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
“…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.…”
KaTie is a parton-level event generator that allows for the use of factorization prescriptions requiring space-like initial-state partons. Some updates are presented, in particular its application to DIS.
“…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.…”
KaTie is a parton-level event generator that allows for the use of factorization prescriptions requiring space-like initial-state partons. Some updates are presented, in particular its application to DIS.
“…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%
“…The BFKL equation [3] seems to be the appropriate effective theory for describing high energy initial state radiation in the kinematic region where the Mandelstam invariants t of the momentum exchange and s of the total scattering momentum are strongly ordered: Λ 2 QCD ≪ |t| ≪ s. It is well known that the relevant phase space region is very important at the LHC, but signs of its importance were already observed at the HERA [7,8] and other colliders.…”
We solve the modified non-linear extension of the CCFM equation -KGBJS equation [1] -numerically for certain initial conditions and compare the resulting gluon Green functions with those obtained from solving the original CCFM equation and the BFKL and BK equations for the same initial conditions. We improve the low transversal momentum behaviour of the KGBJS equation by a small modification.
“…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.…”
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