2012
DOI: 10.1140/epjc/s10052-012-1910-8
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Measurement of the azimuthal correlation between the most forward jet and the scattered positron in deep-inelastic scattering at HERA

Abstract: Deep-inelastic positron-proton scattering events at low photon virtuality, Q 2 , with a forward jet, produced at small angles with respect to the proton beam, are measured with the H1 detector at HERA. A subsample of events with an additional jet in the central region is also studied. For both samples, differential cross sections and normalised distributions are measured as a function of the aza e-mail: krueger@mail.desy.de b Also at Physics Department, National Technical University, Zografou Campus, GR-15773 … Show more

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Cited by 13 publications
(10 citation statements)
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“…The relevant observable sensitive to the final-state momentum inbalance, and therefore potentially to saturation, is the angle between the final-state electron and the two jets (this observable has been studied in other contexts in e.g. [22,23]). One can observe that different rates of saturation included in the Kutak-Sapeta gluon distributions [24] lead to distinguishable shapes for the angle distribution.…”
Section: Dis With Katiementioning
confidence: 99%
“…The relevant observable sensitive to the final-state momentum inbalance, and therefore potentially to saturation, is the angle between the final-state electron and the two jets (this observable has been studied in other contexts in e.g. [22,23]). One can observe that different rates of saturation included in the Kutak-Sapeta gluon distributions [24] lead to distinguishable shapes for the angle distribution.…”
Section: Dis With Katiementioning
confidence: 99%
“…It is important to study especially the behaviour of the solution of the CCFM with the splitting function with only terms singular in z = 0 and z = 1 (7). The most interesting is the x distribution.…”
Section: Different Versions Of the Ccfm Equationmentioning
confidence: 99%
“…Let us do a careful analysis of what happens at z → 0 taking the splitting function (7). Let us calculate the Sudakov form factor with fixed p = |k| = Q0 = 1 GeV to see, that for fixed |q| it grows with z getting smaller:…”
Section: Different Versions Of the Ccfm Equationmentioning
confidence: 99%
See 1 more Smart Citation
“…These MC generators usually use the DokshitzerGribov-Lipatov-Altarelli-Parisi (DGLAP) evolution equations [1][2][3][4] approximation. Alternative approaches like the Balitski-Fadin-Kuraev-Lipatov (BFKL) approximation [5][6][7] or the CiafaloniCatani-Fiorani-Marchesini (CCFM) approach [8][9][10][11] have since long been investigated, especially at HERA [12][13][14][15][16][17]. However, although in some cases significant discrepancies between data and DGLAP-based models have been observed, it has not been possible to pin down BFKL or CCFM effects in a convincing manner.…”
Section: Introductionmentioning
confidence: 99%