{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.89445.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/647076"}},{"@id":"https://doi.org/10.1103/PhysRevLett.94.162301","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"BRAHMS Collaboration"},"creator":{"@type":"Organization","name":"BRAHMS Collaboration"},"datePublished":"2019","description":"BNL-RHIC-BRAHMS. We have measured rapidity densities dN/dy of pions and kaons over a broad rapidity range (-0.1 < y < 3.5) for central Au+Au collisions at sqrt(snn) = 200 GeV. These data have significant implications for the chemistry and dynamics of the dense system that is initially created in the collisions. The full phase-space yields are 1660 +/- 15 +/- 133 (pi+), 1683 +/- 16 +/- 135 (pi-), 286 +/- 5 +/- 23 (K+) and 242 +/- 4 +/- 19 (K-). The systematics of the strange to non--strange meson ratios are found to track the variation of the baryo-chemical potential with rapidity and energy. Landau--Carruthers hydrodynamic is found to describe the bulk transport of the pions in the longitudinal direction.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.89445.v1/t1","@type":"Dataset","description":"$\\frac{1}{2\\pi p_{\\mathrm{T}}}\\frac{\\mathrm{d}^2N}{\\mathrm{d}p_{\\mathrm{T}}\\mathrm{d}y}$ versus $p_{\\mathrm{T}}$ for $\\mathrm{\\pi}^{+}$ in $\\mathrm{Au}-\\mathrm{Au}$ at $\\sqrt{s_{\\mathrm{NN}}}=200\\,\\mathrm{Ge\\!V}$ near $y=-0.1-0.0$ for $0-5$% central","name":"Table 1A"},{"@id":"https://doi.org/10.17182/hepdata.89445.v1/t2","@type":"Dataset","description":"$\\frac{1}{2\\pi p_{\\mathrm{T}}}\\frac{\\mathrm{d}^2N}{\\mathrm{d}p_{\\mathrm{T}}\\mathrm{d}y}$ versus $p_{\\mathrm{T}}$ for $\\mathrm{\\pi}^{+}$ in $\\mathrm{Au}-\\mathrm{Au}$ at $\\sqrt{s_{\\mathrm{NN}}}=200\\,\\mathrm{Ge\\!V}$ near $y=0.0-0.1$ for $0-5$% central","name":"Table 1B"},{"@id":"https://doi.org/10.17182/hepdata.89445.v1/t3","@type":"Dataset","description":"$\\frac{1}{2\\pi 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$\\mathrm{Au}-\\mathrm{Au}$ at $\\sqrt{s_{\\mathrm{NN}}}=200\\,\\mathrm{Ge\\!V}$ near $y=3.2-3.4$ for $0-5$% central","name":"Table 1x"},{"@id":"https://doi.org/10.17182/hepdata.89445.v1/t53","@type":"Dataset","description":"$\\frac{\\mathrm{d}N}{\\mathrm{d}y}$ versus $y$ for $\\mathrm{\\pi}^{+}$ in $\\mathrm{Au}-\\mathrm{Au}$ at $\\sqrt{s_{\\mathrm{NN}}}=200\\,\\mathrm{Ge\\!V}$ for $0-5$% central","name":"Table 2A"},{"@id":"https://doi.org/10.17182/hepdata.89445.v1/t54","@type":"Dataset","description":"$\\frac{\\mathrm{d}N}{\\mathrm{d}y}$ versus $y$ for $\\mathrm{\\pi}^{-}$ in $\\mathrm{Au}-\\mathrm{Au}$ at $\\sqrt{s_{\\mathrm{NN}}}=200\\,\\mathrm{Ge\\!V}$ for $0-5$% central","name":"Table 2B"},{"@id":"https://doi.org/10.17182/hepdata.89445.v1/t55","@type":"Dataset","description":"$\\frac{\\mathrm{d}N}{\\mathrm{d}y}$ versus $y$ for $\\mathrm{K}^{+}$ in $\\mathrm{Au}-\\mathrm{Au}$ at $\\sqrt{s_{\\mathrm{NN}}}=200\\,\\mathrm{Ge\\!V}$ for $0-5$% central","name":"Table 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