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Large Inclusive Charged Particle Distributions in Deep Inelastic Scattering Events at HERA

The ZEUS collaboration Derrick, M. ; Krakauer, D. ; Magill, S. ; et al.

Z.Phys.C 70 (1996) 1-16, 1996.

Inspire Record 402646 DOI 10.17182/hepdata.44930

A measurement of inclusive charged particle distributions in deep inelastic $ep$ scattering for $\gamma~* p$ centre-of-mass energies $75< W < 175$GeV and momentum transfer squared $10< Q~2 < 160$GeV$~2$ from the ZEUS detector at HERA is presented. The differential charged particle rates in the $\gamma~* p$ centre-of-mass system as a function of the scaled longitudinal momentum, $x_F$, and of the transverse momentum, $p_t~*$ and $<\!\!p_t~{*\,2}\!\!>\,\,$ , as a function of $x_F$, $W$ and $Q~2$ are given. Separate distributions are shown for events with (LRG) and without (NRG) a rapidity gap with respect to the proton direction. The data are compared with results from experiments at lower beam energies, with the naive quark parton model and with parton models including perturbative QCD corrections. The comparison shows the importance of the higher order QCD processes. Significant differences of the inclusive charged particle rates between NRG and LRG events at the same $W$ are observed. The value of $<\!\!p_t~{*\,2}\!\!>\,\,$ for LRG events with a hadronic mass $M_X$, which excludes the forward produced baryonic system, is similar to the $<\!\!p_t~{*\,2}\!\!>\,\,$ value observed in fixed target experiments at $W \approx M_X$.

11 data tables

Table 1

Differential multiplicites for NRG events.. XL is parallel to the virtual photon axis.

Table 2

Differential multiplicites for NRG events.. PT is relative to the virtual photon axis.

Table 3

Mean PT**2 for NRG events.. PT is relative to the virtual photon axis.

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Study of the photon remnant in resolved photoproduction at HERA

The ZEUS collaboration Derrick, M. ; Krakauer, D. ; Magill, S. ; et al.

Phys.Lett.B 354 (1995) 163-177, 1995.

Inspire Record 392038 DOI 10.17182/hepdata.44946

Photoproduction at HERA is studied in $ep$ collisions, with the ZEUS detector, for $\gamma p$ centre-of-mass energies ranging from 130-270 GeV. A sample of events with two high-$p_T$ jets ($p_T > 6$ GeV, $\eta <1.6$) and a third cluster in the approximate direction of the electron beam is isolated using a clustering algorithm. These events are mostly due to resolved photoproduction. The third cluster is identified as the photon remnant. Its properties, such as the transverse and longitudinal energy flows around the axis of the cluster, are consistent with those commonly attributed to jets, and in particular with those found for the two jets in these events. The mean value of the photon remnant $p_T$ with respect to the beam axis is measured to be $2.1 \pm 0.2$ GeV, which demonstrates substantial mean transverse momenta for the photon remnant.

3 data tables

Table 1

Pseudorapidity distribution of the third cluster corrected to the hadron level.

Table 2

Corrected PT distribution of the third cluster corrected to the hadron level.

Table 3

Corrected Energy distribution of the third cluster corrected to the hadron level.

rivet Analysis
Properties of high mass multi - jet events at the Fermilab proton - anti-proton collider

The CDF collaboration Abe, F. ; Albrow, M.G. ; Amendolia, S.R. ; et al.

Phys.Rev.Lett. 75 (1995) 608-612, 1995.

Inspire Record 393345 DOI 10.17182/hepdata.52833

The properties of two-, three-, four-, five-, and six-jet events with multijet masses >600 GeV /c2 are compared with QCD predictions. The shapes of the multijet-mass and leading-jet-angular distributions are approximately independent of jet multiplicity and are well described by the NJETS matrix element calculation and the HERWIG parton shower Monte Carlo predictions. The observed jet transverse momentum distributions for three- and four-jet events discriminate between the matrix element and parton shower predictions, the data favoring the matrix element calculation.

19 data tables

Table 1

Exclusive 2-jet mass distribution.

Table 2

Exclusive 3-jet mass distribution.

Table 3

Exclusive 4-jet mass distribution.