2024A&A...690A.297K


Query : 2024A&A...690A.297K

2024A&A...690A.297K - Astronomy and Astrophysics, volume 690A297 (2024/10-1)

Constraints on the primordial misalignment of star-disk systems.

KUFFMEIER M., PINEDA J.E., SEGURA-COX D. and HAUGBOLLE T.

Abstract (from CDS):

A consensus prevails with regard to star-disk systems accreting most of their mass and angular momentum during the collapse of a prestellar core. However, recent results have indicated that stars experience post-collapse or late infall, during which the star and its disk are refreshed with material from the protostellar environment through accretion streamers. Apart from adding mass to the star-disk system, infall potentially supplies a substantial amount of angular momentum, as the infalling material is initially not bound to the collapsing prestellar core. We investigate the orientation of infall on star-disk systems by analyzing the properties of accreting tracer particles in three-dimensional magnetohydrodynamical (3D MHD) simulations of a molecular cloud that is (4 pc)3 in volume. In contrast to the traditional picture, where the rotational axis is inherited from the collapse of a coherent pre-stellar core, the orientation of star-disk systems changes substantially throughout the accretion process, thereby extending the possibility of primordial misalignment as the source of large obliquities. In agreement with previous results that show larger contributions of late infall for increasing stellar masses, a misaligned infall is more likely to lead to a prolonged change in orientation for stars of higher final mass. On average, brown dwarfs and very low mass stars are more likely to form and accrete all of their mass as part of a multiple system, while stars with final masses above a few 0.1 M⊙ are more likely to accrete part of their mass as single stars. Finally, we find an overall trend among our sample: the post-collapse accretion phase is more anisotropic than the early collapse phase. This result is consistent with a scenario of Bondi-Hoyle-Littletlon accretion during the post-collapse phase, while the initial collapse is less anisotropic - despite the fact that material is funneled through accretion channels.

Abstract Copyright: © The Authors 2024

Journal keyword(s): protoplanetary disks - binaries: general - circumstellar matter - stars: formation - stars: low-mass - stars: protostars

Simbad objects: 28

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Number of rows : 28
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 LDN 1455 IRS 1 cor 03 27 39.08 +30 13 03.1           ~ 173 0
2 NGC 1333 OpC 03 29 09.2 +31 20 59           ~ 1575 1
3 LDN 1471 DNe 03 48.0 +32 54           ~ 349 0
4 V* HL Tau Or* 04 31 38.5107609312 +18 13 57.859747968   15.89 14.49 14.39   K5 1546 0
5 V* GG Tau Or* 04 32 30.3506925552 +17 31 40.494063144 14.84 14.78 13.40 11.54   M0e+M2.0e 793 1
6 EM* LkCa 15 Or* 04 39 17.7911622816 +22 21 03.390090984   13.01 12.03 11.61   K5:Ve 792 1
7 V* DR Tau Or* 04 47 06.2151561264 +16 58 42.813872580 12.03 11.86 10.50 12.19   K5Ve 585 0
8 V* GM Aur Or* 04 55 10.9815576936 +30 21 59.373771876 14.59 13.351 12.242 11.798   K3Ve 797 0
9 V* AB Aur Ae* 04 55 45.8458932216 +30 33 04.292077032 7.20 7.16 7.05 6.96 6.70 A0Ve 1176 2
10 V* SU Aur Or* 04 55 59.3866872552 +30 34 01.499608092   10.33 9.30 9.17   G2IIIne 628 0
11 HD 34700 Or* 05 19 41.4089390784 +05 38 42.778590864 9.75 9.778 9.659 9.205 8.47 G0IVe 125 0
12 V* GW Ori TT* 05 29 08.3928710640 +11 52 12.666457092   10.83 10.10 9.52   G5/8Ve 382 0
13 HD 36112 Ae* 05 30 27.5285630040 +25 19 57.076288752   8.57 8.27     A8Ve 551 0
14 IRAS 05377-0733 Or* 05 40 13.7887528608 -07 32 16.020172500     21.389   16.242 M7.5 37 0
15 HD 100453 Ae* 11 33 05.5766482920 -54 19 28.547100696   8.09 7.79     F1Vn 335 1
16 V* DK Cha TT* 12 53 17.2111480272 -77 07 10.736046012           F0e 149 0
17 HD 135344B Or* 15 15 48.4460065200 -37 09 16.024369824   9.21 8.708     F8V 548 0
18 HD 139614 Or* 15 40 46.3820275416 -42 29 53.538761832   8.47 8.24     A9VekA5mA5(_lB) 243 0
19 HD 142527 Ae* 15 56 41.8882637904 -42 19 23.248281828   9.04 8.34     F6III 741 1
20 V* RU Lup TT* 15 56 42.3108692112 -37 49 15.473946900 9.27 10.07 9.60     K7/M0e 528 0
21 HD 143006 Or* 15 58 36.9126279888 -22 57 15.220559196   10.92 10.14   8.70 G5IVe 338 0
22 RX J1604.3-2130 X 16 04.3 -21 30           ~ 41 0
23 IRAS 16253-2429 FIR 16 28 22.2 -24 36 31           ~ 66 0
24 Haro 1-16 Or* 16 31 33.4634997336 -24 27 37.158728076   14.02 12.80     K3e 266 0
25 IRAS 16544-1604 Y*O 16 57 19.626 -16 09 23.30           ~ 53 1
26 2MASS J17110392-2722551 Or* 17 11 03.9294631032 -27 22 55.199684244           ~ 24 0
27 [FCG2011] MM1 cor 18 19 12.114 -20 47 30.61           ~ 31 0
28 V* S CrA Or* 19 01 08.597088 -36 57 19.89504   11.76 10.91 11.41   G0Ve+K0Ve 286 0

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