{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.136560.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2054927"}},{"@id":"https://doi.org/10.1103/PhysRevC.107.024907","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"PHENIX Collaboration"},"creator":{"@type":"Organization","name":"PHENIX Collaboration"},"datePublished":"2023","description":"Recently, the PHENIX Collaboration has published second- and third-harmonic Fourier coefficients $v_2$ and $v_3$ for midrapidity ($|\\eta|<0.35$) charged hadrons in 0\\%--5\\% central $p$$+$Au, $d$$+$Au, and $^3$He$+$Au collisions at $\\sqrt{s_{_{NN}}}=200$ GeV utilizing three sets of two-particle correlations for two detector combinations with different pseudorapidity acceptance [Phys. Rev. C {\\bf 105}, 024901 (2022)]. This paper extends these measurements of $v_2$ to all centralities in $p$$+$Au, $d$$+$Au, and $^3$He$+$Au collisions, as well as $p$$+$$p$ collisions, as a function of transverse momentum ($p_T$) and event multiplicity. The kinematic dependence of $v_2$ is quantified as the ratio $R$ of $v_2$ between the two detector combinations as a function of event multiplicity for $0.5$$<$$p_T$$<$$1$ and $2$$<$$p_T$$<$$2.5$ GeV/$c$. A multiphase-transport (AMPT) model can reproduce the observed $v_2$ in most-central to midcentral $d$$+$Au and $^3$He$+$Au collisions.  However, the AMPT model systematically overestimates the measurements in $p$$+$$p$, $p$$+$Au, and peripheral $d$$+$Au and $^3$He$+$Au collisions, indicating a higher nonflow contribution in AMPT than in the experimental data.  The AMPT model fails to describe the observed $R$ for $0.5$$<$$p_T$$<$$1$ GeV/$c$, but there is qualitative agreement with the measurements for $2$$<$$p_T$$<$$2.5$ GeV/$c$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t1","@type":"Dataset","description":"Azimuthal anisotropy $v_2\\{BB\\}$ as a function of transverse momentum $p_T$ in $p$+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 4.0"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t2","@type":"Dataset","description":"Azimuthal anisotropy $v_2\\{BF\\}$ as a function of transverse momentum $p_T$ in $p$+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 4.1"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t3","@type":"Dataset","description":"Azimuthal anisotropy $v_2\\{BB\\}$ as a function of transverse momentum $p_T$ in $d$+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 5.0"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t4","@type":"Dataset","description":"Azimuthal anisotropy $v_2\\{BF\\}$ as a function of transverse momentum $p_T$ in $d$+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 5.1"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t5","@type":"Dataset","description":"Azimuthal anisotropy $v_2\\{BB\\}$ as a function of transverse momentum $p_T$ in $^3$He+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 6.0"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t6","@type":"Dataset","description":"Azimuthal anisotropy $v_2\\{BF\\}$ as a function of transverse momentum $p_T$ in $^3$He+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 6.1"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t7","@type":"Dataset","description":"Azimuthal anisotropy $v_2$ as a function of transverse momentum $p_T$ in $p$+$p$ collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 7.0"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t8","@type":"Dataset","description":"Azimuthal anisotropy $v_2$ as a function of centrality in $p$+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 8.0"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t9","@type":"Dataset","description":"Azimuthal anisotropy $v_2$ as a function of centrality in $d$+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 8.1"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t10","@type":"Dataset","description":"Azimuthal anisotropy $v_2$ as a function of centrality in $^3$He+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 8.2"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t11","@type":"Dataset","description":"Azimuthal anisotropy $v_2$ as a function of charged particle multiplicity $dN_{ch}/d\\eta$ in $p$+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 9.0"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t12","@type":"Dataset","description":"Azimuthal anisotropy $v_2$ as a function of charged particle multiplicity $dN_{ch}/d\\eta$ in $d$+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 9.1"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t13","@type":"Dataset","description":"Azimuthal anisotropy $v_2$ as a function of charged particle multiplicity $dN_{ch}/d\\eta$ in $^3$He+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 9.2"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t14","@type":"Dataset","description":"Azimuthal anisotropy $v_2$ as a function of charged particle multiplicity $dN_{ch}/d\\eta$ in $p$+$p$ collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 9.3"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t15","@type":"Dataset","description":"Azimuthal anisotropy ratio $R=v_2\\{BF\\}/v_2\\{BB\\}$ as a function of charged particle multiplicity $dN_{ch}/d\\eta$ in $p$+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 10.0"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t16","@type":"Dataset","description":"Azimuthal anisotropy ratio $R=v_2\\{BF\\}/v_2\\{BB\\}$ as a function of charged particle multiplicity $dN_{ch}/d\\eta$ in $d$+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 10.1"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t17","@type":"Dataset","description":"Azimuthal anisotropy ratio $R=v_2\\{BF\\}/v_2\\{BB\\}$ as a function of charged particle multiplicity $dN_{ch}/d\\eta$ in $^3$He+Au collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 10.2"},{"@id":"https://doi.org/10.17182/hepdata.136560.v1/t18","@type":"Dataset","description":"Azimuthal anisotropy ratio $R=v_2\\{BF\\}/v_2\\{BB\\}$ as a function of charged particle multiplicity $dN_{ch}/d\\eta$ in $p$+$p$ collisions at $\\sqrt{s_{NN}} =$ 200 GeV.","name":"Figure 10.3"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2054927?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/136560"}],"inLanguage":"en","name":"Measurements of second-harmonic Fourier coefficients from azimuthal anisotropies in $p+p, p$+Au $d$+Au, and $^3$He + Au collisions at $\\sqrt{s_{_{NN}}}=200$ GeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2054927?version=1","version":1}