Marta Łuszczak
Rzeszów University
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Publication
Featured researches published by Marta Łuszczak.
Physical Review D | 2012
Marta Łuszczak; Rafal Maciula; Antoni Szczurek
We discuss production of two pairs of
Physical Review D | 2016
Marta Łuszczak; Wolfgang Schäfer; Antoni Szczurek
c \bar c
Physical Review D | 2015
Marta Łuszczak; Antoni Szczurek; Rafal Maciula
within a simple formalism of double-parton scattering (DPS). Surprisingly very large cross sections, comparable to single-parton scattering (SPS) contribution, are predicted for LHC energies. Both total inclusive cross section as a function of energy and differential distributions for
Physical Review D | 2014
Antoni Szczurek; Marta Łuszczak; Rafal Maciula
\sqrt{s}
Physical Review D | 2015
Rafal Maciula; Antoni Szczurek; Marta Łuszczak
are shown. We discuss a perspective how to identify the double scattering contribution.
Physics Letters B | 2014
Marta Łuszczak; Wolfgang Schäfer; Antoni Szczurek
We investigate different methods to incorporate the effect of photons in hard processes. We compare the two different approaches used for calculating cross sections for the two-photon
Journal of High Energy Physics | 2018
Marta Łuszczak; Wolfgang Schäfer; Antoni Szczurek
pp\ensuremath{\rightarrow}{l}^{+}{l}^{\ensuremath{-}}X
arXiv: High Energy Physics - Phenomenology | 2016
Antoni Szczurek; Anna Cisek; Marta Łuszczak; Wolfgang Schäfer
process. In one of the approaches the photon is treated as a collinear parton in the proton. In the second approach the recently proposed
Proceedings of XXII. International Workshop on Deep-Inelastic Scattering and Related Subjects — PoS(DIS2014) | 2014
Marta Łuszczak; Antoni Szczurek; Rafal Maciula
{k}_{T}
arXiv: High Energy Physics - Phenomenology | 2013
Marta Łuszczak; Antoni Szczurek
factorization method is used. We discuss how results of the collinear parton model depend on the initial condition for the QCD evolution and discuss an approximate treatment where the photon is excluded from the combined QCD-QED evolution. We demonstrate that it is not necessary to put the photon into the evolution equation as is often done, but it is sufficient to use a simplified approach in which the photon couples to quarks and antiquarks, which by themselves undergo DGLAP evolution equations. We discuss the sensitivity of the results to the choice of structure function parametrization and experimental cuts in the