2023A&A...679A.121H


Query : 2023A&A...679A.121H

2023A&A...679A.121H - Astronomy and Astrophysics, volume 679A121 (2023/11-1)

Velocity-resolved high-J CO emission from massive star-forming clumps.

HOANG T.D., KARSKA A., LEE M.Y., WYROWSKI F., TRAM L.N., YANG A. and MENTEN K.M.

Abstract (from CDS):

Context. Massive star formation is associated with energetic processes, which result in significant gas cooling via far-infrared (IR) lines. Velocity-resolved observations can constrain the kinematics of the gas, allowing the identification of the physical mechanisms responsible for gas heating.
Aims. Our aim is to quantify far-IR CO line emission towards high-mass star-forming regions, identify the high-velocity gas component associated with outflows, and estimate the physical conditions required for the excitation of the observed lines.
Methods. Velocity-resolved SOFIA/GREAT spectra of 13 high-mass star-forming clumps of various luminosities and evolutionary stages are studied in highly excited rotational lines of CO. For most targets, the spectra are from frequency intervals covering the CO 11-10 and 16-15 lines towards two sources, also the CO 13-12 line was observed with SOFIA/4GREAT. Angular resolutions at the line frequencies range from 14″ to 20″, corresponding to spatial scales of ∼0.1-0.8 pc. Radiative transfer models were used to determine the physical conditions giving rise to the emission in the line wings.
Results. All targets in our sample show strong high-J CO emission in the far-IR, characterised by broad line wings associated with outflows, thereby significantly increasing the sample of high-mass objects with velocity-resolved high-J CO spectra. Twelve sources show emission in the line wings of the CO 11-10 line (Eu/kB=365 K), and eight sources in the CO 16-15 line (Eu/kB =752 K). The contribution of the emission in the line wings to the total emission ranges from ∼28% to 76%, and does not correlate with the envelope mass or evolutionary stage. Gas excitation temperatures cover a narrow range of 120-220 K for the line wings, and 110-200 K for the velocity-integrated line emission, assuming local thermodynamics equilibrium (LTE). For the two additional sources with the CO 13-12 line (Eu/kB=503 K) data, wing emission rotational temperatures of ∼130 K and 165 K were obtained using Boltzmann diagrams. The corresponding non-LTE radiative transfer models indicate gas densities of 105-107 cm–3 and CO column densities of 1017-1018 cm–2 in the line wings, similar to physical conditions in deeply embedded low- and high-mass protostars. The velocity-integrated CO line fluxes correlate with the bolometric luminosity over 7 orders of magnitude, including data on the low-mass protostars from the literature. This suggests that similar processes are responsible for the high-J CO excitation over a significant range of physical scales.
Conclusions. Velocity-resolved line profiles allow the detection of outflows towards massive star-forming clumps spanning a broad range of evolutionary stages. The lack of clear evolutionary trends suggest that mass accretion and ejection prevail during the entire lifetime of star-forming clumps.

Abstract Copyright: © The Authors 2023

Journal keyword(s): stars: formation - stars: protostars - ISM: molecules - ISM: kinematics and dynamics - line: profiles - ISM: jets and outflows

Status at CDS : All or part of tables of objects could be ingested in SIMBAD with priority 2.

Simbad objects: 25

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Number of rows : 25
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 W3 IRS 5 Y*O 02 25 40.54 +62 05 51.4           B1 367 0
2 NAME Orion S reg 05 35 12.9 -05 24 10           ~ 156 0
3 NAME Orion-KL SFR 05 35 14.16 -05 22 21.5           ~ 2421 1
4 AGAL G351.161+00.697 cor 17 19 57 -35 57.8           ~ 22 0
5 AGAL G351.244+00.669 cor 17 20 17.84 -35 54 46.0           ~ 35 0
6 AGAL G351.444+00.659 cor 17 20 54.60 -35 45 12.8           ~ 35 0
7 MMB G351.581-00.353 cor 17 25 25.220 -36 12 45.34           ~ 44 0
8 AGAL G351.774-00.537 cor 17 26 43 -36 09.3           ~ 43 0
9 NAME Sgr B MoC 17 47 02 -28 25.4           ~ 241 0
10 NAME Sgr B2 Main Rad 17 47 20.5 -28 23 06           ~ 436 1
11 AGAL G012.804-00.199 cor 18 14 13.34 -17 55 45.3           ~ 49 0
12 AGAL G014.194-00.194 Y*O 18 16 59 -16 42.2           ~ 40 0
13 MMB G013.657-00.599 cor 18 17 24.26 -17 22 12.5           ~ 30 0
14 MMB G014.631-00.577 cor 18 19 15.21 -16 30 04.5           ~ 27 0
15 NAME M 17 SW SFR 18 20 23.1 -16 11 43           ~ 281 0
16 AGAL G034.411+00.234 Y*O 18 53 18.0319 +01 25 25.500           ~ 108 0
17 AGAL G034.401+00.226 cor 18 53 18.6 +01 24 40           ~ 74 1
18 [CUS2014] G034.2572+0.1535 cor 18 53 18.6449 +01 15 01.574           ~ 43 0
19 AGAL G035.197-00.742 cor 18 58 12.816 +01 40 36.62           ~ 23 0
20 W 49n HII 19 10 13.2 +09 06 12           ~ 497 3
21 RAFGL 2591 Y*O 20 29 24.8230 +40 11 19.590           ~ 640 0
22 DR 21 (OH) cor 20 39 01.01 +42 22 50.2           ~ 427 0
23 NAME Cepheus A SFR 22 56 17.9 +62 01 49           ~ 760 2
24 NAME Cep E HII 23 03 12.779 +61 42 25.75           ~ 183 0
25 [WBN74] NGC 7538 IRS 1 Y*O 23 13 45.318 +61 28 11.69           ~ 433 3

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