{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.160597.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2848478"}},{"@id":"https://doi.org/10.1007/JHEP08(2025)035","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2025","description":"The momentum-differential invariant cross sections of $\\pi^{0}$ and $\\eta$ 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 $\\pi^{0}$ and $\\eta$, respectively, extending the $\\eta$ 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 $x$ ($\\eta$) scaling of the $\\pi^{0}$ 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 is compared to predictions from next-to-leading order perturbative QCD calculations, where the $\\pi^{0}$ 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 $\\pi^{0}$ and are not able to describe the shape and magnitude of the $\\eta$ spectrum. The charged-particle multiplicity dependent $\\pi^{0}$ and $\\eta$ $p_{\\rm T}$ spectra show the expected hardening 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 absolute magnitude of the $\\eta/\\pi^{0}$ ratio shows a dependence on the charged-particle multiplicity for $p_{\\rm T}$ $<$ 4 GeV/$c$, qualitatively described by PYTHIA8 and EPOS LHC due to a rising contribution from feed-down of heavier particles to the $\\pi^{0}$ spectrum.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.160597.v1/t1","@type":"Dataset","description":"Invariant differential cross section of the $\\pi^{0}$ versus transverse momentum for pp collisions at $\\sqrt{s}$ = 13 TeV.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.160597.v1/t2","@type":"Dataset","description":"Invariant differential cross section of the $\\eta$ meson versus transverse momentum for pp collisions at $\\sqrt{s}$ = 13 TeV.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.160597.v1/t3","@type":"Dataset","description":"The $\\eta/\\pi^{0}$ ratio as a function of $p_{\\rm T}$ for pp collisions at $\\sqrt{s}$ = 13 TeV.","name":"Table 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collisions at $\\sqrt{s}$ = 8 TeV, with $n = 5.01$.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.160597.v1/t9","@type":"Dataset","description":"$x_{\\rm T}$ scaled $\\pi^{0}$ spectrum for pp collisions at $\\sqrt{s}$ = 13 TeV, with $n = 5.01$.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.160597.v1/t10","@type":"Dataset","description":"$x_{\\rm T}$ scaled $\\eta$ spectrum for pp collisions at $\\sqrt{s}$ = 2.76 TeV, with $n = 4.91$.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.160597.v1/t11","@type":"Dataset","description":"$x_{\\rm T}$ scaled $\\eta$ spectrum for pp collisions at $\\sqrt{s}$ = 7 TeV, with $n = 4.91$.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.160597.v1/t12","@type":"Dataset","description":"$x_{\\rm T}$ scaled $\\eta$ spectrum for pp collisions at $\\sqrt{s}$ = 8 TeV, with $n = 4.91$.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.160597.v1/t13","@type":"Dataset","description":"$x_{\\rm T}$ 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