2020A&A...644A..52A


Query : 2020A&A...644A..52A

2020A&A...644A..52A - Astronomy and Astrophysics, volume 644A52-52 (2020/12-1)

Role of the magnetic field in the fragmentation process: the case of G14.225-0.506.

ANEZ-LOPEZ N., BUSQUET G., KOCH P.M., GIRART J.M., LIU H.B., SANTOS F., CHAPMAN N.L., NOVAK G., PALAU A., HO P.T.P. and ZHANG Q.

Abstract (from CDS):


Context. Magnetic fields are predicted to play a significant role in the formation of filamentary structures and their fragmentation to form stars and star clusters.
Aims. We aim to investigate the role of the magnetic field in the process of core fragmentation toward the two hub-filament systems in the infrared dark cloud G14.225-0.506, which present different levels of fragmentation.
Methods. We performed observations of the thermal dust polarization at 350µm using the Caltech Submillimeter Observatory (CSO) with an angular resolution of 10'' toward the two hubs (Hub-N and Hub-S) in the infrared dark cloud G14.225-0.506. We additionally applied the polarization-intensity-gradient method to estimate the significance of the magnetic field over the gravitational force.
Results. The sky-projected magnetic field in Hub-N shows a rather uniform structure along the east-west orientation, which is roughly perpendicular to the major axis of the hub-filament system. The intensity gradient in Hub-N displays a single local minimum coinciding with the dust core MM1a detected with interferometric observations. Such a prevailing magnetic field orientation is slightly perturbed when approaching the dust core. Unlike the northern Hub, Hub-S shows two local minima, reflecting the bimodal distribution of the magnetic field. In Hub-N, both east and west of the hub-filament system, the intensity gradient and the magnetic field are parallel whereas they tend to be perpendicular when penetrating the dense filaments and hub. Analysis of the |δ|- and ΣB-maps indicates that, in general, the magnetic field cannot prevent gravitational collapse, both east and west, suggesting that the magnetic field is initially dragged by the infalling motion and aligned with it, or is channeling material toward the central ridge from both sides. Values of ΣB≥1 are found toward a north-south ridge encompassing the dust emission peak, indicating that in this region magnetic field dominates over gravity force, or that with the current angular resolution we cannot resolve a hypothetically more complex structure. We estimated the magnetic field strength, the mass-to-flux ratio, and the Alfven Mach number, and found differences between the two hubs.
Conclusions. The different levels of fragmentation observed in these two hubs could arise from differences in the properties of the magnetic field rather than from differences in the intensity of the gravitational field because the density in the two hubs is similar. However, environmental effects could also play a role.

Abstract Copyright: © ESO 2020

Journal keyword(s): stars: formation - ISM: clouds - ISM: individual objects: G14.225-0.506 - ISM: magnetic fields

Simbad objects: 17

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Number of rows : 17
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 4B Y*O 03 29 12.058 +31 13 02.05           ~ 625 0
2 NAME Orion-KL SFR 05 35 14.16 -05 22 21.5           ~ 2421 1
3 IRAS 16293-2422 cor 16 32 22.56 -24 28 31.8           ~ 1357 1
4 NAME the Pipe Nebula DNe 17 30 -25.0           ~ 442 1
5 [PFA2014] SDC13 DNe 18 14 29.7 -17 32 35           ~ 22 0
6 [BEP2016] Hub-N MM1a mm 18 18 12.32 -16 49 28.1           ~ 5 0
7 [BEP2016] Hub-S MM4 mm 18 18 12.84 -16 57 20.3           ~ 3 0
8 [BEP2016] Hub-S MM5a mm 18 18 13.34 -16 57 24.1           ~ 4 0
9 [BEP2016] Hub-S MM7a mm 18 18 13.92 -16 57 11.7           ~ 3 0
10 IRAS 18153-1651 IR 18 18 16.0 -16 50 39           ~ 22 0
11 NAME M17 SWex MoC 18 19.0 -16 40           ~ 62 0
12 NGC 6618 OpC 18 20 47 -16 10.3           ~ 1700 0
13 NAME Serpens South molecular cloud MoC 18 30 -02.0           ~ 116 0
14 AGAL G034.411+00.234 Y*O 18 53 18.0319 +01 25 25.500           ~ 108 0
15 MSXDC G034.43+00.24 MoC 18 53 18.9 +01 26 39           ~ 122 0
16 W 51e2 Ma* 19 23 43.906 +14 30 34.48           ~ 222 0
17 W 51 SNR 19 23 50 +14 06.0           ~ 1352 1

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