2021ApJ...913...57K


Query : 2021ApJ...913...57K

2021ApJ...913...57K - Astrophys. J., 913, 57-57 (2021/May-3)

The JCMT BISTRO-2 survey: the magnetic field in the center of the Rosette Molecular Cloud.

KONYVES V., WARD-THOMPSON D., PATTLE K., DI FRANCESCO J., ARZOUMANIAN D., CHEN Z., DIEP P.N., ESWARAIAH C., FANCIULLO L., FURUYA R.S., HOANG T., HULL C.L.H., HWANG J., JOHNSTONE D., KANG J.-H., KAROLY J., KIRCHSCHLAGER F., KIRK J.M., KOCH P.M., KWON J., LEE C.W., ONAKA T., ROBITAILLE J.-F., SOAM A., TAHANI M., TANG X., TAMURA M., BERRY D., BASTIEN P., CHING T.-C., COUDE S., KWON W., WANG J.-W., HASEGAWA T., LAI S.-P. and QIU K.

Abstract (from CDS):

We present the first 850 µm polarization observations in the most active star-forming site of the Rosette Molecular Cloud (d ∼ 1.6 kpc) in the wall of the Rosette Nebula, imaged with the SCUBA-2/POL-2 instruments of the James Clerk Maxwell telescope, as part of the B-Fields In Star-forming Region Observations 2 (BISTRO-2) survey. From the POL-2 data we find that the polarization fraction decreases with the 850 µm continuum intensity with α = 0.49 ± 0.08 in the p ∝ I–α relation, which suggests that some fraction of the dust grains remain aligned at high densities. The north of our 850 µm image reveals a "gemstone ring" morphology, which is a ∼1 pc diameter ring-like structure with extended emission in the "head" to the southwest. We hypothesize that it might have been blown by feedback in its interior, while the B-field is parallel to its circumference in most places. In the south of our SCUBA-2 field the clumps are apparently connected with filaments that follow infrared dark clouds. Here, the POL-2 magnetic field orientations appear bimodal with respect to the large-scale Planck field. The mass of our effective mapped area is ∼174 M☉, which we calculate from 850 µm flux densities. We compare our results with masses from large-scale emission-subtracted Herschel 250 µm data and find agreement within 30%. We estimate the plane-of-sky B-field strength in one typical subregion using the Davis-Chandrasekhar-Fermi technique and find 80 ± 30 µG toward a clump and its outskirts. The estimated mass-to-flux ratio of λ = 2.3 ± 1.0 suggests that the B-field is not sufficiently strong to prevent gravitational collapse in this subregion.

Abstract Copyright: © 2021. The American Astronomical Society. All rights reserved.

Journal keyword(s): Interstellar magnetic fields - Polarimetry - Submillimeter astronomy - Interstellar dust processes - Star-forming regions

Simbad objects: 18

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Number of rows : 18
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 Ori B MoC 05 41 43.0 -01 54 44           ~ 1498 0
2 NAME Rosette OB Association As* 06 31.7 +04 58           ~ 148 0
3 NGC 2244 OpC 06 32 06.9 +04 54 19           ~ 673 1
4 NAME Rosette Nebula HII 06 32 26.76 +04 47 37.1           ~ 522 1
5 [YP2004] RMC-L PoC 06 33 48.5 +04 26 18           ~ 2 0
6 HD 46485 Y*O 06 33 50.9566745256 +04 31 31.613196504 7.92 8.60 8.27   8.10 O7V((f))nzvar? 162 0
7 IRAS 06314+0427 IR 06 34 04.92 +04 25 00.1           ~ 25 1
8 [PL97] 4a Cl* 06 34.1 +04 25           ~ 2 0
9 [YP2004] RMC-M PoC 06 34 10.1 +04 22 33           ~ 2 0
10 [PL97] 4b Cl* 06 34.2 +04 28           ~ 3 0
11 [PRG2008] E Cl* 06 34 14.237 +04 22 46.42           ~ 6 1
12 REFL 08 Cl* 06 34.2 +04 19           ~ 13 0
13 [PL97] 5 Cl* 06 34 32 +04 18.5           ~ 19 1
14 NAME Rosette Molecular Cloud MoC 06 34.7 +04 02           ~ 277 0
15 REFL 09 Cl* 06 35 02.791 +03 43 00.62           ~ 11 0
16 LDN 1689B DNe 16 34 42.1 -24 36 11           ~ 181 0
17 [ABB2014] WISE G011.893+00.748 bub 18 08 52.6 -18 16 07           ~ 32 0
18 MSXDC G034.43+00.24 MoC 18 53 18.9 +01 26 39           ~ 122 0

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