2023A&A...677A.171A


Query : 2023A&A...677A.171A

2023A&A...677A.171A - Astronomy and Astrophysics, volume 677A171 (2023/9-1)

Kinematics and stability of high-mass protostellar disk candidates at sub-arcsecond resolution Insights from the IRAM NOEMA large programme CORE.

AHMADI A., BEUTHER H., BOSCO F., GIESER C., SURI S., MOTTRAM J.C., KUIPER R., HENNING T., SANCHEZ-MONGE A., LINZ H., PUDRITZ R.E., SEMENOV D., WINTERS J.M., MOLLER T., BELTRAN M.T., CSENGERI T., GALVAN-MADRID R., JOHNSTON K.G., KETO E., KLAASSEN P.D., LEURINI S., LONGMORE S.N., LUMSDEN S.L., MAUD L.T., MOSCADELLI L., PALAU A., PETERS T., RAGAN S.E., URQUHART J.S., ZHANG Q. and ZINNECKER H.

Abstract (from CDS):

Context. The fragmentation mode of high-mass molecular clumps and the accretion processes that form the most massive stars (M ≳ 8 M⊙) are still not well understood. A growing number of case studies have found massive young stellar objects (MYSOs) to harbour disk-like structures, painting a picture that the formation of high-mass stars may proceed through disk accretion, similar to that of lower-mass stars. However, the properties of such structures have yet to be uniformly and systematically characterised.
Aims. The aim of this work is to uniformly study the kinematic properties of a large sample of MYSOs and characterise the stability of possible circumstellar disks against gravitational fragmentation.
Methods. We have undertaken a large observational programme (CORE) making use of interferometric observations from the Northern Extended Millimetre Array (NOEMA) for a sample of 20 luminous (L > 104L⊙) protostellar objects in the 1.37 mm wavelength regime in both continuum and spectral line emission, reaching 0.4″ resolution (800 au at 2 kpc).
Results. We present the gas kinematics of the full sample and detect dense gas emission surrounding 15 regions within the CORE sample. Using the dense gas tracer CH3CN, we find velocity gradients across 13 cores perpendicular to the directions of bipolar molecular outflows, making them excellent disk candidates. The extent of the CH3CN emission tracing the disk candidates varies from 1800 to 8500 au. Analysing the free-fall to rotational timescales, we find that the sources are rotationally supported. The rotation profiles of some disk candidates are well described by differential rotation while for others the profiles are poorly resolved. Fitting the velocity profiles with a Keplerian model, we find protostellar masses in the range of ∼ 10-25 M⊙. Modelling the level population of CH3CN (12K-11K) K = 0-6 lines, we present temperature maps and find median temperature in the range 70-210 K with a diversity in distributions. Radial profiles of the specific angular momentum (j) for the best disk candidates span a range of 1-2 orders of magnitude, on average ∼10–3 km s–1 pc, and they follow j ∝ r1.7, which is consistent with a poorly resolved rotating and infalling envelope-disk model. Studying the Toomre stability of the disk candidates, we find almost all (11 out of 13) disk candidates to be prone to fragmentation due to gravitational instabilities at the scales probed by our observations, as a result of their high disk to stellar mass ratio. In particular, disks with masses greater than ∼ 10-20% of the mass of their host (proto)stars are Toomre unstable, and more luminous YSOs tend to have disks that are more massive compared to their host star and hence more prone to fragmentation.
Conclusions. In this work, we show that most disk structures around high-mass YSOs are prone to disk fragmentation early in their formation due to their high disk to stellar mass ratio. This impacts the accretion evolution of high-mass protostars which will have significant implications for the formation of the most massive stars.

Abstract Copyright: © The Authors 2023

Journal keyword(s): stars: formation - stars: massive - stars: kinematics and dynamics - techniques: interferometric

Simbad objects: 30

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Number of rows : 30
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 NGC 753 GiG 01 57 42.2040241440 +35 54 57.729210264   12.6   11.59   ~ 207 1
2 MPCM J022530.99+620620.9 HII 02 25 31.18 +62 06 24.5           O8V-B0.5V 107 1
3 NAME W 3 OH HII 02 27 04.1 +61 52 22           ~ 1064 2
4 W 3(H2O) Mas 02 27 04.6 +61 52 25           ~ 154 0
5 MSX6C G138.2957+01.5552 Y*O 03 01 31.253 +60 29 13.07           ~ 25 0
6 MSX6C G139.9091+00.1969 Y*O 03 07 24.0 +58 30 49           ~ 10 0
7 NGC 1275 Bla 03 19 48.1599902040 +41 30 42.108850836   13.10 12.48 11.09   ~ 4243 3
8 NAME SH 2-255 IRS 3 Y*O 06 12 55.03 +17 59 29.9           ~ 25 0
9 3C 273 BLL 12 29 06.6998257176 +02 03 08.597629980   13.05 14.830 14.11   ~ 6022 1
10 NAME SH 2-87 IRS 1 HII 19 46 20.130 +24 35 29.43           ~ 17 0
11 GAL 075.78+00.34 cor 20 21 44.00 +37 26 38.0           ~ 131 1
12 2MASS J20272677+3722477 Y*O 20 27 26.7731405016 +37 22 47.849902500           B0V 5 0
13 RAFGL 2591 Y*O 20 29 24.8230 +40 11 19.590           ~ 640 0
14 NAME Cyg X Cld 20 30 04.7973633 +40 51 36.002197           ~ 962 1
15 EM* MWC 349 ** 20 32 45.499080 +40 39 36.74124   15.88 13.15 12.13   Bep 837 0
16 2MASS J20553247+4406101 Y*O 20 55 32.47752 +44 06 10.1016           ~ 10 0
17 IRAS 21078+5211 HII 21 09 31.03 +52 24 16.1           ~ 65 0
18 V* V645 Cyg Ae* 21 39 58.2745507632 +50 14 21.042184668   14.23 13.10 13.82   O6/9eq 279 0
19 MSX6C G100.3779-03.5784 Y*O 22 16 10.3651 +52 21 34.113           ~ 18 0
20 3C 454.3 Bla 22 53 57.7480438728 +16 08 53.561508864   16.57 16.10 15.22   ~ 3004 2
21 NAME Cep A HW 2 Y*O 22 56 17.9 +62 01 49           B0.5 243 0
22 NAME Cepheus A SFR 22 56 17.9 +62 01 49           ~ 760 2
23 IRAS 22566+5828 Y*O 22 58 47.25 +58 45 01.6           ~ 25 0
24 [RM2008] IRAS 23033+5951-MMS1 mm 23 05 25.0 +60 08 17           ~ 3 0
25 IRAS 23033+5951 Y*O 23 05 25.1762883456 +60 08 15.374293800           ~ 97 0
26 NGC 7538S Y*O 23 13 44.8 +61 26 51           ~ 91 1
27 [WBN74] NGC 7538 IRS 1 Y*O 23 13 45.318 +61 28 11.69           ~ 433 3
28 IRAS 23118+6110 Y*O 23 14 02.09473 +61 27 18.8460           ~ 385 0
29 IRAS 23151+5912 HII 23 17 21.0 +59 28 49           ~ 102 0
30 Mol 160 Rad 23 40 54.5 +61 10 28           ~ 121 0

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