Browsing by Author "Karpenko, Iu"
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Publication Charm production in high multiplicity pp events(2016-08-24) ;Werner, K. ;Guiot, B. ;Karpenko, Iu ;Pierog, T.Sophys, G.Studying proton-proton scattering at 7 TeV, the ALICE collaboration found the unexpected result that the D meson multiplicity increases more than linear as a function of the charged particle multiplicity. We try to understand this behavior using the EPOS3 approach. Two issues play an important role in this context: multiple scattering, in particular its impact on multiplicity fluctuations, and the collective hydrodynamic expansion. These data contain therefore valuable information about very basic features of the reaction mechanism in protonproton collisions.Scopus© Citations 4 - Some of the metrics are blocked by yourconsent settings
Publication Hydrodynamic flow in proton-nucleus collisions at the LHC(2014-01-01) ;Werner, K. ;Guiot, B. ;Karpenko, IuPierog, T.There is little doubt that hydrodynamic flow has been observed in heavy ion collisions at the LHC and RHIC, mainly based on results on azimuthal anisotropies, but also on particle spectra of identified particles, perfectly compatible with hydrodynamic expansions. Surprisingly, in p-Pb collisions one observes a very similar behavior. So do we see flow even in p-Pb? We will try to answer this question.Scopus© Citations 1 - Some of the metrics are blocked by yourconsent settings
Publication Jets, bulk matter, and their interaction in heavy ion collisions at the LHC(2013-01-01) ;Werner, K. ;Guiot, B. ;Karpenko, Iu ;Bleicher, M. ;Pierog, T.Porteboeuf-Houssais, S.We discuss a theoretical scheme that accounts for bulk matter, jets, and the interaction between the two. The physical picture of our approach is the following: Initial hard scatterings result in mainly longitudinal flux tubes, with transversely moving pieces carrying the pt of the partons from hard scatterings. These flux tubes constitute eventually both bulk matter (which thermalizes, flows, and finally hadronizes) and jets, according to some criteria based on partonic energy loss. High energy flux tube segments will leave the fluid, providing jet hadrons via the usual Schwinger mechanism of flux-tube breaking caused by quark-antiquark production. But the jets may also be produced at the freeze-out surface. Here we assume that the quark-antiquark needed for the flux tube breaking is provided by the fluid, with properties (momentum, flavor) determined by the fluid rather than the Schwinger mechanism. Considering transverse fluid velocities up to 0.7c, and thermal parton momentum distributions, one may get a "push" of a couple of GeV to be added to the transverse momentum of the string segment. This will be a crucial effect for intermediate pt jet hadrons.Scopus© Citations 1 - Some of the metrics are blocked by yourconsent settings
Publication Resonance production in high energy collisions from small to big systems(2018-02-02) ;Werner, K. ;Knospe, A. G. ;Markert, C. ;Guiot, B. ;Karpenko, Iu ;Pierog, T. ;Sophys, G. ;Stefaniak, M. ;Bleicher, M. ;Steinheimer, J. ;A. MischkeP. KuijerThe aim of this paper is to understand resonance production (and more generally particle production) for different collision systems, namely proton-proton (pp), proton-nucleus (pA), and nucleus-nucleus (AA) scattering at the LHC. We will investigate in particular particle yields and ratios versus multiplicity, using the same multiplicity definition for the three different systems, in order to analyse in a compact way the evolution of particle production with the system size and the origin of a very different system size dependence of the different particles.Scopus© Citations 12 - Some of the metrics are blocked by yourconsent settings
Publication System size dependence of particle production in EPOS(2018-09-18) ;Werner, K.; ;Karpenko, Iu ;Pierog, T. ;Sophys, G.Stefaniak, M.The aim of this paper is to understand particle production for different collision systems, namely proton-proton (pp), proton-nucleus (pA), and nucleus-nucleus (AA) scattering at the LHC. We will investigate in particular particle yields and ratios versus multiplicity, using the same multiplicity definition for the three different systems, in order to analyse in a compact way the evolution of particle production with the system size and the origin of a very different system size dependence of the different particles.Scopus© Citations 1
