Table 2:
The stellar yields (expressed in solar masses) as derived in this paper, namely those that produce the best
agreement with observations.
) |
K |
Sc |
Ti |
Cr |
Mn |
Co |
Ni |
11.00 |
.4040E-04 |
.2564E-05 |
.3300E-03 |
.2037E-02 |
.1290E-03 |
.1272E-03 |
.1670E-01 |
12.00 |
.1712E-02 |
.2714E-05 |
.3960E-03 |
.2091E-02 |
.1400E-03 |
.2010E-04 |
.7000E-02 |
13.00 |
.6160E-04 |
.2553E-05 |
.3990E-03 |
.1929E-02 |
.4490E-03 |
.2019E-04 |
.1120E-01 |
15.00 |
.2544E-03 |
.6751E-05 |
.7515E-03 |
.1371E-02 |
.4710E-03 |
.3030E-04 |
.6800E-02 |
18.00 |
.1176E-03 |
.2415E-05 |
.8400E-03 |
.8910E-03 |
.4040E-03 |
.4290E-04 |
.3760E-02 |
19.00 |
.6952E-03 |
.6038E-05 |
.8670E-03 |
.7980E-03 |
.2060E-03 |
.7710E-04 |
.4680E-02 |
20.00 |
.7496E-03 |
.1086E-04 |
.8700E-03 |
.5400E-03 |
.2130E-03 |
.8160E-04 |
.4440E-02 |
22.00 |
.1200E-02 |
.2530E-04 |
.8940E-04 |
.4050E-03 |
.2300E-03 |
.8820E-04 |
.1120E-01 |
25.00 |
.4032E-03 |
.2622E-05 |
.7500E-04 |
.3900E-03 |
.2580E-03 |
.7500E-03 |
.7590E-02 |
30.00 |
.2648E-03 |
.1610E-05 |
.1500E-03 |
.4500E-03 |
.1040E-03 |
.8070E-03 |
.3350E-01 |
35.00 |
.1328E-03 |
.1345E-05 |
.4500E-03 |
.4500E-03 |
.1330E-03 |
.7950E-03 |
.2040E-02 |
40.00 |
.8960E-04 |
.1621E-05 |
.4560E-03 |
.9120E-04 |
.1340E-03 |
.8250E-03 |
.2120E-02 |
50.00 |
.8960E-04 |
.1621E-05 |
.4560E-03 |
.6120E-04 |
.1340E-03 |
.8250E-03 |
.2120E-02 |
60.00 |
.8960E-04 |
.1621E-05 |
.4560E-03 |
.3120E-04 |
.1340E-03 |
.8250E-03 |
.2120E-02 |
70.00 |
.8960E-04 |
.1621E-05 |
.4560E-03 |
.3120E-04 |
.1340E-03 |
.8250E-03 |
.2120E-02 |
80.00 |
.8960E-04 |
.1621E-05 |
.4560E-03 |
.3120E-04 |
.1340E-03 |
.8250E-03 |
.2120E-02 |
90.00 |
.8960E-04 |
.1621E-05 |
.4560E-03 |
.3120E-04 |
.1340E-03 |
.8250E-03 |
.2120E-02 |
100.00 |
.8960E-04 |
.1621E-05 |
.4560E-03 |
.3120E-04 |
.1340E-03 |
.8250E-03 |
.2120E-02 |
Source LaTeX |
All tables |
In the text