{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.115569.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1986611"}},{"@id":"https://doi.org/10.1016/j.physletb.2022.136941","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2022","description":"In high-energy heavy-ion collisions, partonic collectivity is evidenced by the constituent quark number scaling of elliptic flow anisotropy for identified hadrons. A breaking of this scaling and dominance of baryonic interactions is found for identified hadron collective flow measurements in $\\sqrt{s_{\\rm NN}}$ = 3 GeV Au+Au collisions. In this paper, we report measurements of the first- and second-order azimuthal anisotropic parameters, $v_1$ and $v_2$, of light nuclei ($d$, $t$, $^{3}$He, $^{4}$He) produced in $\\sqrt{s_{\\rm NN}}$ = 3 GeV Au+Au collisions at the STAR experiment. An atomic mass number scaling is found in the measured $v_1$ slopes of light nuclei at mid-rapidity. For the measured $v_2$ magnitude, a strong rapidity dependence is observed. Unlike $v_2$ at higher collision energies, the $v_2$ values at mid-rapidity for all light nuclei are negative and no scaling is observed with the atomic mass number. Calculations by the Jet AA Microscopic Transport Model (JAM), with baryonic mean-field plus nucleon coalescence, are in good agreement with our observations, implying baryonic interactions dominate the collective dynamics in 3 GeV Au+Au collisions at RHIC.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t1","@type":"Dataset","description":"The rapidity and $p_{T}$ dependencies of $v_{1}$ for $p$ in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 3a proton"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t2","@type":"Dataset","description":"The rapidity and $p_{T}$ dependencies of $v_{1}$ for $d$ in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 3a deuteron"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t3","@type":"Dataset","description":"The $p_{T}$ dependencies of $v_{1}$ within $-0.1&lt;y&lt;0$ for $t$ in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 3a triton (-0.1 < y < 0)"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t4","@type":"Dataset","description":"The $p_{T}$ dependencies of $v_{1}$ within $-0.4&lt;y&lt;-0.1$ for $t$ in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 3a triton (-0.4 < y < -0.1)"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t5","@type":"Dataset","description":"The rapidity and $p_{T}$ dependencies of $v_{1}$ for $^{3}$He in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 3a $^{3}$He"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t6","@type":"Dataset","description":"The $p_{T}$ dependencies of $v_{1}$ within $-0.1&lt;y&lt;0$ for $^4$He in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 3a $^{4}$He (-0.1 < y < 0)"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t7","@type":"Dataset","description":"The $p_{T}$ dependencies of $v_{1}$ within $-0.4&lt;y&lt;-0.1$ for $^{4}$He in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 3a $^{4}$He (-0.4 < y < -0.1)"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t8","@type":"Dataset","description":"The rapidity and $p_{T}$ dependencies of $v_{2}$ for $p$ in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 4(a-d) proton"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t9","@type":"Dataset","description":"The rapidity and $p_{T}$ dependencies of $v_{2}$ for $d$ in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 4(a-d) deuteron"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t10","@type":"Dataset","description":"The $p_{T}$ dependencies of $v_{2}$ within $-0.1&lt;y&lt;0$ for $t$ in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 4(a-d) triton (-0.1 < y < 0)"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t11","@type":"Dataset","description":"The $p_{T}$ dependencies of $v_{2}$ within $-0.4&lt;y&lt;-0.1$ for $t$ in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 4(a-d) triton (-0.4 < y < -0.3)"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t12","@type":"Dataset","description":"The rapidity and $p_{T}$ dependencies of $v_{2}$ for $^{3}$He in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 4(a-d) $^{3}$He"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t13","@type":"Dataset","description":"The $p_{T}$ dependencies of $v_{2}$ within $-0.1&lt;y&lt;0$ for $^4$He in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 4(a-d) $^{4}$He (-0.1 < y <0)"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t14","@type":"Dataset","description":"The $p_{T}$ dependencies of $v_{2}$ within $-0.4&lt;y&lt;-0.1$ for $^{4}$He in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 4(a-d) $^{4}$He (-0.4 < y < -0.1)"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t15","@type":"Dataset","description":"The rapidity dependencies of $v_{1}$ for $p$, $d$, and $^{3}$He in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 5a proton, deuteron, and $^{3}$He"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t16","@type":"Dataset","description":"The rapidity dependencies of $v_{1}$ for $t$ and $^{4}$He in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 5a triton and $^{4}$He"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t17","@type":"Dataset","description":"The rapidity dependencies of $v_{1}$ from JAM plus coalescence calculations in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 5a model"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t18","@type":"Dataset","description":"The rapidity dependencies of $v_{2}$ for $p$, $d$, and $^{3}$He in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 5b proton, deuteron, and $^{3}$He"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t19","@type":"Dataset","description":"The rapidity dependencies of $v_{2}$ for $t$ and $^{4}$He in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 5b triton and $^{4}$He"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t20","@type":"Dataset","description":"The rapidity dependencies of $v_{2}$ from JAM plus coalescence calculations in 10-40% mid-central Au+Au collisions at 3 GeV.","name":"Figure 5b model"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t21","@type":"Dataset","description":"Light nucleus scaled $v_{1}$ slopes as a function os collision energy in 10-40 mid-cantral Au+Au collisions.","name":"Figure 6 data"},{"@id":"https://doi.org/10.17182/hepdata.115569.v1/t22","@type":"Dataset","description":"Light nucleus scaled $v_{1}$ slopes from JAM plus coalescence in 10-40 mid-cantral Au+Au collisions at 3 GeV.","name":"Figure 6 model"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1986611?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/115569"}],"inLanguage":"en","name":"Light Nuclei Collectivity from $\\sqrt{s_{\\rm NN}}$ = 3 GeV Au+Au Collisions at RHIC","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1986611?version=1","version":1}