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Light neutral-meson production in pp collisions at $\mathbf{\sqrt{s}}$ = 13 TeV

ALICE Collaboration

TL;DR

This study measures the production cross sections of $\pi^{0}$ and $\eta$ mesons in inelastic $pp$ collisions at $\sqrt{s}=13$ TeV with ALICE, at midrapidity, across a broad $p_{\rm T}$ range to test scaling laws and constrain fragmentation functions. By combining three photon-reconstruction methods (EMCal, PHOS, PCM) and invariant-mass techniques, the analysis provides detailed cross sections and multiplicity-dependent spectra, revealing a $m_{\rm T}$-scaling violation at low $p_{\rm T}$ and validating $x_{\rm T}$ scaling for $\pi^{0}$ with $n=5.01 \pm 0.05$. NLO pQCD calculations with CT18 PDFs and NNFF1.0/BDSS FFs describe the data best for $\pi^{0}$, while PYTHIA8 and EPOS LHC overpredict the yields and struggle with the $\eta$ spectrum. The multiplicity-dependent results show spectral shape hardening with increasing $\text{d}N_{\rm ch}/\text{d}\eta$ and a multiplicity-dependent $\eta/\pi^{0}$ ratio at low $p_{\rm T}$, providing stringent constraints for hadronization models and MC tuning, including feed-down effects from heavier states.

Abstract

The momentum-differential invariant cross sections of ${π^{0}}$ and $η$ mesons are reported for pp collisions at $\sqrt{s}$ = 13 TeV at midrapidity ($|y|<0.8$). The measurement is performed in a broad transverse-momentum range of $0.2<p_{\rm T}<200$ GeV/$c$ and $0.4 < p_{\rm T} < 60$ GeV/$c$ for the ${π^{0}}$ and $η$, respectively, extending the $p_{\rm T}$ coverage of previous measurements. Transverse-mass-scaling violation of up to 60% at low transverse momentum has been observed, agreeing with measurements at lower collision energies. Transverse Bjorken $x$ ($x_{\rm T}$) scaling of the ${π^{0}}$ cross sections at LHC energies is fulfilled with a power-law exponent of $n = 5.01 \pm 0.05$, consistent with values obtained for charged pions at similar collision energies. The data are compared to predictions from next-to-leading order perturbative QCD calculations, where the ${π^{0}}$ spectrum is best described using the CT18 parton distribution function and the NNFF1.0 or BDSS fragmentation function. Expectations from PYTHIA8 and EPOS LHC overestimate the spectrum for the ${π^{0}}$ and are not able to describe the shape and magnitude of the $η$ spectrum. The charged-particle multiplicity dependent ${π^{0}}$ and $η$ $p_{\rm T}$ spectra show the expected change of the spectral shape, characterized by a flatter slope with increasing multiplicity. This is demonstrated across a broad transverse-momentum range and up to events with a charged-particle multiplicity exceeding five times the mean value in minimum bias collisions. The $η/π^{0}$ ratio depends on the charged-particle multiplicity for $ p_{\rm T} < 4$ GeV/$c$. PYTHIA8 and EPOS LHC qualitatively explain this behavior with an increasing contribution from the feed-down of heavier particles to the ${π^{0}}$ spectrum.

Light neutral-meson production in pp collisions at $\mathbf{\sqrt{s}}$ = 13 TeV

TL;DR

This study measures the production cross sections of and mesons in inelastic collisions at TeV with ALICE, at midrapidity, across a broad range to test scaling laws and constrain fragmentation functions. By combining three photon-reconstruction methods (EMCal, PHOS, PCM) and invariant-mass techniques, the analysis provides detailed cross sections and multiplicity-dependent spectra, revealing a -scaling violation at low and validating scaling for with . NLO pQCD calculations with CT18 PDFs and NNFF1.0/BDSS FFs describe the data best for , while PYTHIA8 and EPOS LHC overpredict the yields and struggle with the spectrum. The multiplicity-dependent results show spectral shape hardening with increasing and a multiplicity-dependent ratio at low , providing stringent constraints for hadronization models and MC tuning, including feed-down effects from heavier states.

Abstract

The momentum-differential invariant cross sections of and mesons are reported for pp collisions at = 13 TeV at midrapidity (). The measurement is performed in a broad transverse-momentum range of GeV/ and GeV/ for the and , respectively, extending the coverage of previous measurements. Transverse-mass-scaling violation of up to 60% at low transverse momentum has been observed, agreeing with measurements at lower collision energies. Transverse Bjorken () scaling of the cross sections at LHC energies is fulfilled with a power-law exponent of , consistent with values obtained for charged pions at similar collision energies. The data are compared to predictions from next-to-leading order perturbative QCD calculations, where the spectrum is best described using the CT18 parton distribution function and the NNFF1.0 or BDSS fragmentation function. Expectations from PYTHIA8 and EPOS LHC overestimate the spectrum for the and are not able to describe the shape and magnitude of the spectrum. The charged-particle multiplicity dependent and spectra show the expected change of the spectral shape, characterized by a flatter slope with increasing multiplicity. This is demonstrated across a broad transverse-momentum range and up to events with a charged-particle multiplicity exceeding five times the mean value in minimum bias collisions. The ratio depends on the charged-particle multiplicity for GeV/. PYTHIA8 and EPOS LHC qualitatively explain this behavior with an increasing contribution from the feed-down of heavier particles to the spectrum.

Paper Structure

This paper contains 6 sections, 2 figures, 5 tables.

Figures (2)

  • Figure 1: Trigger rejection factors for the EMC-L1 $\gamma$ (low) (green), EMC-L1 $\gamma$ (high) (cyan) and the PHOS-PHI7 (red) trigger as a function of the cluster energy. The dip in the EMC-L1 $\gamma$ (high)/EMC-L1 $\gamma$ (low) ratio arises due to the trigger turn-on of the EMC-L1 $\gamma$ (low) trigger of about $4$ GeemV as explained in \ref{['sec:EventSelection']}.
  • Figure 2: Invariant mass distribution of $\gamma\gamma$ pairs around the ${\pi^{0}}$ (left) and $\eta$ (right) rest mass for the PCM and EMC reconstruction methods, respectively. The extracted meson peak is shown in red, with the parametrization in blue and its uncertainty represented by a blue band. The vertical dashed lines correspond to the limits of the signal integration window.