On Pseudorapidity Distribution and Speed of Sound in High Energy Heavy Ion Collisions Based on a New Revised Landau Hydrodynamic Model

Table 9

Values of intercept, slope, and   for the linear relations in Figures 14(a)–14(g) and for the linear relations   in Figure 14(h).

Figure	or type	Intercept		Slope
		Value	Error	Value	Error
Figure 14(a)	19.6 GeV	0.130	0.028	0	0	0
	62.4 GeV	0.088	0.019	0	0	0
	130 GeV	0.073	0.016	0	0	0
	200 GeV	0.066	0.014	0	0	0
Figure 14(b)	19.6 GeV	0.364	0.004	0.003	0.001	0.019
	62.4 GeV	0.354	0.005	0.004	0.001	0.030
	130 GeV	0.386	0.004	0.002	0.001	0.022
	200 GeV	0.398	0.006	0.002	0.001	0.042
Figure 14(c)	22.4 GeV	0.123	0.026	0	0	0
	62.4 GeV	0.088	0.019	0	0	0
	200 GeV	0.066	0.014	0	0	0
Figure 14(d)	22.4 GeV	0.374	0.009	0.003	0.001	0.115
	62.4 GeV	0.368	0.004	0.003	0.001	0.025
	200 GeV	0.421	0.004	0.002	0.001	0.021
Figure 14(e)		0.066	0.014	0	0	0
		0.553	0.033	−0.002	0.001	0.478
Figure 14(f)		0.042	0.009	0	0	0
		0.500	0.001	0.001	0.001	0.001
Figure 14(g)		0.310	0.056	0	0	0
		0.226	0.031	0.002	0.001	0.159
Figure 14(h)		0.223	0.022	−0.004	0.001	0.170
		0.255	0.023	0.001	0.001	0.294