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Table 1.

Mean abundances in the mass fraction of different chemical species in the mass ejected by 11 massive Pop III star models.

Mtot MCO




(M) (M) 10% 40% CO core
491 104 0.360 0.430 0.002 0.056 0.150 0.256 0.450 0.002 0.079 0.210 0.235 0.451 0.002 0.084 0.224
771 165 0.319 0.460 0.002 0.053 0.162 0.235 0.466 0.002 0.074 0.218 0.217 0.465 0.002 0.079 0.232
778 163 0.299 0.473 0.003 0.038 0.180 0.240 0.454 0.002 0.058 0.235 0.220 0.447 0.002 0.065 0.253
932 247 0.339 0.588 0.002 0.056 0.015 0.185 0.682 0.002 0.102 0.028 0.161 0.695 0.003 0.108 0.031
1135 440 0.204 0.669 0.003 0.086 0.038 0.124 0.691 0.003 0.122 0.058 0.115 0.691 0.005 0.126 0.063
1331 317 0.293 0.519 0.005 0.067 0.114 0.201 0.528 0.003 0.103 0.163 0.186 0.528 0.003 0.108 0.172
1662 630 0.198 0.766 0.001 0.031 0.004 0.095 0.852 0.001 0.047 0.004 0.078 0.864 0.002 0.050 0.006
1923 746 0.232 0.577 0.001 0.046 0.137 0.181 0.573 0.001 0.061 0.174 0.171 0.571 0.001 0.064 0.183
3053 650 0.202 0.737 0.000 0.018 0.004 0.202 0.737 0.000 0.022 0.004 0.157 0.765 0.001 0.033 0.012
4477 759 0.297 0.687 0.000 0.015 0.001 0.153 0.816 0.001 0.029 0.001 0.073 0.884 0.003 0.034 0.006
6127 1252 0.173 0.779 0.001 0.039 0.006 0.079 0.855 0.001 0.056 0.008 0.040 0.875 0.004 0.060 0.017

Notes. The first column shows the final mass of each model and the second column depicts the mass of CO core at the end of core helium burning. The next 5 columns depict the mean abundances (see Eq. (1)) in the mass fraction for 1H, 4He, 12C, 14N and 16O when the outermost 10% of total mass is ejected. The following five columns are the mean abundance in the ejecta when 40% of the outermost total mass is ejected and the final five columns when all the mass above CO core is ejected.

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