 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 0.28 to 2 GeV, to the total cross section for Q**2 = 2.7 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 0.28 to 2 GeV, to the total cross section for Q**2 = 4.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 0.28 to 2 GeV, to the total cross section for Q**2 = 6.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 0.28 to 2 GeV, to the total cross section for Q**2 = 8.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 0.28 to 2 GeV, to the total cross section for Q**2 = 14.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 0.28 to 2 GeV, to the total cross section for Q**2 = 27.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 0.28 to 2 GeV, to the total cross section for Q**2 = 55.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 2 to 4 GeV, to the total cross section for Q**2 = 2.7 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 2 to 4 GeV, to the total cross section for Q**2 = 4.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 2 to 4 GeV, to the total cross section for Q**2 = 6.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 2 to 4 GeV, to the total cross section for Q**2 = 8.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 2 to 4 GeV, to the total cross section for Q**2 = 14.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 2 to 4 GeV, to the total cross section for Q**2 = 27.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 2 to 4 GeV, to the total cross section for Q**2 = 55.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 4 to 8 GeV, to the total cross section for Q**2 = 2.7 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 4 to 8 GeV, to the total cross section for Q**2 = 4.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 4 to 8 GeV, to the total cross section for Q**2 = 6.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 4 to 8 GeV, to the total cross section for Q**2 = 8.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 4 to 8 GeV, to the total cross section for Q**2 = 14.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 4 to 8 GeV, to the total cross section for Q**2 = 27.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 4 to 8 GeV, to the total cross section for Q**2 = 55.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 8 to 15 GeV, to the total cross section for Q**2 = 2.7 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 8 to 15 GeV, to the total cross section for Q**2 = 4.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 8 to 15 GeV, to the total cross section for Q**2 = 6.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 8 to 15 GeV, to the total cross section for Q**2 = 8.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 8 to 15 GeV, to the total cross section for Q**2 = 14.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 8 to 15 GeV, to the total cross section for Q**2 = 27.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 8 to 15 GeV, to the total cross section for Q**2 = 55.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 15 to 25 GeV, to the total cross section for Q**2 = 2.7 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 15 to 25 GeV, to the total cross section for Q**2 = 4.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 15 to 25 GeV, to the total cross section for Q**2 = 6.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 15 to 25 GeV, to the total cross section for Q**2 = 8.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 15 to 25 GeV, to the total cross section for Q**2 = 14.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 15 to 25 GeV, to the total cross section for Q**2 = 27.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 15 to 25 GeV, to the total cross section for Q**2 = 55.0 GeV**2.
Ratio of the cross sections for diffractive scattering GAMMA* P --> DD X integrated over the diffractive mass 25 to 35 GeV, to the total cross section for Q**2 = 2.7 GeV**2.
Ratio of the total diffractive cross section observed to the total cross section.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 2.7 GeV**2 and BETA = 0.6522.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 2.7 GeV**2 and BETA = 0.2308.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 2.7 GeV**2 and BETA = 0.0698.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 2.7 GeV**2 and BETA = 0.0218.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 2.7 GeV**2 and BETA = 0.0067.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 2.7 GeV**2 and BETA = 0.0030.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 4.0 GeV**2 and BETA = 0.7353.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 4.0 GeV**2 and BETA = 0.3077.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 4.0 GeV**2 and BETA = 0.1000.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 4.0 GeV**2 and BETA = 0.0320.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 4.0 GeV**2 and BETA = 0.0099.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 4.0 GeV**2 and BETA = 0.0044.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 6.0 GeV**2 and BETA = 0.8065.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 6.0 GeV**2 and BETA = 0.4000.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 6.0 GeV**2 and BETA = 0.1429.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 6.0 GeV**2 and BETA = 0.0472.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 6.0 GeV**2 and BETA = 0.0148.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 6.0 GeV**2 and BETA = 0.0066.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 8.0 GeV**2 and BETA = 0.8475.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 8.0 GeV**2 and BETA = 0.4706.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 8.0 GeV**2 and BETA = 0.1818.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 8.0 GeV**2 and BETA = 0.0620.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 8.0 GeV**2 and BETA = 0.0196.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 8.0 GeV**2 and BETA = 0.0088.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 14.0 GeV**2 and BETA = 0.9067.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 14.0 GeV**2 and BETA = 0.6087.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 14.0 GeV**2 and BETA = 0.2800.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 14.0 GeV**2 and BETA = 0.1037.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 14.0 GeV**2 and BETA = 0.0338.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 14.0 GeV**2 and BETA = 0.0153.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 27.0 GeV**2 and BETA = 0.9494.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 27.0 GeV**2 and BETA = 0.7500.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 27.0 GeV**2 and BETA = 0.4286.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 27.0 GeV**2 and BETA = 0.1824.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 27.0 GeV**2 and BETA = 0.0632.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 27.0 GeV**2 and BETA = 0.0291.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 55.0 GeV**2 and BETA = 0.9745.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 55.0 GeV**2 and BETA = 0.8594.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 55.0 GeV**2 and BETA = 0.6044.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 55.0 GeV**2 and BETA = 0.3125.
The diffractive structure function F2(NAME=D3) multiplied by X(NAME=POMERON), for Q**2 = 55.0 GeV**2 and BETA = 0.1209.
The diffractive structure function of the proton multiplied by X(NAME=POMERON) at the point X(POMERON) = 0.01 and Q**2 = 2.7 GeV**2.
The diffractive structure function of the proton multiplied by X(NAME=POMERON) at the point X(POMERON) = 0.01 and Q**2 = 4.0 GeV**2.
The diffractive structure function of the proton multiplied by X(NAME=POMERON) at the point X(POMERON) = 0.01 and Q**2 = 6.0 GeV**2.
The diffractive structure function of the proton multiplied by X(NAME=POMERON) at the point X(POMERON) = 0.01 and Q**2 = 8.0 GeV**2.
The diffractive structure function of the proton multiplied by X(NAME=POMERON) at the point X(POMERON) = 0.01 and Q**2 = 14.0 GeV**2.
The diffractive structure function of the proton multiplied by X(NAME=POMERON) at the point X(POMERON) = 0.01 and Q**2 = 27.0 GeV**2.
The diffractive structure function of the proton multiplied by X(NAME=POMERON) at the point X(POMERON) = 0.01 and Q**2 = 55.0 GeV**2.
Deep inelastic scattering and its diffractive component, $ep \to e^{\prime}\gamma^* p \to e^{\prime}XN$, have been studied at HERA with the ZEUS detector using an integrated luminosity of 52.4 pb$^{-1}$. The $M_X$ method has been used to extract the diffractive contribution. A wide range in the centre-of-mass energy $W$ (37 -- 245 GeV), photon virtuality $Q^2$ (20 -- 450 GeV$^2$) and mass $M_X$ (0.28 -- 35 GeV) is covered. The diffractive cross section for $2 < M_X < 15$ GeV rises strongly with $W$, the rise becoming steeper as $Q^2$ increases. The data are also presented in terms of the diffractive structure function, $F^{\rm D(3)}_2$, of the proton. For fixed $Q^2$ and fixed $M_X$, $\xpom F^{\rm D(3)}_2$ shows a strong rise as $\xpom \to 0$, where $\xpom$ is the fraction of the proton momentum carried by the Pomeron. For Bjorken-$x < 1 \cdot 10^{-3}$, $\xpom F^{\rm D(3)}_2$ shows positive $\log Q^2$ scaling violations, while for $x \ge 5 \cdot 10^{-3}$ negative scaling violations are observed. The diffractive structure function is compatible with being leading twist. The data show that Regge factorisation is broken.
Proton structure function F2 at Q**2 = 25 GeV**2.
Proton structure function F2 at Q**2 = 35 GeV**2.
Proton structure function F2 at Q**2 = 45 GeV**2.
Proton structure function F2 at Q**2 = 55 GeV**2.
Proton structure function F2 at Q**2 = 70 GeV**2.
Proton structure function F2 at Q**2 = 90 GeV**2.
Proton structure function F2 at Q**2 = 120 GeV**2.
Proton structure function F2 at Q**2 = 190 GeV**2.
Proton structure function F2 at Q**2 = 320 GeV**2.
Total GAMMA* P cross section as a function of W at Q**2 = 25 GeV**2.
Total GAMMA* P cross section as a function of W at Q**2 = 35 GeV**2.
Total GAMMA* P cross section as a function of W at Q**2 = 45 GeV**2.
Total GAMMA* P cross section as a function of W at Q**2 = 55 GeV**2.
Total GAMMA* P cross section as a function of W at Q**2 = 70 GeV**2.
Total GAMMA* P cross section as a function of W at Q**2 = 90 GeV**2.
Total GAMMA* P cross section as a function of W at Q**2 = 120 GeV**2.
Total GAMMA* P cross section as a function of W at Q**2 = 190 GeV**2.
Total GAMMA* P cross section as a function of W at Q**2 = 320 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 1.2 GeV for Q**2 = 25 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 1.2 GeV for Q**2 = 35 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 1.2 GeV for Q**2 = 45 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 1.2 GeV for Q**2 = 55 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 1.2 GeV for Q**2 = 70 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 1.2 GeV for Q**2 = 90 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 1.2 GeV for Q**2 = 120 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 1.2 GeV for Q**2 = 190 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 1.2 GeV for Q**2 = 320 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 3 GeV for Q**2 = 25 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 3 GeV for Q**2 = 35 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 3 GeV for Q**2 = 45 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 3 GeV for Q**2 = 55 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 3 GeV for Q**2 = 70 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 3 GeV for Q**2 = 90 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 3 GeV for Q**2 = 120 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 3 GeV for Q**2 = 190 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 3 GeV for Q**2 = 320 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 6 GeV for Q**2 = 25 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 6 GeV for Q**2 = 35 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 6 GeV for Q**2 = 45 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 6 GeV for Q**2 = 55 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 6 GeV for Q**2 = 70 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 6 GeV for Q**2 = 90 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 6 GeV for Q**2 = 120 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 6 GeV for Q**2 = 190 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 6 GeV for Q**2 = 320 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 11 GeV for Q**2 = 25 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 11 GeV for Q**2 = 35 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 11 GeV for Q**2 = 45 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 11 GeV for Q**2 = 55 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 11 GeV for Q**2 = 70 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 11 GeV for Q**2 = 90 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 11 GeV for Q**2 = 120 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 11 GeV for Q**2 = 190 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 11 GeV for Q**2 = 320 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 20 GeV for Q**2 = 25 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 20 GeV for Q**2 = 35 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 20 GeV for Q**2 = 45 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 20 GeV for Q**2 = 55 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 20 GeV for Q**2 = 70 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 20 GeV for Q**2 = 90 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 20 GeV for Q**2 = 120 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 20 GeV for Q**2 = 190 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 20 GeV for Q**2 = 320 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 30 GeV for Q**2 = 25 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 30 GeV for Q**2 = 35 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 30 GeV for Q**2 = 45 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 30 GeV for Q**2 = 55 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 30 GeV for Q**2 = 70 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 30 GeV for Q**2 = 90 GeV**2.
Cross section for diffractive scattering GAMMA* P --> DD X where M(DD) < 2.3 GeV and M(X) = 30 GeV for Q**2 = 190 GeV**2.
The diffractive cross section multiplied by (Q**2)*(Q**2+M(X)**2) as a function of Q**2 for W=220 GeV and M(X) = 1.2 GeV.
The diffractive cross section multiplied by (Q**2)*(Q**2 M(X)**2) as a function of Q**2 for W=220 GeV and M(X) = 3 GeV.
The diffractive cross section multiplied by (Q**2)*(Q**2 M(X)**2) as a function of Q**2 for W=220 GeV and M(X) = 6 GeV.
The diffractive cross section multiplied by (Q**2)*(Q**2 M(X)**2) as a function of Q**2 for W=220 GeV and M(X) = 11 GeV.
The diffractive cross section multiplied by (Q**2)*(Q**2 M(X)**2) as a function of Q**2 for W=220 GeV and M(X) = 20 GeV.
The diffractive cross section multiplied by (Q**2)*(Q**2 M(X)**2) as a function of Q**2 for W=220 GeV and M(X) = 30 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 0.28 to 2 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 0.28 to 2 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 0.28 to 2 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 0.28 to 2 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 0.28 to 2 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 0.28 to 2 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 0.28 to 2 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 0.28 to 2 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 0.28 to 2 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 2 to 4 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 2 to 4 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 2 to 4 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 2 to 4 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 2 to 4 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 2 to 4 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 2 to 4 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 2 to 4 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 2 to 4 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 4 to 8 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 4 to 8 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 4 to 8 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 4 to 8 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 4 to 8 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 4 to 8 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 4 to 8 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 4 to 8 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 4 to 8 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 8 to 15 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 8 to 15 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 8 to 15 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 8 to 15 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 8 to 15 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 8 to 15 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 8 to 15 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 8 to 15 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 8 to 15 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 15 to 25 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 15 to 25 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 15 to 25 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 15 to 25 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 15 to 25 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 15 to 25 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 15 to 25 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 15 to 25 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 15 to 25 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 25 to 35 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 25 to 35 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 25 to 35 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 25 to 35 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 25 to 35 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 25 to 35 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 25 to 35 GeV.
Ratio of the cross section for diffractive scattering to total cross section integrated over the interval M(X) = 0.28 to 35 GeV for W = 220 GeV.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.9455 and Q**2 = 25 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.7353 and Q**2 = 25 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.4098 and Q**2 = 25 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.1712 and Q**2 = 25 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.0588 and Q**2 = 25 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.0270 and Q**2 = 25 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.9605 and Q**2 = 35 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.7955 and Q**2 = 35 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.4930 and Q**2 = 35 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.2244 and Q**2 = 35 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.0805 and Q**2 = 35 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.0374 and Q**2 = 35 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.9690 and Q**2 = 45 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.8333 and Q**2 = 45 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.5556 and Q**2 = 45 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.2711 and Q**2 = 45 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.1011 and Q**2 = 45 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.0476 and Q**2 = 45 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.9745 and Q**2 = 55 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.8594 and Q**2 = 55 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.6044 and Q**2 = 55 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.3125 and Q**2 = 55 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.1209 and Q**2 = 55 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.0576 and Q**2 = 55 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.9798 and Q**2 = 70 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.8861 and Q**2 = 70 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.6604 and Q**2 = 70 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.3665 and Q**2 = 70 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.1489 and Q**2 = 70 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.0722 and Q**2 = 70 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.9843 and Q**2 = 90 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.9091 and Q**2 = 90 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.7143 and Q**2 = 90 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.4265 and Q**2 = 90 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.1837 and Q**2 = 90 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.0909 and Q**2 = 90 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.9881 and Q**2 = 120 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.9302 and Q**2 = 120 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.7692 and Q**2 = 120 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.4979 and Q**2 = 120 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.2308 and Q**2 = 120 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.9925 and Q**2 = 190 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.9548 and Q**2 = 190 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.8407 and Q**2 = 190 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.6109 and Q**2 = 190 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.3220 and Q**2 = 190 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.1743 and Q**2 = 190 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.9726 and Q**2 = 320 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.8989 and Q**2 = 320 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.7256 and Q**2 = 320 GeV**2.
The diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON) for BETA = 0.4444 and Q**2 = 320 GeV**2.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.00015 and BETA = 0.700.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.00015 and BETA = 0.900.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0003 and BETA = 0.400.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0003 and BETA = 0.700.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0003 and BETA = 0.900.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0006 and BETA = 0.400.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0006 and BETA = 0.700.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0006 and BETA = 0.900.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0012 and BETA = 0.125.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0012 and BETA = 0.400.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0012 and BETA = 0.700.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0012 and BETA = 0.900.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0012 and BETA = 0.970.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0025 and BETA = 0.025.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0025 and BETA = 0.125.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0025 and BETA = 0.400.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0025 and BETA = 0.700.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0025 and BETA = 0.900.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0025 and BETA = 0.970.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0050 and BETA = 0.025.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.0050 and BETA = 0.125.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.005 and BETA = 0.400.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.005 and BETA = 0.700.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.005 and BETA = 0.900.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.005 and BETA = 0.970.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.010 and BETA = 0.005.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.010 and BETA = 0.025.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.010 and BETA = 0.125.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.010 and BETA = 0.400.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.010 and BETA = 0.700.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.010 and BETA = 0.900.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.010 and BETA = 0.970.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.020 and BETA = 0.005.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.020 and BETA = 0.025.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.020 and BETA = 0.125.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.020 and BETA = 0.400.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.020 and BETA = 0.700.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.020 and BETA = 0.900.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.020 and BETA = 0.970.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.030 and BETA = 0.025.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.030 and BETA = 0.125.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.030 and BETA = 0.040.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.030 and BETA = 0.700.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.030 and BETA = 0.900.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.030 and BETA = 0.970.. Statistical and systematic errors added in quadrature.
Diffractive structure function F2(NAME=D3) for fixed X(NAME=POMERON) = 0.060 and BETA = 0.970.. Statistical and systematic errors added in quadrature.
Results are presented onK+p elastic scattering and on the reactionK+p→K+pπ+π− at 70 GeV/c. For the
.
.
.
INTEGRATION OVER RANGE OF ABS(T) FROM 0 TO 1 GEV.
ELASTIC DIFFERENTIAL CROSS SECTION AT T=0 DERIVED FROM THE OPTICAL THEOREM.
.
DIFFRACTIVE CROSS SECTION.
.
'K*(892)' REACTION CORRECTED FOR ALL UNSEEN DECAY MODES. 'K*(1430)' REACTION CORRECTED ONLY FOR K*(1430)0-->K0 PI0 DECAY MODE.
Charm production in deep inelastic scattering has been measured with the ZEUS detector at HERA using an integrated luminosity of 82 pb^{-1}. Charm has been tagged by reconstructing D^{*+}, D^0, D^{+} and D_s^+ (+ c.c.) charm mesons. The charm hadrons were measured in the kinematic range p_T(D^{*+},D^0,D^{+}) > 3 GeV, p_T(D_s^+)>2 GeV and |\eta(D)| < 1.6 for 1.5 < Q^2 < 1000 GeV^2 and 0.02 < y < 0.7. The production cross sections were used to extract charm fragmentation ratios and the fraction of c quarks hadronising into a particular charm meson in the kinematic range considered. The cross sections were compared to the predictions of next-to-leading-order QCD, and extrapolated to the full kinematic region in p_T(D) and \eta(D) in order to determine the open-charm contribution, F_2^{c\bar{c}}(x,Q^2), to the proton structure function F_2.
Production cross section for all D0 mesons, those not originating fom D* decays and those originating from D* decays.
Production cross section for additional D* mesons (not decaying to D0) and all D* mesons.
Production cross section for D+ mesons.
Production cross section for D/S+ mesons.
Measured differential cross sections for D0 (not coming from D*+ decay) and D+.
Measured differential cross sections for D0 (not coming from D*+ decay) and D+.
Measured differential cross sections for D0 (not coming from D*+ decay) and D+.
Measured differential cross sections for D0 (not coming from D*+ decay) and D+.
Measured differential cross sections for D/S+.
Measured differential cross sections for D/S+.
Measured differential cross sections for D/S+.
Measured differential cross sections for D/S+.
Measured cross sections for D0 not coming fom a D*+ decay, and D+ as a function of Y.
Measured cross sections for D0 not coming fom a D*+ decay, and D+ as a function of Y.
Measured cross sections for D0 not coming fom a D*+ decay, and D+ as a function of Y.
Measured cross sections for D/S+ as a function of Y.
Measured cross sections for D/S+ as a function of Y.
Measured cross sections for D/S+ as a function of Y.
The extracted values of F2(CC) from the production cross section of D0 (not coming from D*+ decay), D_ and D/S+.
The extracted values of F2(CC) from the production cross section of D0 (not coming from D*+ decay), D_ and D/S+.
The extracted values of F2(CC) from the production cross section of D0 (not coming from D*+ decay), D_ and D/S+.
The extracted values of F2(CC) from a combination of the production cross section of D0 (not coming from D*+ decay), D_ and D/S+.
The extracted values of F2(CC) from a combination of the production cross section of D0 (not coming from D*+ decay), D_ and D/S+.
The extracted values of F2(CC) from a combination of the production cross section of D0 (not coming from D*+ decay), D_ and D/S+.
Inclusive-jet and dijet differential cross sections have been measured in neutral current deep inelastic ep scattering for exchanged boson virtualities Q2 > 125 GeV2 with the ZEUS detector at HERA using an integrated luminosity of 82 pb-1. Jets were identified in the Breit frame using the kt cluster algorithm. Jet cross sections are presented as functions of several kinematic and jet variables. The results are also presented in different regions of Q2. Next-to-leading-order QCD calculations describe the measurements well. Regions of phase space where the theoretical uncertainties are small have been identified. Measurements in these regions have the potential to constrain the gluon density in the proton when used as inputs to global fits of the proton parton distribution functions.
Dijet cross section as a function of Q**2 in the Breit frame.
Dijet cross section as a function of Bjorken X in the Breit frame.
Dijet cross section as a function of the mean ET of the jets in the Breit frame.
Dijet cross section as a function of the mass of the dijet system in the Breit frame.
Dijet cross section as a function of the jet pseudorapidity difference in the Breit frame.
Dijet cross section as a function of the fraction of the proton momentum taken by the interacting parton in the Breit frame.
Dijet cross sections as a function of the parton momentum taken by the interacting proton in the Breit frames in the Q**2 region 125 to 250 GeV**2.
Dijet cross sections as a function of the parton momentum taken by the interacting proton in the Breit frames in the Q**2 region 250 to 500 GeV**2.
Dijet cross sections as a function of the parton momentum taken by the interacting proton in the Breit frames in the Q**2 region 500 to 1000 GeV**2.
Dijet cross sections as a function of the parton momentum taken by the interacting proton in the Breit frames in the Q**2 region 1000 to 2000 GeV**2.
Dijet cross sections as a function of the parton momentum taken by the interacting proton in the Breit frames in the Q**2 region 2000 to 5000 GeV**2.
Inclusive jet cross sections as a function of jet ET in the Breit frames in the Q**2 region 125 to 250 GeV**2.
Inclusive jet cross sections as a function of jet ET in the Breit frames in the Q**2 region 250 to 500 GeV**2.
Inclusive jet cross sections as a function of jet ET in the Breit frames in the Q**2 region 500 to 1000 GeV**2.
Inclusive jet cross sections as a function of jet ET in the Breit frames in the Q**2 region 1000 to 2000 GeV**2.
Inclusive jet cross sections as a function of jet ET in the Breit frames in the Q**2 region 2000 to 5000 GeV**2.
Inclusive jet cross sections as a function of jet ET in the Breit frames in the Q**2 region 5000 to 10000 GeV**2.
Differential inclusive-jet cross sections have been measured for different jet radii in neutral current deep inelastic ep scattering for boson virtualities Q^2 > 125 GeV^2 with the ZEUS detector at HERA using an integrated luminosity of 81.7 pb^-1. Jets were identified in the Breit frame using the k_T cluster algorithm in the longitudinally inclusive mode for different values of the jet radius R. Differential cross sections are presented as functions of Q^2 and the jet transverse energy, E_T,B^jet. The dependence on R of the inclusive-jet cross section has been measured for Q^2 > 125 and 500 GeV^2 and found to be linear with R in the range studied. Next-to-leading-order QCD calculations give a good description of the measurements for 0.5 <= R <= 1. A value of alpha_s(M_Z) has been extracted from the measurements of the inclusive-jet cross-section dsigma/dQ^2 with R=1 for Q^2 > 500 GeV^2: alpha_s(M_Z) = 0.1207 +- 0.0014 (stat.) -0.0033 +0.0035 (exp.) -0.0023 +0.0022 (th.). The variation of alpha_s with E_T,B^jet is in good agreement with the running of alpha_s as predicted by QCD.
No description provided.
No description provided.
No description provided.
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No description provided.
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No description provided.
The production of energetic neutrons in $ep$ collisions has been studied with the ZEUS detector at HERA. The neutron energy and $p_T^2$ distributions were measured with a forward neutron calorimeter and tracker in a $40 \pb^{-1}$ sample of inclusive deep inelastic scattering (DIS) data and a $6 \pb^{-1}$ sample of photoproduction data. The neutron yield in photoproduction is suppressed relative to DIS for the lower neutron energies and the neutrons have a steeper $p_T^2$ distribution, consistent with the expectation from absorption models. The distributions are compared to HERA measurements of leading protons. The neutron energy and transverse-momentum distributions in DIS are compared to Monte Carlo simulations and to the predictions of particle exchange models. Models of pion exchange incorporating absorption and additional secondary meson exchanges give a good description of the data.
Ratio of leading neutron to inclusive cross sections integrated to the full PT range.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.
The intercepts and slope for the exponential parameterisation of the differential cross section of the form A exp(-B*PT**2). Errors do not contain additional 2.1 PCT uncertainty on the intercepts.
Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.
Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.
The intercepts and slope for the exponential parameterisation of the differential cross section of the form Aexp(-B*PT**2) for the photoproduction sample. The errors do not contain the additional 2.1 PCT uncertainty on the DIS intercepts, nor the additional 5.1 PCT uncertainty on the photoproduction intercepts.
The intercept and slope for the exponential parameterisation of the differential cross section of the form Aexp(-B*PT**2) for the low-Q**2 DIS sample. The errors do not contain the additional 2.1 PCT uncertainty on the DIS intercepts, nor the additional 5.1 PCT uncertainty on the photoproduction intercepts.
The intercept and slope for the exponential parameterisation of the differential cross section of the form Aexp(-B*PT**2) for the mid-Q**2 DIS sample. The errors do not contain the additional 2.1 PCT uncertainty on the DIS intercepts, nor the additional 5.1 PCT uncertainty on the photoproduction intercepts.
The intercept and slope for the exponential parameterisation of the differential cross section of the form Aexp(-B*PT**2) for the high-Q**2 DIS sample. The errors do not contain the additional 2.1 PCT uncertainty on the DIS intercepts, nor the additional 5.1 PCT uncertainty on the photoproduction intercepts.
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