Forward-jet production in deep inelastic ep scattering at HERA

The ZEUS collaboration Chekanov, S. ; Derrick, M. ; Magill, S. ; et al.
Eur.Phys.J.C 52 (2007) 515-530, 2007.
Inspire Record 756364 DOI 10.17182/hepdata.45524

Forward jet cross sections have been measured in neutral current deep inelastic scattering at low Bjorken-x with the ZEUS detector at HERA using an integrated luminosity of ${81.8 \rm pb}^{-1}$. Measurements are presented for inclusive forward jets as well as for forward jets accompanied by a dijet system. The explored phase space, with jet pseudorapidity up to 4.3 is expected to be particularly sensitive to the dynamics of QCD parton evolution at low x. The measurements are compared to fixed-order QCD calculations and to leading-order parton-shower Monte Carlo models.

14 data tables

Differential cross section DSIG/DQ**2 in bins of Q**2 .

Differential cross section DSIG/DX in bins of X .

Differential cross section DSIG/DET(P=4) in bins of ET(P=4) .

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Inclusive-jet and dijet cross sections in deep inelastic scattering at HERA.

The ZEUS collaboration Chekanov, S. ; Derrick, M. ; Magill, S. ; et al.
Nucl.Phys.B 765 (2007) 1-30, 2007.
Inspire Record 724050 DOI 10.17182/hepdata.45641

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.

17 data tables

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.

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