Observation of abnormal suppression of $\mathrm{f}_{0}$(980) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV

The ALICE collaboration
Phys.Lett.B 853 (2024) 138665, 2024.

Abstract (data abstract)
The dependence of f$_{0}$(980) production on the final-state charged-particle multiplicity in p-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is reported. The production of f$_{0}$(980) is measured with the ALICE detector via the f$_{0}$(980) $\rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $-0.5 < \mathrm{y} < 0$. Particle yield ratios of f$_{0}$(980) to $\pi$ and K$^{*}$(892)$^{0}$ are found to be decreasing with increasing charged-particle multiplicity. The magnitude of the suppression of the f$_{0}$(980)/$\pi$ and f$_{0}$(980)/K$^{*}$(892)$^{0}$ yield ratios is found to be dependent on the transverse momentum $p_\mathrm{T}$, suggesting different mechanisms responsible for the measured effects. Furthermore, the nuclear modification factor $Q_\mathrm{pPb}$ of f$_{0}$(980) is measured in various multiplicity ranges. The $Q_\mathrm{pPb}$ shows a strong suppression of the f$_{0}$(980) production in the $p_\mathrm{T}$ region up to about 4 GeV/$c$ The results on the particle yield ratios and $Q_\mathrm{pPb}$ for f$_{0}$(980) may help to understand the late hadronic phase in p-Pb collisions and the nature of the internal structure of f$_{0}$(980) particle

  • Table 1

    Data from Figures 2

    10.17182/hepdata.151390.v1/t1

    Transverse momentum spectra in different multiplicity classes. Each spectrum is corrected for the branching ratio of (46 $\pm$ 6)% based...

  • Table 2

    Data from Figures 2

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    The ratio of transverse momentum spectrum to the NSD spectrum

  • Table 3

    Data from Figures 3

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    The double ratio of particle yield of f0((980) to charged pions

  • Table 4

    Data from Figures 3

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    The double ratio of particle yield of f0((980) to K*(892)0

  • Table 5

    Data from Figures 4

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    Transverse-momentum-differential particle yield ratio of f$_{0}$(980) to charged pions and its double ratio

  • Table 6

    Data from Figures 5

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    Transverse-momentum-differential particle yield ratio of f$_{0}$(980) to K$^{*}(892)$^{0}$ and its double ratio

  • Table 7

    Data from Figures 6

    10.17182/hepdata.151390.v1/t7

    Nuclear modification factor of f0(980) in p-Pb collisions at 5.02 TeV

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