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 57 which show Cu-Cu collisions for different energies and centralities.

FigureBin (%)

22.4 GeV
Figure 5(a)0–3−1.20 ± 0.200.03 ± 0.021.60 ± 0.080.2380.123 ± 0.0260.342 ± 0.027
Figure 5(b)3–6−1.10 ± 0.190.01 ± 0.011.70 ± 0.080.1150.123 ± 0.0260.375 ± 0.027
Figure 5(c)6–10−1.10 ± 0.170.01 ± 0.011.78 ± 0.100.1300.123 ± 0.0260.402 ± 0.033
Figure 5(d)10–15−1.12 ± 0.200.01 ± 0.011.82 ± 0.111.2640.123 ± 0.0260.415 ± 0.035
Figure 5(e)15–20−1.14 ± 0.230.01 ± 0.011.85 ± 0.062.7960.123 ± 0.0260.424 ± 0.019
Figure 5(f)20–25−1.10 ± 0.210.01 ± 0.011.94 ± 0.063.0010.123 ± 0.0260.453 ± 0.019
Figure 5(g)25–30−1.10 ± 0.200.01 ± 0.011.95 ± 0.074.0560.123 ± 0.0260.456 ± 0.022
Figure 5(h)30–35−1.04 ± 0.200.01 ± 0.011.96 ± 0.106.1650.123 ± 0.0260.459 ± 0.031
Figure 5(i)35–40−1.07 ± 0.170.01 ± 0.011.98 ± 0.108.0680.123 ± 0.0260.465 ± 0.030
Figure 5(j)40–45−1.02 ± 0.200.01 ± 0.012.02 ± 0.0810.2560.123 ± 0.0260.477 ± 0.024
Figure 5(k)45–50−1.05 ± 0.200.01 ± 0.012.07 ± 0.088.5950.123 ± 0.0260.491 ± 0.023
Figure 5(l)50–55−1.10 ± 0.220.01 ± 0.012.10 ± 0.0813.7130.123 ± 0.0260.500 ± 0.023

62.4 GeV
Figure 6(a)0–3−1.80 ± 0.210.05 ± 0.012.00 ± 0.070.2640.088 ± 0.0190.370 ± 0.020
Figure 6(b)3–6−1.50 ± 0.210.04 ± 0.012.00 ± 0.090.3420.088 ± 0.0190.370 ± 0.025
Figure 6(c)6–10−1.60 ± 0.200.04 ± 0.012.10 ± 0.100.2620.088 ± 0.0190.370 ± 0.028
Figure 6(d)10–15−1.60 ± 0.200.04 ± 0.012.13 ± 0.100.1700.088 ± 0.0190.406 ± 0.027
Figure 6(e)15–20−1.40 ± 0.280.03 ± 0.012.18 ± 0.080.1000.088 ± 0.0190.419 ± 0.022
Figure 6(f)20–25−1.40 ± 0.300.03 ± 0.012.25 ± 0.100.0960.088 ± 0.0190.438 ± 0.026
Figure 6(g)25–30−1.40 ± 0.280.02 ± 0.012.30 ± 0.080.1330.088 ± 0.0190.451 ± 0.021
Figure 6(h)30–35−1.40 ± 0.300.02 ± 0.012.35 ± 0.110.1290.088 ± 0.0190.464 ± 0.028
Figure 6(i)35–40−1.40 ± 0.250.02 ± 0.012.45 ± 0.100.1230.088 ± 0.0190.489 ± 0.024
Figure 6(j)40–45−1.40 ± 0.180.01 ± 0.012.48 ± 0.100.0950.088 ± 0.0190.496 ± 0.024
Figure 6(k)45–50−1.40 ± 0.200.01 ± 0.012.48 ± 0.080.1590.088 ± 0.0190.496 ± 0.019
Figure 6(l)50–55−1.40 ± 0.200.01 ± 0.012.55 ± 0.100.1760.088 ± 0.0190.513 ± 0.024

200 GeV
Figure 7(a)0–3−2.35 ± 0.280.04 ± 0.022.50 ± 0.080.1940.066 ± 0.0140.415 ± 0.019
Figure 7(b)3–6−2.35 ± 0.280.04 ± 0.022.55 ± 0.100.1140.066 ± 0.0140.427 ± 0.023
Figure 7(c)6–10−2.30 ± 0.250.04 ± 0.022.60 ± 0.100.0850.066 ± 0.0140.438 ± 0.023
Figure 7(d)10–15−2.25 ± 0.240.03 ± 0.012.65 ± 0.120.1250.066 ± 0.0140.450 ± 0.027
Figure 7(e)15–20−2.30 ± 0.250.04 ± 0.022.65 ± 0.120.1210.066 ± 0.0140.450 ± 0.027
Figure 7(f)20–25−2.25 ± 0.270.03 ± 0.012.70 ± 0.080.1290.066 ± 0.0140.461 ± 0.018
Figure 7(g)25–30−2.25 ± 0.320.03 ± 0.022.78 ± 0.080.0760.066 ± 0.0140.479 ± 0.017
Figure 7(h)30–35−2.25 ± 0.350.03 ± 0.022.78 ± 0.100.0820.066 ± 0.0140.479 ± 0.022
Figure 7(i)35–40−2.25 ± 0.330.03 ± 0.022.85 ± 0.100.0530.066 ± 0.0140.494 ± 0.021
Figure 7(j)40–45−2.25 ± 0.350.03 ± 0.022.85 ± 0.080.0740.066 ± 0.0140.494 ± 0.017
Figure 7(k)45–50−2.25 ± 0.320.03 ± 0.022.85 ± 0.100.0830.066 ± 0.0140.494 ± 0.021
Figure 7(l)50–55−2.25 ± 0.320.03 ± 0.022.95 ± 0.070.0850.066 ± 0.0140.514 ± 0.014