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Extraction of Effective Parameters from Transverse Momentum Spectra of Heavy Quarkonia in Proton-Proton Collisions at the LHC

Peng-Cheng Zhang, Hailong Zhu, Fu-Hu Liu, Khusniddin K. Olimov

TL;DR

This work addresses whether a temperature concept is applicable in small collision systems by extracting two effective parameters, the Schwinger string tension $\kappa$ and the initial effective temperature $T$, from heavy quarkonium $p_T$ spectra in p+p collisions at the LHC. It introduces a multi-component framework combining Schwinger mechanism and Bose-Einstein statistics to fit the spectra of $J/\psi$ and $\Upsilon(nS)$ measured by LHCb at $\sqrt{s}=13$ and 8 TeV, yielding a consistent $\kappa$–$T$ correlation and a derived $R_{\min}$ that characterizes the initial color field overlap. The extracted $\kappa$ values are large (tens to hundreds of GeV/fm) and $T$ values (roughly 0.7–2.1 GeV) exceed typical QGP freeze-out scales, consistent with initial-state dynamics and possible collectivity in small systems. The positive $\kappa$–$T$ correlation and the very small $R_{\min}$ imply intense initial energy density and potential early-time collective behavior, offering a microscopic lens for comparing small- and large-system dynamics and guiding future investigations across collision systems and energies.

Abstract

The effective string tension ($κ$) in the Schwinger mechanism and the effective temperature ($T$) in Bose-Einstein statistics are extracted from the transverse momentum ($p_T$) spectra of heavy quarkonia produced in proton-proton (p+p) collisions at the Large Hadron Collider (LHC). Here, $T$ derived from the heavy quarkonium $p_T$ spectra also serves as the initial effective temperature (effective temperature at the initial stage) of small collision systems. This is because, despite the absence of quark-gluon plasma (QGP) formation during the collisions, which leaves $T$ largely unaffected by QGP-related effects, the initial geometric asymmetry and local partonic thermalization still induce radial and transverse flows, thereby contributing to an increase in $T$. The effective parameters ($κ$ and $T$) are obtained by fitting the experimental $p_T$ spectra of $J/ψ$ and $Υ(nS)$ ($n=1$, 2, and 3) within various rapidity intervals, produced in p+p collisions at center-of-mass energies of $\sqrt{s}=13$ and 8 TeV, as measured by the LHCb Collaboration. It is found that the multi-component distribution structured within the framework of the Schwinger mechanism or Bose-Einstein statistics can effectively describe the heavy quarkonium $p_T$ spectra in small collision systems. With decreasing rapidity in the forward region, both $κ$ and $T$ increase, indicating a directly proportional relationship between them. Based on $κ$, the average minimum strong force radius of participant quarks is determined.

Extraction of Effective Parameters from Transverse Momentum Spectra of Heavy Quarkonia in Proton-Proton Collisions at the LHC

TL;DR

This work addresses whether a temperature concept is applicable in small collision systems by extracting two effective parameters, the Schwinger string tension and the initial effective temperature , from heavy quarkonium spectra in p+p collisions at the LHC. It introduces a multi-component framework combining Schwinger mechanism and Bose-Einstein statistics to fit the spectra of and measured by LHCb at and 8 TeV, yielding a consistent correlation and a derived that characterizes the initial color field overlap. The extracted values are large (tens to hundreds of GeV/fm) and values (roughly 0.7–2.1 GeV) exceed typical QGP freeze-out scales, consistent with initial-state dynamics and possible collectivity in small systems. The positive correlation and the very small imply intense initial energy density and potential early-time collective behavior, offering a microscopic lens for comparing small- and large-system dynamics and guiding future investigations across collision systems and energies.

Abstract

The effective string tension () in the Schwinger mechanism and the effective temperature () in Bose-Einstein statistics are extracted from the transverse momentum () spectra of heavy quarkonia produced in proton-proton (p+p) collisions at the Large Hadron Collider (LHC). Here, derived from the heavy quarkonium spectra also serves as the initial effective temperature (effective temperature at the initial stage) of small collision systems. This is because, despite the absence of quark-gluon plasma (QGP) formation during the collisions, which leaves largely unaffected by QGP-related effects, the initial geometric asymmetry and local partonic thermalization still induce radial and transverse flows, thereby contributing to an increase in . The effective parameters ( and ) are obtained by fitting the experimental spectra of and (, 2, and 3) within various rapidity intervals, produced in p+p collisions at center-of-mass energies of and 8 TeV, as measured by the LHCb Collaboration. It is found that the multi-component distribution structured within the framework of the Schwinger mechanism or Bose-Einstein statistics can effectively describe the heavy quarkonium spectra in small collision systems. With decreasing rapidity in the forward region, both and increase, indicating a directly proportional relationship between them. Based on , the average minimum strong force radius of participant quarks is determined.

Paper Structure

This paper contains 7 sections, 6 equations, 6 figures.

Figures (6)

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