{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.152804.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2132332"}},{"@id":"https://doi.org/10.1140/epja/s10050-023-00936-6","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"HADES Collaboration"},"creator":{"@type":"Organization","name":"HADES Collaboration"},"datePublished":"2024","description":"High precision measurements of flow coefficients $v_{n}$ ($n = 1 - 4$) for protons, deuterons and tritons relative to the first-order spectator plane have been performed in Au+Au collisions at $\\sqrt{s_{NN}} = 2.4$ GeV with the High-Acceptance Di-Electron Spectrometer (HADES) at the SIS18/GSI. Flow coefficients are studied as a function of transverse momentum $p_{t}$ and rapidity $y_{cm}$ over a large region of phase space and for several classes of collision centrality. A clear mass hierarchy is found for the slope of $v_{1}$, $d v_{1}/d y^{\\prime}|_{y^{\\prime} = 0}$ where $y^{\\prime}$ is the scaled rapidity, and for $v_{2}$ at mid-rapidity. Scaling with the number of nucleons is observed for the $p_{t}$ dependence of $v_{2}$ and $v_{4}$ at mid-rapidity, which is indicative for nuclear coalescence as the main process responsible for light nuclei formation. $v_{2}$ is found to scale with the initial eccentricity $\\langle \\epsilon_{2} \\rangle$, while $v_{4}$ scales with $\\langle \\epsilon_{2} \\rangle^{2}$ and $\\langle \\epsilon_{4} \\rangle$. The multi-differential high-precision data on $v_{1}$, $v_{2}$, $v_{3}$, and $v_{4}$ provides important constraints on the equation-of-state of compressed baryonic matter.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.152804.v1/t1","@type":"Dataset","description":"The resolution $\\Re_{n}$ of the first-order spectator event plane for flow coefficients of different orders $n$ as a function of...","name":"Figure 5 Event Plane Resolution 10pct"},{"@id":"https://doi.org/10.17182/hepdata.152804.v1/t2","@type":"Dataset","description":"The resolution $\\Re_{n}$ of the first-order spectator event plane for flow coefficients of different orders $n$ as a function of...","name":"Figure 5 Event Plane Resolution 5pct"},{"@id":"https://doi.org/10.17182/hepdata.152804.v1/t3","@type":"Dataset","description":"The flow coefficients $v_{1}$, $v_{2}$, $v_{3}$, and $v_{4}$ (from top to bottom panels) of protons, deuterons and tritons (from left...","name":"Figure 8 v1 ycm 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Listed are...","name":"Table 4 Eccentricities"},{"@id":"https://doi.org/10.17182/hepdata.152804.v1/t33","@type":"Dataset","description":"Scaled elliptic flow of protons, deuterons and tritons in two transverse momentum intervals at mid-rapidity in Au+Au collisions at $\\sqrt{s_{NN}}...","name":"Figure 15 v2eps2 Centrality"},{"@id":"https://doi.org/10.17182/hepdata.152804.v1/t34","@type":"Dataset","description":"Same as in Figure 15, but for the scaled quadrangular flow. The values are divided by the square of second...","name":"Figure 16 v4eps22 Centrality"},{"@id":"https://doi.org/10.17182/hepdata.152804.v1/t35","@type":"Dataset","description":"Same as in Figure 15, but for the scaled quadrangular flow. 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