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Table 2

Most probable masses and rotation speed of the O-type component of the 11 WR+O binaries in our sample.

System Sp. type P [days] WR mass O-mass vrot [km s−1] vrot [km s−1]
begin WR
WR21 WN5o+O4-5 8.3 >19 >37 331/138 415/173
WR30 WC6+O6-8 18.8 16.4 34 ?/ >178 ?/ >205
WR31 WN4o+O8V 4.8 >11 >24 336/274 493/402
WR42 WC7+O7V 7.9 16 27 500–511/170–177 620–630/211–218
WR47 WN6o+O5V 6.2 52 60 ?/ >88 ?/ >190
WR79 WC7+O5-8 8.9 >9.5 >24 ?/ >174 ?/ >250
WR97 WN5b+O7 12.6 18 30 470/279 502/298
WR113 WC8d+O8-9IV 29.7 >11 >22 310–330/170–181 320–340/175–186
WR11 WC8+O7.5III-V 78.5 9.6 30 220/? 232/?
WR127 WN5o+O8.5V 9.5 >9 >20 300–366/? 350–416/?
WR139 WN5o+O6III-V 4.2 9.4 28 215/? 365/?

Notes. Column 7 lists the rotation velocities at the end of the RLOF (= the beginning of the WR phase) of the progenitor binary calculated as explained in the text. The vrot (Col. 6) lists the speed values resulting from the He I/He II line measurements as explained in Shara et al. (2017). A question mark meansthat this particular measurement is not available.

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