2019A&A...630A..54B


Query : 2019A&A...630A..54B

2019A&A...630A..54B - Astronomy and Astrophysics, volume 630A54-54 (2019/10-1)

ALMA resolves the hourglass magnetic field in G31.41+0.31.

BELTRAN M.T., PADOVANI M., GIRART J.M., GALLI D., CESARONI R., PALADINO R., ANGLADA G., ESTALELLA R., OSORIO M., RAO R., SANCHEZ-MONGE A. and ZHANG Q.

Abstract (from CDS):


Context. Submillimeter Array (SMA) 870µm polarization observations of the hot molecular core G31.41+0.31 revealed one of the clearest examples up to date of an hourglass-shaped magnetic field morphology in a high-mass star-forming region.
Aims. To better establish the role that the magnetic field plays in the collapse of G31.41+0.31, we carried out Atacama Large Millimeter/ submillimeter Array (ALMA) observations of the polarized dust continuum emission at 1.3mm with an angular resolution four times higher than that of the previous (sub)millimeter observations to achieve an unprecedented image of the magnetic field morphology.
Methods. We used ALMA to perform full polarization observations at 233GHz (Band 6). The resulting synthesized beam is 0.28"x0.20" which, at the distance of the source, corresponds to a spatial resolution of ∼875au.
Results. The observations resolve the structure of the magnetic field in G31.41+0.31 and allow us to study the field in detail. The polarized emission in the Main core of G31.41+0.41is successfully fit with a semi-analytical magnetostatic model of a toroid supported by magnetic fields. The best fit model suggests that the magnetic field is well represented by a poloidal field with a possible contribution of a toroidal component of ∼10% of the poloidal component, oriented southeast to northwest at approximately -44° and with an inclination of approximately -45°. The magnetic field is oriented perpendicular to the northeast to southwest velocity gradient detected in this core on scales from 103 to 104au. This supports the hypothesis that the velocity gradient is due to rotation of the core and suggests that such a rotation has little effect on the magnetic field. The strength of the magnetic field estimated in the central region of the core with the Davis-Chandrasekhar-Fermi method is ∼8-13mG and implies that the mass-to-flux ratio in this region is slightly supercritical.
Conclusions. The magnetic field in G31.41+0.31 maintains an hourglass-shaped morphology down to scales of <1000au. Despite the magnetic field being important in G31.41+0.31, it is not enough to prevent fragmentation and collapse of the core, as demonstrated by the presence of at least four sources embedded in the center of the core.

Abstract Copyright: © ESO 2019

Journal keyword(s): ISM: individual objects: G31.41+0.31 - ISM: magnetic fields - stars: formation - techniques: interferometric

VizieR on-line data: <Available at CDS (J/A+A/630/A54): list.dat fits/*>

Simbad objects: 10

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Number of rows : 10
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 [JCC87] IRAS 4A Y*O 03 29 10.49 +31 13 30.8           ~ 770 1
2 GBS-VLA J162626.39-242430.9 Y*O 16 26 26.39 -24 24 30.8           ~ 38 0
3 NAME Ophiuchus Molecular Cloud SFR 16 28 06 -24 32.5           ~ 3969 1
4 2MASS J17112317-2724315 Y*O 17 11 23.17752 -27 24 31.5288           ~ 91 0
5 4C 09.57 BLL 17 51 32.81857326 +09 39 00.7284066   17.46 16.78 15.57   ~ 1007 1
6 GCNM 23 Y*O 18 29 49.63 +01 15 21.9           ~ 291 2
7 IRAS 18449-0115 cor 18 47 34.27 -01 12 43.2           ~ 430 1
8 QSO J1851+005 QSO 18 51 46.72295 +00 35 32.3649           ~ 138 1
9 QSO B1921-293 BLL 19 24 51.05595254 -29 14 30.1210248   18.71 18.21 15.07   ~ 918 1
10 LDN 663 DNe 19 36 55 +07 34.4           ~ 698 0

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