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Table A.1.

Mass estimates of R136a from single and binary stellar mergers for the winds described in this work.

Method and Binarity R136a1 R136a2 R136a3



MZAMS Mcurrent MZAMS Mcurrent MZAMS Mcurrent
rdw (Single) 315 13 + 11 $ ^{+11}_{-13} $ 295 16 + 14 $ ^{+14}_{-16} $ 240 6 + 6 $ ^{+6}_{-6} $ 225 8 + 9 $ ^{+9}_{-8} $ 241 5 + 5 $ ^{+5}_{-5} $ 232 9 + 9 $ ^{+9}_{-9} $
rdw (Stellar merger) 186 30 + 53 $ ^{+53}_{-30} $ 278 18 + 25 $ ^{+25}_{-18} $ 146 21 + 42 $ ^{+42}_{-21} $ 222 7 + 7 $ ^{+7}_{-7} $ 145 21 + 41 $ ^{+41}_{-21} $ 221 9 + 9 $ ^{+9}_{-9 } $
Γe (Single) 389 64 + 1 $ ^{+1}_{-64} $ 202 66 + 12 $ ^{+12}_{-66} $ 296 20 + 12 $ ^{+12}_{-20} $ 169 13 + 13 $ ^{+13}_{-13} $ 286 25 + 4 $ ^{+4}_{-25} $ 180 14 + 42 $ ^{+42}_{-14} $
Γe (Stellar merger) 207 56 + 69 $ ^{+69}_{-56} $ 200 6 + 10 $ ^{+10}_{-6} $ 160 40 + 53 $ ^{+53}_{-40} $ 164 4 + 13 $ ^{+13}_{-4} $ 162 36 + 52 $ ^{+52}_{-36} $ 171 11 + 12 $ ^{+12}_{-11} $
L/M (Single) 359 10 + 30 $ ^{+30}_{-10} $ 254 44 + 22 $ ^{+22}_{-44} $ 260 1 + 130 $ ^{+130}_{-1} $ 201 80 + 32 $ ^{+32}_{-80} $ 257 4 + 39 $ ^{+39}_{-4} $ 220 41 + 17 $ ^{+17}_{-41} $
L/M (Stellar merger, Class 1) 141 23 + 22 $ ^{+22}_{-23} $ 185 14 + 25 $ ^{+25}_{-14} $ 121 16 + 33 $ ^{+33}_{-16} $ 138 8 + 8 $ ^{+8}_{-8} $ 127 20 + 36 $ ^{+36}_{-20} $ 138 8 + 9 $ ^{+9}_{-8} $
L/M (Stellar merger, Class 2) 310 33 + 27 $ ^{+27}_{-33} $ 204 29 + 23 $ ^{+23}_{-29} $ 259 30 + 52 $ ^{+52}_{-30} $ 141 14 + 2 $ ^{+2}_{-14} $ 251 32 + 55 $ ^{+55}_{-32} $ 140 9 + 8 $ ^{+8}_{-9} $

Brands et al. (2022) 273 36 + 25 $ ^{+25}_{-36} $ 222 29 + 28 $ ^{+28}_{-29} $ 221 12 + 16 $ ^{+16}_{-12} $ 186 15 + 17 $ ^{+17}_{-15} $ 213 11 + 12 $ ^{+12}_{-11} $ 179 11 + 16 $ ^{+16}_{-11} $
Bestenlehner et al. (2020) 251 35 + 48 $ ^{+48}_{-35} $ 215 31 + 45 $ ^{+45}_{-31} $ 211 32 + 31 $ ^{+31}_{-32} $ 187 33 + 23 $ ^{+23}_{-33} $ 181 31 + 29 $ ^{+29}_{-31} $ 154 23 + 28 $ ^{+28}_{-23} $
Crowther et al. (2010) 320 40 + 100 $ ^{+100}_{-40} $ 265 35 + 80 $ ^{+80}_{-35} $ 240 45 + 45 $ ^{+45}_{-45} $ 195 35 + 35 $ ^{+35}_{-35} $ 165 30 + 30 $ ^{+30}_{-30} $ 135 20 + 25 $ ^{+25}_{-20} $

Notes. Column 1: The mass-loss recipe used and the origin of the star. Columns 2 and 3: ZAMS mass and current mass estimate of R136a1. Columns 4 and 5: ZAMS mass and current mass estimate of R136a2. Columns 5 and 6: ZAMS mass and current mass estimate of R136a3. In the case of a stellar merger, the MZAMS shows the mass of the primary star only. For stellar mergers computed with L/M, we split the results into two mass regimes: primary mass below 200 M (class 1) and above 200 M (class 2), to account for the bimodal distribution. The last three rows present comparisons from the literature, all of which assume a single star origin. Crowther et al. (2010) results use the Geneva stellar evolution tracks, and the results from Bestenlehner et al. (2020) and Brands et al. (2022) both used the stellar models from Brott et al. (2011) and Köhler et al. (2015).

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