2019A&A...622A..50H


Query : 2019A&A...622A..50H

2019A&A...622A..50H - Astronomy and Astrophysics, volume 622A50-50 (2019/2-1)

Massive star evolution: rotation, winds, and overshooting vectors in the mass-luminosity plane. I. A calibrated grid of rotating single star models.

HIGGINS E.R. and VINK J.S.

Abstract (from CDS):


Context. Massive star evolution is dominated by various physical effects, including mass loss, overshooting, and rotation, but the prescriptions of their effects are poorly constrained and even affect our understanding of the main sequence.
Aims. We aim to constrain massive star evolution models using the unique test-bed eclipsing binary HD 166734 with new grids of MESA stellar evolution models, adopting calibrated prescriptions of overshooting, mass loss, and rotation.
Methods. We introduce a novel tool, called the mass-luminosity plane or M-L plane, as an equivalent to the traditional HR diagram, utilising it to reproduce the test-bed binary HD 166734 with newly calibrated MESA stellar evolution models for single stars.
Results. We can only reproduce the Galactic binary system with an enhanced amount of core overshooting (αov=0.5), mass loss, and rotational mixing. We can utilise the gradient in the M-L plane to constrain the amount of mass loss to 0.5-1.5 times the standard prescription test-bed, and we can exclude extreme reduction or multiplication factors. The extent of the vectors in the M-L plane leads us to conclude that the amount of core overshooting is larger than is normally adopted in contemporary massive star evolution models. We furthermore conclude that rotational mixing is mandatory to obtain the correct nitrogen abundance ratios between the primary and secondary components (3:1) in our test-bed binary system.
Conclusions. Our calibrated grid of models, alongside our new M-L plane approach, present the possibility of a widened main sequence due to an increased demand for core overshooting. The increased amount of core overshooting is not only needed to explain the extended main sequence, but the enhanced overshooting is also needed to explain the location of the upper-luminosity limit of the red supergiants. Finally, the increased amount of core overshooting has - via the compactness parameter - implications for supernova explodability.

Abstract Copyright: © ESO 2019

Journal keyword(s): stars: massive - stars: mass-loss - stars: evolution - stars: rotation - stars: luminosity function - mass function - stars: early-type

VizieR on-line data: <Available at CDS (J/A+A/622/A50): list.dat history_columns.list models/*>

Simbad objects: 32

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Number of rows : 32
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
2 HD 46223 Y*O 06 32 09.3068103600 +04 49 24.705695568 6.73 7.50 7.28 6.95 6.79 O4V((f)) 406 0
3 HD 46202 bC* 06 32 10.4706981304 +04 57 59.764912343 7.60 8.332 8.269 7.98 7.86 O9.2V 300 0
4 HD 63005 * 07 45 49.0332176232 -26 29 31.436407572 8.29 9.12 9.13 9.64   O6.5IV 89 0
5 HD 64568 * 07 53 38.2051918848 -26 14 02.598056556 8.64 9.50 9.39 9.77 9.204 O3V((f*))z 116 0
6 HD 69106 * 08 14 03.7995306624 -36 57 07.938057852 6.12 7.020 7.128 8.02   O9.7IIn 129 0
7 HD 69464 s*b 08 15 48.5652200520 -35 37 52.863334428 8.47 9.11 8.80 9.42   O7Ib(f) 108 0
8 HD 75211 SB* 08 47 01.5921294816 -44 04 28.848481212 7.35 7.90 7.50 8.28   O8.5II((f)) 99 0
9 HD 75222 s*b 08 47 25.1378783304 -36 45 02.670440616 7.24 7.80 7.42 8.22   O9.7Iab 102 0
10 CD-44 4865 * 08 50 02.2858329192 -44 34 39.926878500 9.88 10.16 9.63 9.67   B0III 57 0
11 CD-43 4690 * 08 50 52.0461382848 -43 50 22.900242948 10.05 10.48 9.79 9.68   O7.5 35 0
12 HD 76968 V* 08 57 28.8524478672 -50 44 58.197488784 6.53 7.33 7.21 7.01 6.87 O9.2Ib 99 1
13 CD-47 4551 s*b 08 57 54.6180604176 -47 44 15.708893424 9.11 9.41 8.54 8.92   O5Ifc 84 0
14 HD 78344 * 09 05 51.3294079248 -47 46 06.834233424 10.10 10.12 9.00 8.55 8.16 O9.5/B0(Ib) 87 0
15 HD 302505 * 10 05 20.5426689984 -58 44 20.696151660 9.41 9.95 9.89 9.79   B2 37 0
16 HD 91572 * 10 33 12.2657051544 -58 10 13.653979140 7.44 8.29 8.24 9.03   O6.5V((f))z 98 0
17 HD 91824 SB* 10 34 46.6322493936 -58 09 22.038466896 7.17 8.11 8.14 9.02   O7V((f))z 165 0
18 HD 92504 * 10 39 36.8683124520 -57 27 40.634282304 7.47 8.38 8.46 9.296   O8.5V(n) 79 0
19 CD-58 3529 * 10 43 59.9072622960 -59 32 25.452459240 8.631 9.439 9.286 9.73 9.11 O7V((f))z 31 0
20 HD 93204 * 10 44 32.3390794992 -59 44 31.020804780 7.63 8.52 8.42 8.20 7.92 O5.5V((f)) 200 0
21 HD 93222 Y*O 10 44 36.2481200208 -60 05 28.890759120 7.26 8.18 8.10 8.91   O7V((f))z 212 0
22 CD-59 3300 * 10 44 41.7962304024 -59 46 56.405228916 8.07 8.79 8.57 9.33   O6V((f)) 150 0
23 HD 93843 Er* 10 48 37.7715351864 -60 13 25.518487656 6.37 7.29 7.33 8.23   O5III(fc) 184 0
24 HD 94370 ** 10 52 23.277192 -58 44 47.56704 7.19 8.69 8.92 8.84   O7.5III(f) 46 0
25 HD 94963 Em* 10 56 35.7867321168 -61 42 32.287821516 6.35 7.17 7.26 8.10   O7II(f) 93 0
26 HD 97848 * 11 14 31.9027108872 -59 01 28.842530124 7.66 8.59 8.60 9.43   O8V 90 0
27 HD 148546 Pu* 16 30 23.3122183296 -37 58 21.169697268 7.28 7.99 7.71 8.58   O9Iab 91 0
28 HD 151804 s*b 16 51 33.7218052272 -41 13 49.919519496 4.45 5.29 5.22     O8Iaf 389 0
29 HD 152003 s*b 16 52 47.3744351712 -41 47 08.990966004 6.90 7.47 7.08 6.72 6.35 O9.7IabNwk 132 1
30 HD 152249 s*b 16 54 11.6395658856 -41 50 57.295111524 5.91 6.65 6.45     OC9Iab 254 0
31 HD 166734 s*b 18 12 24.6551425392 -10 43 53.060750040 9.36 9.49 8.42 7.33 6.47 O7.5Iabf 193 0
32 HD 169582 s*b 18 25 43.1466928224 -09 45 11.033442216 8.74 9.24 8.70     O6Iaf 95 0

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