Research Article
On Pseudorapidity Distribution and Speed of Sound in High Energy Heavy Ion Collisions Based on a New Revised Landau Hydrodynamic Model
Table 8
Values of intercept, slope, and
for the linear relations
in Figures
13(a)–
13(e) and for the linear relation
in Figure
13(f).
| Figure | or | Intercept | Slope | | Value | Error | Value | Error |
| Figure 13(a) | 19.6 GeV | 1.625 | 0.017 | 0.008 | 0.001 | 0.021 | 62.4 GeV | 1.935 | 0.018 | 0.014 | 0.001 | 0.022 | 130 GeV | 2.262 | 0.016 | 0.009 | 0.001 | 0.018 | 200 GeV | 2.423 | 0.026 | 0.008 | 0.001 | 0.029 |
| Figure 13(b) | 22.4 GeV | 1.686 | 0.026 | 0.008 | 0.001 | 0.072 | 62.4 GeV | 1.987 | 0.012 | 0.011 | 0.001 | 0.015 | 200 GeV | 2.519 | 0.015 | 0.009 | 0.001 | 0.015 |
| Figure 13(c) | 0.2 TeV | 3.144 | 0.149 | −0.008 | 0.003 | 0.315 |
| Figure 13(d) | 2.76 TeV | 3.609 | 0.009 | 0.001 | 0.001 | 0.001 |
| Figure 13(e) | 10.6A GeV | 0.757 | 0.055 | 0.004 | 0.001 | 0.094 |
| Figure 13(f) | 6.7–38.7 GeV | 0.955 | 0.049 | 0.019 | 0.003 | 0.130 |
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