2024ApJ...972L...6S


Query : 2024ApJ...972L...6S

2024ApJ...972L...6S - Astrophys. J., 972, L6 (2024/September-1)

Magnetic Fields in Massive Star-forming Regions (MagMaR): Unveiling an Hourglass Magnetic Field in G333.46-0.16 Using ALMA.

SAHA P., SANHUEZA P., PADOVANI M., GIRART J.M., CORTES P.C., MORII K., LIU J., SANCHEZ-MONGE A., GALLI D., BASU S., KOCH P.M., BELTRAN M.T., LI S., BEUTHER H., STEPHENS I.W., NAKAMURA F., ZHANG Q., JIAO W., FERNANDEZ-LOPEZ M., HWANG J., CHUNG E.J., PATTLE K., ZAPATA L.A., XU F., OLGUIN F.A., KANG J.-H., KAROLY J., LAW C.-Y., WANG J.-W., CSENGERI T., LU X., CHENG Y., KIM J., CHOUDHURY S., CHEN H.-R.V. and HULL C.L.H.

Abstract (from CDS):

The contribution of the magnetic field to the formation of high-mass stars is poorly understood. We report the high angular resolution (∼0.″3, 870 au) map of the magnetic field projected on the plane of the sky (BPOS) toward the high-mass star-forming region G333.46-0.16 (G333), obtained with the Atacama Large Millimeter/submillimeter Array at 1.2 mm as part of the Magnetic fields in Massive star-forming Regions survey. The BPOS morphology found in this region is consistent with a canonical “hourglass” with an embedded flattened envelope in a perpendicular direction, which suggests a dynamically important field. This region is fragmented into two protostars that appear to be gravitationally bound in a stable binary system with a separation of ∼1740 au. Interestingly, by analyzing H13CO+ (J = 3-2) line emission, we find no velocity gradient over the extent of the continuum, which is consistent with a strong field. We model the BPOS, obtaining a marginally supercritical mass-to-flux ratio of 1.43, suggesting an initially strongly magnetized environment. Based on the Davis-Chandrasekhar-Fermi method, the magnetic field strength toward G333 is estimated to be 5.7 mG. The absence of strong rotation and outflows toward the central region of G333 suggests strong magnetic braking, consistent with a highly magnetized environment. Our study shows that despite being a strong regulator, the magnetic energy fails to prevent the process of fragmentation, as revealed by the formation of the two protostars in the central region.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Dust continuum emission - Magnetic fields - Polarimetry - Star formation

Nomenclature: Fig. 1, Table 1: [SSP2024] G333.46-0.16 MMN (Nos MM1-MM2).

Simbad objects: 9

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Number of rows : 9
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 QSO B1424-41 Bla 14 27 56.29756617 -42 06 19.4376238   18.48 17.7 16.30   ~ 547 1
2 AGAL G333.466-00.164 cor 16 21 20.170 -50 09 47.77           ~ 27 0
3 [SSP2024] G333.46-0.16 MM2 Y*O 16 21 20.170 -50 09 46.41           ~ 1 0
4 [SSP2024] G333.46-0.16 MM1 Y*O 16 21 20.200 -50 09 46.91           ~ 1 0
5 ICRF J165016.6-504448 QSO 16 50 16.62710806 -50 44 48.2106956   20.95       ~ 89 2
6 NAME NGC 6334-I Cl* 17 20 53.35 -35 47 01.5           ~ 373 0
7 NAME NGC 6334 I(N) smm 17 20 54 -35 45.0           ~ 165 1
8 RAFGL 2046 HII 18 00 32.1 -24 04 03           ~ 380 0
9 GAL 012.89+00.49 HII 18 11 51.3 -17 31 29           ~ 217 0

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