PRODUCTION OF K*(892) MESONS IN CU+AU AND U+U COLLISIONS

17 Oct 2020, 17:05
25m
Online

Online

Oral report Section 4. Relativistic nuclear physics, elementary particle physics and high-energy physics. Section 4. Relativistic nuclear physics, elementary particle physics and high-energy physics

Speaker

Vladislav Borisov (Peter the Great St.Petersburg Polytechnic University (SPbPU))

Description

One of the first proposed signatures of quark-gluon plasma (QGP) formation in heavy ion collisions was strangeness enhancement [1]. Due to its strange quark content, the $K^*$ meson is a good probe for the study of the QGP formed in heavy-ion collisions. $K^*$-meson production was previously measured by PHENIX [2] in symmetric Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 GeV [3]. To continue the study of the QGP properties, we have performed analyses of $K^*$-meson production in asymmetric Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV as well as collisions of highly deformed uranium nuclei at $\sqrt{s_{NN}}$ = 192 GeV. In this talk, we present invariant transverse momentum spectra and nuclear modification factors of $K^*$-mesons measured in Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV and U+U collisions at $\sqrt{s_{NN}}$ = 192 GeV. In central Cu+Au and U+U collisions in the intermediate transverse momentum range, $K^*$-meson yields are less suppressed than the yields of non-strange mesons such as $\pi^0$, $\eta$, and $\omega$, which might indicate that additional particle production mechanisms are involved in $K^*$-meson production. Production of $K^*$-mesons in Cu+Cu, Cu+Au, and U+U collisions scales with number of participants and seems to depend on nuclear overlap size, but not on its geometry [4]. Implications for hadronization and strangeness production will be discussed.

  1. Adcox, K. Formation of dense partonic matter in relativistic nucleus-nucleus collisions at RHIC: Experimental evaluation by the PHENIX Collaboration. Nuclear Physics A. 2005. Volume 757, Issue 1-2, Pages 184-28
  2. K. Adcox et al, PHENIX detector overview, Nucl. Instrum. Meth. A 499 (2003)
  3. A. Adare et al, Measurement of $K_S^0$ and $K^{*0}$ in p+p, d+Au, and Cu + Cu collisions at $\sqrt{s_{NN}}$ = 200 GeV, Phys. Rev. C 90, 054905 (2014)
  4. I. Mitrankov, Scaling properties of high-pT light hadrons from small to large systems by PHENIX. Proceedings of Science, 2018, Volume 345

Primary author

Vladislav Borisov (Peter the Great St.Petersburg Polytechnic University (SPbPU))

Co-authors

Dmitry Kotov (Peter the Great St.Petersburg Polytechnic University (SPbPU)) Yaroslav Berdnikov (Peter the Great St.Petersburg Polytechnic University (SPbPU)) Iurii Mitrankov (Peter the Great St.Petersburg Polytechnic University (SPbPU)) Aleksandr Berdnikov (Peter the Great St.Petersburg Polytechnic University (SPbPU))

Presentation materials