2017ApJ...850..195E


Query : 2017ApJ...850..195E

2017ApJ...850..195E - Astrophys. J., 850, 195-195 (2017/December-1)

Understanding the links among the magnetic fields, filament, bipolar bubble, and star formation in RCW 57A using NIR polarimetry.

ESWARAIAH C., LAI S.-P., CHEN W.-P., PANDEY A.K., TAMURA M., MAHESWAR G., SHARMA S., WANG J.-W., NISHIYAMA S., NAKAJIMA Y., KWON J., PURCELL R. and MAGALHAES A.M.

Abstract (from CDS):

The influence of magnetic fields (B-fields) on the formation and evolution of bipolar bubbles, due to the expanding ionization fronts (I-fronts) driven by the H II regions that are formed and embedded in filamentary molecular clouds, has not been well-studied yet. In addition to the anisotropic expansion of I-fronts into a filament, B-fields are expected to introduce an additional anisotropic pressure, which might favor the expansion and propagation of I-fronts forming a bipolar bubble. We present results based on near-infrared polarimetric observations toward the central ∼8' x 8' area of the star-forming region RCW 57A, which hosts an H II region, a filament, and a bipolar bubble. Polarization measurements of 178 reddened background stars, out of the 919 detected sources in the JHKs bands, reveal B-fields that thread perpendicularly to the filament long axis. The B-fields exhibit an hourglass morphology that closely follows the structure of the bipolar bubble. The mean B-field strength, estimated using the Chandrasekhar-Fermi method (CF method), is 91 ± 8 µG. B-field pressure dominates over turbulent and thermal pressures. Thermal pressure might act in the same orientation as the B-fields to accelerate the expansion of those I-fronts. The observed morphological correspondence among the B-fields, filament, and bipolar bubble demonstrate that the B-fields are important to the cloud contraction that formed the filament, to the gravitational collapse and star formation in it, and in feedback processes. The last one includes the formation and evolution of mid-infrared bubbles by means of B-field supported propagation and expansion of I-fronts. These may shed light on preexisting conditions favoring the formation of the massive stellar cluster in RCW 57A.

Abstract Copyright: © 2017. The American Astronomical Society.

Journal keyword(s): dust, extinction - ISM: magnetic fields - open clusters and associations: individual: RCW 57A - polarization - polarization

VizieR on-line data: <Available at CDS (J/ApJ/850/195): table1.dat>

Nomenclature: Table 1: [ELC2017] NNNN (Nos 1-1074).

Status at CDS : All or part of tables of objects will not be ingested in SIMBAD.

Simbad objects: 23

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Number of rows : 23
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 SH 2-201 HII 03 03 17.9 +60 27 52           ~ 116 0
2 Barnard 211 DNe 04 17 35 +27 43.1           ~ 127 0
3 Barnard 213 DNe 04 20 51 +27 16.3           ~ 217 0
4 NGC 2024 Cl* 05 41 43 -01 50.5           ~ 1154 1
5 NGC 2100 Cl* 05 42 07.200 -69 12 26.99   9.6       ~ 189 0
6 NAME Orion Molecular Cloud MoC 05 56 -01.8           ~ 1098 1
7 NAME IRAS Vela Shell IR 07 44 -42.4           ~ 40 0
8 NAME Vela-D Molecular Cloud MoC 08 39 -41.0           ~ 49 0
9 RCW 36 HII 08 59 00.9 -43 44 10     15.20     ~ 147 0
10 [AMG2008] S5-M8 Mas 11 11 34.660 -61 21 11.09           ~ 4 0
11 [AMG2008] S4-M6 Y*O 11 11 39.690 -61 19 43.18           ~ 6 0
12 [AMG2008] S3-C3 Y*O 11 11 45.540 -61 18 45.27           ~ 3 0
13 [AMG2008] S3-M5 Y*O 11 11 49.65 -61 18 52.0           ~ 4 0
14 NGC 3576 HII 11 11 49.8 -61 18 14           ~ 236 2
15 [AMG2008] S3-M4 Y*O 11 11 53.050 -61 18 31.37           ~ 3 0
16 NAME NGC 3576 IRS 1 HII 11 11 54.8 -61 18 26           ~ 31 1
17 [AMG2008] S1-M2 Y*O 11 12 14.430 -61 17 17.50           ~ 4 0
18 [AMG2008] S1-M1 Y*O 11 12 17.210 -61 17 43.50           ~ 4 0
19 [TUW2004] SFO 74 Rad 14 19 40.9 -61 25 17           ~ 2 1
20 NAME Serpens Cloud SFR 18 29 49 +01 14.8           ~ 1100 2
21 LBN 061.50+00.29 HII 19 46 45.7 +25 12 56           ~ 66 0
22 [CPA2006] N131 bub 19 52 21.0 +26 20 54           ~ 14 0
23 SH 2-106 HII 20 27 26.8 +37 22 49           ~ 440 1

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