2019ApJ...876..134C


Query : 2019ApJ...876..134C

2019ApJ...876..134C - Astrophys. J., 876, 134-134 (2019/May-2)

The dependence of convective core overshooting on stellar mass: reality check and additional evidence.

CLARET A. and TORRES G.

Abstract (from CDS):

Overshooting from the convective cores of stars more massive than about 1.2 M has a profound impact on their subsequent evolution. And yet, the formulation of the overshooting mechanism in current stellar evolution models has a free parameter (fov in the diffusive approximation) that remains poorly constrained by observations, affecting the determination of astrophysically important quantities such as stellar ages. In an earlier series of papers, we assembled a sample of 37 well-measured detached eclipsing binaries to calibrate the dependence of fov on stellar mass, showing that it increases sharply up to a mass of roughly 2 M, and remains constant thereafter out to at least 4.4 M. Recent claims have challenged the utility of eclipsing binaries for this purpose, on the basis that the uncertainties in fov from the model fits are typically too large to be useful, casting doubt on a dependence of overshooting on mass. Here we reexamine those claims and show them to be too pessimistic, mainly because they did not account for all available constraints-both observational and theoretical-in assessing the true uncertainties. We also take the opportunity to add semiempirical fov determinations for 13 additional binaries to our previous sample, and to update the values for 9 others. All are consistent with and strengthen our previous conclusions, supporting a dependence of fov on mass that is now based on estimates for a total of 50 binary systems (100 stars).

Abstract Copyright: © 2019. The American Astronomical Society. All rights reserved.

Journal keyword(s): binaries: eclipsing - stars: evolution - stars: interiors

Simbad objects: 31

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Number of rows : 31
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 V* AI Phe SB* 01 09 34.1924055096 -46 15 56.071719360   9.26 8.60     G3V 147 0
2 OGLE LMC-ECL-1866 EB* 04 52 15.2769484488 -68 19 10.222622148     15.986 15.453 15.010 ~ 20 0
3 OGLE LMC-CEP-227 cC* 04 52 15.6979950672 -70 14 31.242378408     15.317   14.438 ~ 57 0
4 OGLE LMC-ECL-3160 LP* 04 55 51.4783969128 -69 13 47.925605388     16.83 15.978 15.869 ~ 25 0
5 2MASS J05043288-6920509 LP* 05 04 32.8759490616 -69 20 51.030442032     15.62 14.736 14.659 ~ 23 0
6 OGLE J051019.64-685812.3 EB* 05 10 19.65 -68 58 12.0     16.673   15.715 ~ 30 0
7 2MASS J05114945-6705451 LP* 05 11 49.4660106384 -67 05 45.128063004     16.21 15.70 15.130 ~ 20 0
8 2MASS J05115174-6931010 LP* 05 11 51.7830315528 -69 31 01.137728172     17.10 16.56 16.070 ~ 8 0
9 2MASS J05140190-6841184 LP* 05 14 01.908 -68 41 18.41     16.58 16.04 15.377 ~ 20 0
10 2MASS J05140595-6915568 LP* 05 14 05.9513254032 -69 15 56.782018224     16.56 15.639   ~ 21 1
11 OGLE LMC-SC7 333638 EB* 05 19 12.905 -69 06 45.45     16.82 16.31 16.048 ~ 9 0
12 2MASS J05194538-6944384 LP* 05 19 45.383 -69 44 38.44     17.29 16.66 15.974 ~ 9 0
13 2MASS J05195369-6917204 LP* 05 19 53.696 -69 17 20.43     17.07 16.143 16.050 ~ 11 0
14 OGLE LMC-ECL-13360 EB* 05 20 59.4573624528 -70 07 35.290203348     15.818   14.800 ~ 8 0
15 OGLE LMC-SC21 116240 EB* 05 21 23.3454398616 -70 33 00.003463488     17.356 16.92 16.386 ~ 10 0
16 2MASS J05252555-6933044 LP* 05 25 25.550 -69 33 04.49     17.01 16.40 15.620 ~ 25 0
17 2MASS J05325304-6859123 LP* 05 32 53.0670286320 -68 59 12.242782860     17.66 16.416 16.199 ~ 11 0
18 2MASS J05395119-6753005 LP* 05 39 51.1936404480 -67 53 00.599763876     16.84 16.34 15.778 ~ 7 0
19 OGLE LMC-ECL-24887 EB* 05 50 39.0329116632 -69 14 20.617707228     17.677   16.559 ~ 6 0
20 OGLE LMC-CEP-4506 cC* 05 53 29.3579289240 -67 53 59.361341352     15.459   14.778 ~ 23 0
21 OGLE LMC-ECL-25658 EB* 06 01 58.7793442320 -68 30 55.138566096     16.995 16.53 15.870 G8III+G9III 16 0
22 V* AY Cam SB* 08 25 51.7866730824 +77 13 06.845960820   10.12 9.72     A0V+F0V 62 0
23 NGC 2682 OpC 08 51 23.0 +11 48 50           ~ 2342 0
24 * chi02 Hya EB* 11 05 57.5699938080 -27 17 16.272708396   5.64 5.71     B8V 115 0
25 V* SZ Cen EB* 13 50 35.0928355776 -58 29 57.097515840   8.89 8.59     A6III 102 0
26 V* V4089 Sgr EB* 19 34 08.4856054632 -40 02 04.702519428   6.00 5.91     A2V 62 0
27 HD 187669 EB* 19 52 22.0878263112 -32 33 39.740568048   10.12 8.88     K0III 24 0
28 HD 187699 * 19 52 46.9342362456 -37 39 42.677358228   9.43 8.18     K1/2III 10 0
29 HD 188872 SB* 19 55 11.4169251384 +46 55 48.871496856   10.01 9.56     F2II 29 0
30 HD 190585 EB* 20 03 48.3209367264 +45 36 14.805207576   10.74 9.65     K2 42 0
31 V* BK Peg SB* 23 47 08.4664310208 +26 33 59.970121200   10.46 10.04     F8 74 0

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