2024A&A...689A.234D


Query : 2024A&A...689A.234D

2024A&A...689A.234D - Astronomy and Astrophysics, volume 689A234 (2024/9-1)

The mass distribution of stellar mergers A new scenario for several FS CMa stars.

DVORAKOVA N., KORCAKOVA D., DINNBIER F. and KROUPA P.

Abstract (from CDS):

Context. FS CMa stars belong to a diverse group of stars exhibiting the B[e] phenomenon, which manifests itself mainly by the presence of forbidden emission lines and a strong infrared (IR) excess in their spectra. Only a few tens of FS CMa stars are known and their nature is still unclear. Recently, a strong magnetic field has been discovered in the FS CMa star IRAS 17449+2320. Its strength combined with an unusually high space velocity in the direction of the Galactic north pole point to the object having a post-merger nature. Such stellar mergers may provide an explanation for the complex and sometimes chaotic behaviour of some of the FS CMa stars.
Aims. In order to find out whether B-type stellar mergers are detectable, we did a statistical study of numerical simulations using Aarseth's NBODY6 code. We show the importance of stellar mergers of low- to intermediate-mass stars (from ≈1.4 to ≈8 M⊙) and for B-type stars in particular.
Methods. We analysed two sets of N-body simulations with different initial orbital period distributions. In the simulations, more massive binaries are treated differently than less massive binaries and the mass limit usually used is 5 M⊙. In addition to this, we also used the value of 2 M⊙ to test the influence of this ambiguous limit on the results. Looking at mass, distance from their birth cluster, and velocity distributions, we investigated the statistical significance of individual spectral types in terms of merger dynamics and how merger events affect the stellar evolution.
Results. We have found that around 50% of stars in the simulated open clusters involved in the formation of mergers are B-type stars. As a result, more than 50% of the merger products end up as a B-type star as well. Also, between 12.54% and 23.24% of all B-type stars are mergers. These results are a natural consequence of the initial mass function, initial distribution of the binary star parameters, and large range of masses for B-type stars. A non-negligible fraction of mergers occurred before entering the common envelope phase and we detected merger events at extragalactic distances. The total amount of detected mergers could have an impact on the chemical evolution of galaxies. The resulting mass distribution of merger products shows a peak for A-type stars, which is in agreement with observed massive Ap stars. Post-mergers among late B-type FS CMa stars could be the progenitors of very massive magnetic Ap stars. our results could also help to explain the nature of some magnetic white dwarfs. We present a comparison of the W component and the space velocity of the simulated mergers with a sample of observed FS CMa stars.

Abstract Copyright: © The Authors 2024

Journal keyword(s): stars: chemically peculiar - stars: emission-line, Be - stars: evolution - stars: magnetic field - galaxies: clusters: general

Simbad objects: 34

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Number of rows : 34
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 PB 5937 CV* 00 24 52.5551076576 -01 53 35.436920100   15.334 15.240 15.141   ~ 16 1
2 HD 281192 Em* 03 45 14.7163837704 +29 45 03.178318824   9.974 9.80     B8:e 29 0
3 V* MO Cam Be* 03 58 59.4438030480 +56 11 12.624758052 13.618 11.97 11.26     Be 40 0
4 V* CI Cam HXB 04 19 42.1355996520 +55 59 57.706599192 12.13 12.41 11.77 10.79 9.99 B0/2I[e] 271 0
5 EM* MWC 485 Y*O 05 14 26.9228765712 +32 48 03.269287044   12.700 12.245 12.183   Be 14 0
6 BD-10 1351 Ae* 06 02 14.8852964880 -10 00 59.515555464   10.54 10.40     B3V[e] 41 0
7 EM* AS 119 TT* 06 09 25.5040515456 -09 38 49.182807588   13.28 12.36     B3IV[e] 28 1
8 IRAS 06071+2925 Ae? 06 10 17.3285419104 +29 25 16.605726312   14.58 13.73     B9 19 0
9 EM* MWC 137 Ae* 06 18 45.5220873216 +15 16 52.244494608 12.89 13.30 13.759 11.67 10.31 sgB[e]d 259 1
10 HD 45677 Be* 06 28 17.4219710352 -13 03 11.128860972 7.86 8.52 8.50 8.11 8.01 B2IV/V[e] 343 0
11 HD 50138 Ae* 06 51 33.3989823840 -06 57 59.450772852 6.28 6.68 6.67     A1Ib/II 236 0
12 HD 51585 pA? 06 58 30.4066932552 +16 19 26.138751492   11.48 11.20     B:eI/BQ[] 82 0
13 [KW97] 34-26 Em* 07 10 43.8683682264 +06 00 07.935249600   12.212 12.077 12.109   A0-A1II 13 0
14 CD-24 5721 Em* 07 39 06.1599984144 -24 45 04.948772328 10.84 11.42 10.94 10.79   B[e] 40 0
15 SS 147 Em* 07 39 48.0497382096 -25 30 28.202718456   13.268 12.902 13.118   B8III/Ve 9 0
16 * l Pup sg* 07 43 48.4696146486 -28 57 17.374357218 4.06 4.09 3.93 3.68 3.50 A4Iabe 201 0
17 CD-49 3441 Be* 08 14 20.4677690448 -50 09 46.380031992   10.36 10.34     B8e 24 0
18 HD 85567 Be* 09 50 28.5375988920 -60 58 02.954048268 8.16 8.67 8.57     B5Vne 105 0
19 CD-48 7859 Be* 13 01 17.8030714320 -48 53 18.799911852   10.65 10.58     B5e 61 0
20 EM* AS 222 Be* 17 14 18.0009782328 -38 58 59.642143140   13.99 12.44 11.84   Be 19 0
21 EM* AS 225 Be* 17 20 55.5371447304 -38 00 00.366018840   14.82 13.44 12.99   Be 16 0
22 BD+23 3183 Em* 17 47 03.2744329776 +23 19 45.354097632   10.257 10.191 10.117   A1-A2II/III 28 0
23 V* V1309 Sco CV* 17 57 32.9368332984 -30 43 09.965039880           ~ 320 0
24 EM* LkHA 348 Be* 18 34 12.6529075104 -00 26 21.795198000   15.978 14.323 13.698   Be 42 0
25 EM* MWC 939 pA* 18 34 16.2191401512 -17 36 13.989813120     12.4     Be 39 0
26 EM* AS 319 Be* 18 43 15.9609528336 -05 05 37.245784956       14.277   Be 16 0
27 EM* MWC 623 ** 19 56 31.5417133728 +31 06 20.124534348   11.98 10.92     K2Ib/II+B4III[e] 81 0
28 EM* MWC 342 LP? 20 23 03.6172964112 +39 29 49.920095616 11.62 11.5 10.6     B[e] 91 1
29 EM* AS 446 Em* 20 50 55.8626784000 +49 00 37.395748368   11.38 10.32     A0II 14 0
30 EM* GGR 8 Y*O 21 11 19.0666935096 +47 38 47.598624096   13.054 12.447 12.365   A 13 0
31 EM* GGR 25 Em* 21 28 05.4063995328 +49 41 00.184256052   13.38 12.60 12.56   ~ 7 0
32 EM* MWC 645 Be* 21 53 27.4866658080 +52 59 58.019076852   13.72 13.00 12.98   B[e] 52 0
33 EM* MWC 1055 Em* 22 08 25.4277987048 +54 13 26.164151040   12.51 12.10     Be 32 0
34 EM* GGR 71 Be* 22 26 38.7333592272 +61 13 31.568432916   13.254 12.411 12.140   B[e] 36 0

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