2023MNRAS.523.5554M


Query : 2023MNRAS.523.5554M

2023MNRAS.523.5554M - Mon. Not. R. Astron. Soc., 523, 5554-5564 (2023/August-3)

2.5D magnetohydrodynamic models of circumstellar discs around FS CMa post-mergers - I. Non-stationary accretion stage.

MORANCHEL-BASURTO A., KORCAKOVA D. and CHAMETLA R.O.

Abstract (from CDS):

We investigate the dynamic evolution of the gaseous regions around FS CMa post-mergers. Owing to the slow rotation of the central B-type star, the dynamics is driven mainly by the magnetic field of the central star. Recent observations have allowed us to set realistic initial conditions, such as the magnetic field value ($B_\star \approx 6\times 10^{3}\, \mathrm{G}$), the mass of the central star ($M_\star =6\, \mathrm{M}_\odot$), and the initial disc density $\rho _{d0}\in [10^{-13}\, \mathrm{g\, cm^{-3}},10^{-11}\, \mathrm{g \, cm^{-3}}]$. We use the PLUTO code to perform 2.5D magnetohydrodynamic simulations of thin and thick disc models. Especially relevant for the interpretation of the observed properties of FS CMa post-mergers are the results for low-density discs, in which we find a jet emerging from the inner edge of the disc, as well as the formation of the so-called 'hot plasmoid' in the coronal region. Jets are probably detected as discrete absorption components in the resonance lines of FS CMa stars. Moreover, the magnetic field configuration in the low-density plasma region favours the appearance of magnetocentrifugal winds from the disc. The currents towards the star created by the magnetic field may explain accidentally observed material infall. The disc structure is significantly changed owing to the presence of the magnetic field. The magnetic field is also responsible for the formation of a hot corona, as observed in several FS CMa stars through the Raman lines. Our results are valid for all magnetic stars surrounded by a low-density plasma, that is, by some stars showing the B[e] phenomenon.

Abstract Copyright: © 2023 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): accetion, accretion discs - MHD - methods: numerical - stars: magnetic field

Simbad objects: 29

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Number of rows : 29
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 EM* GGA 2 LP* 00 50 05.9718580056 +64 45 35.046643752   12.406 11.545     Beq 28 0
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 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
6 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
7 HD 50138 Ae* 06 51 33.3989823840 -06 57 59.450772852 6.28 6.68 6.67     A1Ib/II 236 0
8 [KW97] 34-26 Em* 07 10 43.8683682264 +06 00 07.935249600   12.212 12.077 12.109   A0-A1II 13 0
9 CD-24 5721 Em* 07 39 06.1599984144 -24 45 04.948772328 10.84 11.42 10.94 10.79   B[e] 40 0
10 * l Pup sg* 07 43 48.4696146486 -28 57 17.374357218 4.06 4.09 3.93 3.68 3.50 A4Iabe 201 0
11 CD-49 3441 Be* 08 14 20.4677690448 -50 09 46.380031992   10.36 10.34     B8e 24 0
12 WRAY 15-406 s?b 09 36 44.2100146392 -53 28 01.350852996   14.606 12.627 11.880   B[e] 17 0
13 HD 85567 Be* 09 50 28.5375988920 -60 58 02.954048268 8.16 8.67 8.57     B5Vne 105 0
14 HD 87643 Or* 10 04 30.2839505304 -58 39 52.091224848 8.92 10.38 9.50 9.68   B3I[e] 157 0
15 HD 94878 ** 10 55 58.9149262296 -60 23 33.436864428 8.67 9.37 8.70 8.07   B0/2eq 159 0
16 CD-48 7859 Be* 13 01 17.8030714320 -48 53 18.799911852   10.65 10.58     B5e 61 0
17 Hen 3-938 s*b 13 52 42.8520468288 -63 32 49.169086332 15.33 14.782 13.404 13.557   B0-B1I 33 0
18 CPD-52 9243 AB* 16 07 02.0298241344 -53 03 45.415519128 12.36 11.84 10.22 9.87   B3Ieq 62 0
19 HD 327083 s*b 17 15 15.3711774600 -40 20 06.792259560 12.07 11.44 10.00 9.64   B6Ieq 63 0
20 CD-38 11837 Ae* 17 24 44.7035716704 -38 43 51.463262568 11.05 11.37 10.62 10.46   B1Ve 48 2
21 BD+23 3183 Em* 17 47 03.2744329776 +23 19 45.354097632   10.257 10.191 10.117   A1-A2II/III 28 0
22 EM* MWC 300 Ae* 18 29 25.6913480400 -06 04 37.290320796 12.55 12.67 13.795     B1Ia+[e] 145 0
23 EM* MWC 939 pA* 18 34 16.2191401512 -17 36 13.989813120     12.4     Be 39 0
24 EM* MWC 623 ** 19 56 31.5417133728 +31 06 20.124534348   11.98 10.92     K2Ib/II+B4III[e] 81 0
25 EM* AS 386 SB* 20 10 54.2004527784 +38 18 09.361842084   11.62 10.95     OB 35 0
26 EM* MWC 342 LP? 20 23 03.6172964112 +39 29 49.920095616 11.62 11.5 10.6     B[e] 91 1
27 EM* MWC 349A Or* 20 32 45.5291969760 +40 39 36.651807828           ~ 180 0
28 EM* GGR 71 Be* 22 26 38.7333592272 +61 13 31.568432916   13.254 12.411 12.140   B[e] 36 0
29 EM* MWC 657 Be* 22 42 41.8293417264 +60 24 00.649510452   14.064 12.706 12.043   Be 40 0

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