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Study of Collective Phenomena in Heavy-Ion Collisions Using CMS Open Data

Allan E. F. G. Ferreira, Cesar A. Bernardes

Abstract

In this work, we present preliminary results from a measurement of the recently proposed observable, $v_0(p_T)$, in lead-lead (PbPb) collisions at $\sqrt{s_{NN}}=2.76 \text{ TeV}$, using public data from the CMS Open Data portal. This observable is directly sensitive to radial flow and characterizes the transverse momentum ($p_T$) dependence of radial flow fluctuations, serving as probe of collective phenomena in the quark-gluon plasma (QGP) formed in heavy-ion collisions. Consistently with the ATLAS results at $\sqrt{s_{NN}}=5.02 \text{ TeV}$, we observe the three key features of collective radial flow: long-range correlations in pseudorapidity ($η$), a centrality-independent shape as a function of $p_T$, and factorization in $p_T$. The results presented in this work are generally compatible, within uncertainties, with the ATLAS measurements at $\sqrt{s_{NN}}=5.02\text{ TeV}$ reported in Phys. Rev. Lett. 136, 032301 (2026).

Study of Collective Phenomena in Heavy-Ion Collisions Using CMS Open Data

Abstract

In this work, we present preliminary results from a measurement of the recently proposed observable, , in lead-lead (PbPb) collisions at , using public data from the CMS Open Data portal. This observable is directly sensitive to radial flow and characterizes the transverse momentum () dependence of radial flow fluctuations, serving as probe of collective phenomena in the quark-gluon plasma (QGP) formed in heavy-ion collisions. Consistently with the ATLAS results at , we observe the three key features of collective radial flow: long-range correlations in pseudorapidity (), a centrality-independent shape as a function of , and factorization in . The results presented in this work are generally compatible, within uncertainties, with the ATLAS measurements at reported in Phys. Rev. Lett. 136, 032301 (2026).
Paper Structure (4 sections, 12 equations, 5 figures)

This paper contains 4 sections, 12 equations, 5 figures.

Figures (5)

  • Figure 1: Scheme of the $p_T$ spectrum: the black curve represents the average spectrum over all events, while the blue and red curves represent events with a radial flow larger and smaller than the average, respectively. Events with a larger-than-average radial flow have a flatter spectrum, which is reflected in the covariance, that has a fixed zero-point at $p_T \approx \langle p_T \rangle$atlas-measurement.
  • Figure 2: $v_0$ dependence on centrality (a) and the normalized covariance $v_0(p_T)v_0$(b), both measured in different $p_T^{ref}$ ranges.
  • Figure 3: $v_0(p_T)$ observable in different $p_T^{ref}$ ranges and $\eta_{gap}=1$ in 50-60% centrality.
  • Figure 4: $v_0(p_T)$ in different $\eta_{gap}$ values and $p_T^{ref} \in [0.5,2] \text{ GeV}$ in 50-60% centrality.
  • Figure 5: $v_0(p_T)$ and $v_0(p_T)/v_0$ at default parameters in different centrality ranges.