{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.153244.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2692207"}},{"@id":"https://doi.org/10.1007/JHEP05(2024)317","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2024","description":"The production yields of the $\\Sigma(1385)^{\\pm}$ and $\\Xi(1530)^{0}$ resonances are measured in pp collisions at $\\sqrt{\\it{s}}=13$~Te\\kern-.1emV with ALICE. The measurements are performed as a function of the charged particle multiplicity $\\langle\\mathrm{d}N_\\mathrm{ch}/\\mathrm{d}\\eta\\rangle$, which is related to the energy density produced in the collision. The results include transverse momentum ($p_\\mathrm{T}$) distributions, $p_\\mathrm{T}$-integrated yields, mean transverse momenta of $\\Sigma(1385)^{\\pm}$ and $\\Xi(1530)^{0}$, as well as ratios of the $p_\\mathrm{T}$-integrated resonance yields relative to yields of other hadron species. The $\\Sigma(1385)^{\\pm}/\\pi^{\\pm}$ and $\\Xi(1530)^{0}/\\pi^{\\pm}$ yield ratios are consistent with the trend of the enhancement of strangeness production from low to high multiplicity pp collisions, which was previously observed for strange and multi-strange baryons. The yield ratio between the measured resonances and the long-lived baryons with the same strangeness content exhibits a hint of a mild increasing trend at low multiplicity, despite too large uncertainties to exclude the flat behaviour. The results are compared to predictions from models such as EPOS-LHC and $\\rm{PYTHIA\\,\\,8}$ with Rope shoving. The latter provides the best description of the multiplicity dependence of the $\\Sigma(1385)^{\\pm}$ and $\\Xi(1530)^{0}$ production in pp collisions at $\\sqrt{\\it{s}}=13$~Te\\kern-.1emV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.153244.v1/t1","@type":"Dataset","description":"Sigma(1385)+ pT spectrum in I+II+III V0M mult class","name":"sigma1385plus pT spectrum in I+II+III V0M mult class"},{"@id":"https://doi.org/10.17182/hepdata.153244.v1/t2","@type":"Dataset","description":"Sigma(1385)+ pT spectrum in IV+V+VI V0M mult class","name":"sigma1385plus pT spectrum in IV+V+VI V0M mult class"},{"@id":"https://doi.org/10.17182/hepdata.153244.v1/t3","@type":"Dataset","description":"Sigma(1385)+ pT spectrum in VII+VIII V0M mult class","name":"sigma1385plus pT spectrum in VII+VIII V0M mult class"},{"@id":"https://doi.org/10.17182/hepdata.153244.v1/t4","@type":"Dataset","description":"Sigma(1385)+ pT spectrum in IX V0M mult class","name":"sigma1385plus pT spectrum in IX V0M mult 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