11-16 July 2022
Europe/Moscow timezone
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The role of parton distribution functions in the ϕ meson production in relativistic ion collisions

13 Jul 2022, 18:10
20m
НИИЯФ, ЮК, ауд. 3-13

НИИЯФ, ЮК, ауд. 3-13

Oral talk (15 min + 5 min questions) Intermediate and high energies, heavy ion collisions

Speaker

Mariia Mitrankova (Peter the Great St.Petersburg Polytechnic University (SPbPU))

Description

Lattice gauge QCD calculations predict phase transition from hadronic matter to deconfined state of quarks and gluons - quark-gluon plasma (QGP) - at a high temperature and energy density [1]. Minimal conditions of the QCD phase transition and QGP matter formation are studied in relativistic small-system collisions [2]. One of the ways to investigate QGP properties in experiment is to measure the peculiarities of particles production [2]. Due to its characteristics, the vector ϕ meson is considered as a good probe of the partonic matter formed in relativistic ion collisions [3].

The cross section of particle production in hard processes in the leading order QCD at the parton level is determined using nuclear parton distribution functions (nPDFs) [4-6]. These functions characterize the probability of a parton to have a certain fraction of the nucleon momentum inside the ion at any scale of the square of the momentum transfer in the interaction. The distributions are extracted from comprehensive global analysis of hard scattering data from variety of fix-target and collider experiments in framework of pQCD. The implementing of various sets of nPDF parameterizations [4-6] may help to interpret the experimental results on particle production.

This report presents the comparison of ϕ meson production in p+Al, p+Au, d+Au, and 3He+Au collisions at √sNN = 200 GeV at midrapidity (|η|<0.35), measured at PHENIX [1], to PYTHIA/Angantyr, PYTHIA+EPPS16, and PYTHIA+nCTEQ15 nPDFs calculations. Model calculations are consistent with experimental data within uncertainties. However, at intermediate transverse momentum range, PYTHIA/Angantyr, PYTHIA+EPPS16, and PYTHIA+nCTEQ15 calculations do not predict the ordering of ϕ meson production with the collision system size, observed in the experiment. Therefore, ϕ meson production in p/ d/ 3He+Au collisions at √sNN = 200 GeV might be driven by mechanisms additional to nPDF.

We acknowledge support from Russian Ministry of Education and Science, state assignment for fundamental research (code FSEG-2020-0024) in the ϕ meson production in 3He+Au collisions part of the analysis.

  1. K. Adcox et al. (PHENIX Collaboration), Nucl. Phys. A, 757, 184 (2005).
  2. M.M. Mitrankova et al. Phys. Scr. 96, 084010 (2021).
  3. C.P. Singh, Vivek Kumar Tiwari, K.K. Singh, Phys. Lett. B 393, 188 (1997).
  4. C. Bierlich, G. Gustafson, L. Lönnblad, H. Shah, JHEP 10, 134 (2018).
  5. K.J. Eskola, P. Paakkinen, H. Paukkunen, C.A. Salgado, Eur. Phys. J. C 77, 163 (2017).
  6. K. Kovark et al. Phys. Rev. D. 92, 8, 085037 (2016).
The speaker is a student or young scientist Yes
Section 3. Intermediate and high energies, heavy ion collisions

Primary author

Mariia Mitrankova (Peter the Great St.Petersburg Polytechnic University (SPbPU))

Co-authors

Mr Egor Bannikov (Peter the Great St.Petersburg Polytechnic University (SPbPU)) Dr Alexander Berdnikov (Peter the Great St.Petersburg Polytechnic University (SPbPU)) Prof. Yaroslav Berdnikov (Peter the Great St.Petersburg Polytechnic University (SPbPU)) Dr Dmitry Kotov (Peter the Great St.Petersburg Polytechnic University (SPbPU)) Mr Iurii Mitrankov (Peter the Great St.Petersburg Polytechnic University (SPbPU)) Ms Daria Larionova (Peter the Great St.Petersburg Polytechnic University (SPbPU))

Presentation Materials