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Table 1

CO-core mass, remnant mass, and ejected masses in hydrogen, helium, carbon, nitrogen, oxygen, and remaining heavy elements for the 15 M models at the three metallicities and all the rotation rates.

ω ini M CO M rem 1

Z = 0.002 0.00 2.6961 1.4265 6.8329 5.0423 0.3638 0.0056 0.6237 0.2129
0.10 3.0113 1.4915 6.5290 4.8647 0.3795 0.0058 0.9746 0.1920
0.30 3.1037 1.5097 6.0193 5.1801 0.4782 0.0066 1.1124 0.1496
0.50 3.0275 1.4947 5.5969 5.2227 0.5249 0.0071 1.1904 0.1022
0.60 2.8358 1.4556 5.8074 5.5233 0.5636 0.0084 1.0755 0.0744
0.70 3.3706 1.5619 5.1903 4.8331 0.5772 0.0071 1.5936 0.1491
0.80 3.3276 1.5535 4.9495 5.2080 0.6117 0.0079 1.5929 0.1397
0.90 3.7427 1.6335 4.3507 4.8306 0.6983 0.0069 1.9760 0.0207
0.95 3.8653 1.6568 4.1340 4.7515 0.7848 0.0069 2.0926 0.0442

Z = 0.006 0.00 2.6607 1.4191 6.2795 4.8178 0.4218 0.0167 0.6678 0.1142
0.10 2.8571 1.4600 5.7171 4.5974 0.3637 0.0162 0.8697 0.2075
0.30 3.1193 1.5128 5.2323 4.7427 0.4892 0.0167 1.1535 0.1483
0.50 3.0771 1.5045 5.2111 5.0265 0.5610 0.0185 1.1342 0.1446
0.60 2.9607 1.4815 5.1949 5.0690 0.5576 0.0192 1.1200 0.1409
0.70 3.1077 1.5105 5.2193 4.7928 0.6010 0.0203 1.4027 0.1191
0.80 3.1568 1.5202 4.9762 4.7993 0.5864 0.0204 1.5126 0.1071
0.90 3.4196 1.5714 3.9929 4.4800 0.6119 0.0180 1.6830 0.1459
0.95 3.4000 1.5676 3.8333 4.3666 0.6419 0.0175 1.6814 0.1237

Z = 0.014 0.00 2.4065 1.3655 5.8070 4.8193 0.2956 0.0400 0.4983 0.2577
0.10 2.7714 1.4422 4.8298 4.2007 0.3913 0.0337 0.8906 0.1801
0.30 3.3153 1.5511 3.4444 3.5356 0.5674 0.0272 1.4047 0.1666
0.50 3.1867 1.5260 3.4473 3.7215 0.6409 0.0287 1.3235 0.1908
0.60 3.2256 1.5337 3.4455 3.8259 0.5787 0.0309 1.4612 0.1081
0.70 3.2558 1.5395 3.4518 3.9198 0.5009 0.0334 1.5509 0.0936
0.80 2.9022 1.4694 4.1405 4.7817 0.5307 0.0392 1.0723 0.1649
0.90 2.9977 1.4888 4.0481 4.3689 0.6091 0.0382 1.2925 0.1168
0.95 3.0261 1.4944 4.2465 4.6714 0.5045 0.0420 1.1951 0.1783

Notes.All masses are expressed in M units.

(1)

The remnant mass is computed following the same method as in Hirschi et al. (2005) and Georgy et al. (2009).

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