Advances in High Energy Physics / 2015 / Article / Tab 2 / Research Article
On Pseudorapidity Distribution and Speed of Sound in High Energy Heavy Ion Collisions Based on a New Revised Landau Hydrodynamic Model Table 2 This table is like Table
1 but is showing the results for the curves in Figures
5 –
7 which show Cu-Cu collisions for different energies and centralities.
Figure Bin (%) 22.4 GeV Figure 5 (a) 0–3 −1.20 ± 0.20 0.03 ± 0.02 1.60 ± 0.08 0.238 0.123 ± 0.026 0.342 ± 0.027 Figure 5 (b) 3–6 −1.10 ± 0.19 0.01 ± 0.01 1.70 ± 0.08 0.115 0.123 ± 0.026 0.375 ± 0.027 Figure 5 (c) 6–10 −1.10 ± 0.17 0.01 ± 0.01 1.78 ± 0.10 0.130 0.123 ± 0.026 0.402 ± 0.033 Figure 5 (d) 10–15 −1.12 ± 0.20 0.01 ± 0.01 1.82 ± 0.11 1.264 0.123 ± 0.026 0.415 ± 0.035 Figure 5 (e) 15–20 −1.14 ± 0.23 0.01 ± 0.01 1.85 ± 0.06 2.796 0.123 ± 0.026 0.424 ± 0.019 Figure 5 (f) 20–25 −1.10 ± 0.21 0.01 ± 0.01 1.94 ± 0.06 3.001 0.123 ± 0.026 0.453 ± 0.019 Figure 5 (g) 25–30 −1.10 ± 0.20 0.01 ± 0.01 1.95 ± 0.07 4.056 0.123 ± 0.026 0.456 ± 0.022 Figure 5 (h) 30–35 −1.04 ± 0.20 0.01 ± 0.01 1.96 ± 0.10 6.165 0.123 ± 0.026 0.459 ± 0.031 Figure 5 (i) 35–40 −1.07 ± 0.17 0.01 ± 0.01 1.98 ± 0.10 8.068 0.123 ± 0.026 0.465 ± 0.030 Figure 5 (j) 40–45 −1.02 ± 0.20 0.01 ± 0.01 2.02 ± 0.08 10.256 0.123 ± 0.026 0.477 ± 0.024 Figure 5 (k) 45–50 −1.05 ± 0.20 0.01 ± 0.01 2.07 ± 0.08 8.595 0.123 ± 0.026 0.491 ± 0.023 Figure 5 (l) 50–55 −1.10 ± 0.22 0.01 ± 0.01 2.10 ± 0.08 13.713 0.123 ± 0.026 0.500 ± 0.023 62.4 GeV Figure 6 (a) 0–3 −1.80 ± 0.21 0.05 ± 0.01 2.00 ± 0.07 0.264 0.088 ± 0.019 0.370 ± 0.020 Figure 6 (b) 3–6 −1.50 ± 0.21 0.04 ± 0.01 2.00 ± 0.09 0.342 0.088 ± 0.019 0.370 ± 0.025 Figure 6 (c) 6–10 −1.60 ± 0.20 0.04 ± 0.01 2.10 ± 0.10 0.262 0.088 ± 0.019 0.370 ± 0.028 Figure 6 (d) 10–15 −1.60 ± 0.20 0.04 ± 0.01 2.13 ± 0.10 0.170 0.088 ± 0.019 0.406 ± 0.027 Figure 6 (e) 15–20 −1.40 ± 0.28 0.03 ± 0.01 2.18 ± 0.08 0.100 0.088 ± 0.019 0.419 ± 0.022 Figure 6 (f) 20–25 −1.40 ± 0.30 0.03 ± 0.01 2.25 ± 0.10 0.096 0.088 ± 0.019 0.438 ± 0.026 Figure 6 (g) 25–30 −1.40 ± 0.28 0.02 ± 0.01 2.30 ± 0.08 0.133 0.088 ± 0.019 0.451 ± 0.021 Figure 6 (h) 30–35 −1.40 ± 0.30 0.02 ± 0.01 2.35 ± 0.11 0.129 0.088 ± 0.019 0.464 ± 0.028 Figure 6 (i) 35–40 −1.40 ± 0.25 0.02 ± 0.01 2.45 ± 0.10 0.123 0.088 ± 0.019 0.489 ± 0.024 Figure 6 (j) 40–45 −1.40 ± 0.18 0.01 ± 0.01 2.48 ± 0.10 0.095 0.088 ± 0.019 0.496 ± 0.024 Figure 6 (k) 45–50 −1.40 ± 0.20 0.01 ± 0.01 2.48 ± 0.08 0.159 0.088 ± 0.019 0.496 ± 0.019 Figure 6 (l) 50–55 −1.40 ± 0.20 0.01 ± 0.01 2.55 ± 0.10 0.176 0.088 ± 0.019 0.513 ± 0.024 200 GeV Figure 7 (a) 0–3 −2.35 ± 0.28 0.04 ± 0.02 2.50 ± 0.08 0.194 0.066 ± 0.014 0.415 ± 0.019 Figure 7 (b) 3–6 −2.35 ± 0.28 0.04 ± 0.02 2.55 ± 0.10 0.114 0.066 ± 0.014 0.427 ± 0.023 Figure 7 (c) 6–10 −2.30 ± 0.25 0.04 ± 0.02 2.60 ± 0.10 0.085 0.066 ± 0.014 0.438 ± 0.023 Figure 7 (d) 10–15 −2.25 ± 0.24 0.03 ± 0.01 2.65 ± 0.12 0.125 0.066 ± 0.014 0.450 ± 0.027 Figure 7 (e) 15–20 −2.30 ± 0.25 0.04 ± 0.02 2.65 ± 0.12 0.121 0.066 ± 0.014 0.450 ± 0.027 Figure 7 (f) 20–25 −2.25 ± 0.27 0.03 ± 0.01 2.70 ± 0.08 0.129 0.066 ± 0.014 0.461 ± 0.018 Figure 7 (g) 25–30 −2.25 ± 0.32 0.03 ± 0.02 2.78 ± 0.08 0.076 0.066 ± 0.014 0.479 ± 0.017 Figure 7 (h) 30–35 −2.25 ± 0.35 0.03 ± 0.02 2.78 ± 0.10 0.082 0.066 ± 0.014 0.479 ± 0.022 Figure 7 (i) 35–40 −2.25 ± 0.33 0.03 ± 0.02 2.85 ± 0.10 0.053 0.066 ± 0.014 0.494 ± 0.021 Figure 7 (j) 40–45 −2.25 ± 0.35 0.03 ± 0.02 2.85 ± 0.08 0.074 0.066 ± 0.014 0.494 ± 0.017 Figure 7 (k) 45–50 −2.25 ± 0.32 0.03 ± 0.02 2.85 ± 0.10 0.083 0.066 ± 0.014 0.494 ± 0.021 Figure 7 (l) 50–55 −2.25 ± 0.32 0.03 ± 0.02 2.95 ± 0.07 0.085 0.066 ± 0.014 0.514 ± 0.014