Research Article

A New Two-Component Model for Hadron Production in Heavy-Ion Collisions

Table 1

The fitting parameters for various particles with double-Tsallis distribution (3).

ParticleCentrality [%]

0–52811.280.20012.5513.470.2515.92
5–102322.400.19912.2813.740.2566.12
10–201805.780.19411.160.2190.6567.47
20–401079.340.1829.790.01341.22210.66
40–60464.420.1668.660.005301.1379.59
60–80148.160.1497.760.0009581.0408.18

0–5103.770.36080.597.360.2516.08
5–1084.950.35971.498.680.2426.13
10–2064.160.35252.866.870.2586.36
20–4036.890.33231.415.000.2546.36
40–6013.960.30020.743.940.2306.36
60–805.260.25111.710.02050.6529.79

0–545.640.36434.502.040.2536.61
5–1033.400.37843.490.3750.4128.12
10–2029.410.35127.330.4350.3346.92
20–4010.860.38547.700.9910.3097.75
40–603.470.37745.530.6040.2907.67
60–800.9150.34121.390.03590.3256.79