{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.101356.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1843941"}},{"@id":"https://doi.org/10.1103/PhysRevC.104.024902","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2021","description":"We report a systematic measurement of cumulants, $C_{n}$, for net-proton, proton and antiproton, and correlation functions, $\\kappa_n$, for proton and antiproton multiplicity distributions up to the fourth order in Au+Au collisions at $\\sqrt{s_{\\mathrm {NN}}}$ = 7.7, 11.5, 14.5, 19.6, 27, 39, 54.4, 62.4 and 200 GeV. The $C_{n}$ and $\\kappa_n$ are presented as a function of collision energy, centrality and kinematic acceptance in rapidity, $y$, and transverse momentum, $p_{T}$. The data were taken during the first phase of the Beam Energy Scan (BES) program (2010 -- 2017) at the Relativistic Heavy Ion Collider (RHIC) facility. The measurements are carried out at midrapidity ($|y| <$ 0.5) and transverse momentum 0.4 $<$ $p_{\\rm T}$ $<$ 2.0 GeV/$c$, using the STAR detector at RHIC. We observe a non-monotonic energy dependence ({\\snn} = 7.7 -- 62.4 GeV) of the net-proton $C_{4}$/$C_{2}$ with the significance of 3.1$\\sigma$ for the 0-5\\% central Au+Au collisions. This is consistent with the expectations of critical fluctuations in a QCD-inspired model. Thermal and transport model calculations show a monotonic variation with \\snn. For the multiparticle correlation functions, we observe significant negative values for a two-particle correlation function, $\\kappa_2$, of protons and antiprotons, which are mainly due to the effects of baryon number conservation. Furthermore, it is found that the four-particle correlation function, $\\kappa_4$, of protons plays a role in determining the energy dependence of proton $C_4/C_1$ below 19.6 GeV, which cannot be solely understood by the negative values of $\\kappa_2$ for protons.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.101356.v1/t1","@type":"Dataset","description":"Reference charged particle multiplicity distributions using only pions and kaons ...","name":"Reference Charged Particle Multiplicity 7.7 GeV"},{"@id":"https://doi.org/10.17182/hepdata.101356.v1/t2","@type":"Dataset","description":"Reference charged particle multiplicity distributions using only pions and kaons ...","name":"Reference Charged Particle Multiplicity 11.5 GeV"},{"@id":"https://doi.org/10.17182/hepdata.101356.v1/t3","@type":"Dataset","description":"Reference charged particle multiplicity distributions using only pions and kaons ...","name":"Reference Charged Particle Multiplicity 14.5 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