2015A&A...584A..67B


Query : 2015A&A...584A..67B

2015A&A...584A..67B - Astronomy and Astrophysics, volume 584A67-67 (2015/12-1)

Filament fragmentation in high-mass star formation.

BEUTHER H., RAGAN S.E., JOHNSTON K., HENNING Th., HACAR A. and KAINULAINEN J.T.

Abstract (from CDS):

Filamentary structures in the interstellar medium are crucial ingredients of the star formation process. They fragment to form individual star-forming cores, and at the same time they may also funnel gas toward the central gas cores, providing an additional gas reservoir. We want to resolve the length scales for filament formation and fragmentation (resolution ≤0.1pc), in particular the Jeans length and cylinder fragmentation scale. We have observed the prototypical high-mass star-forming filament IRDC18223 with the Plateau de Bure Interferometer (PdBI) in the 3.2mm continuum and N2H+(1-0) line emission in a ten-field mosaic at a spatial resolution of ∼4'' (∼14000au). The dust continuum emission resolves the filament into a chain of at least 12 relatively regularly spaced cores. The mean separation between cores is ∼0.40(±0.18)pc. While this is approximately consistent with the fragmentation of an infinite, isothermal, and gravitationally bound gas cylinder, a high mass-to-length ratio of M/l≃1000M☉/pc requires additional turbulent and/or magnetic support against radial collapse of the filament. The N2H+(1-0) data reveal a velocity gradient perpendicular to the main filament. Although rotation of the filament cannot be excluded, the data are also consistent with the main filament being comprised of several velocity-coherent subfilaments. Furthermore, this velocity gradient perpendicular to the filament resembles results toward Serpens south that are interpreted as signatures of filament formation within magnetized and turbulent sheet-like structures. Lower-density gas tracers ([CI] and C18O) reveal a similar red- and blueshifted velocity structure on scales around 60'' east and west of the filament. This may tentatively be interpreted as a signature of the large-scale cloud and the smaller scale filament being kinematically coupled. We do not identify a velocity gradient along the axis of the filament. This may be due to no significant gas flows along the filamentary axis, but it may also be partly caused by a low inclination angle of the filament with respect to the plane of the sky minimizing such a signature. The IRDC18223 3.2mm continuum data are consistent with thermal fragmentation of a gravitationally bound and compressible gas cylinder. However, the high mass-to-length ratio requires additional support - most likely turbulence and/or magnetic fields - against collapse. The N2H+ spectral line data indicate a kinematic origin of the filament, but we cannot conclusively differentiate whether it has formed out of (pre-existing) velocity-coherent subfilaments, whether magnetized converging gas flows, a larger-scale collapsing cloud, or even whether rotation played a significant role during filament formation.

Abstract Copyright: ∼

Journal keyword(s): stars: formation - stars: early-type - stars: individual: IRDC 18223 - stars: massive - ISM: clouds - ISM: structure

VizieR on-line data: <Available at CDS (J/A+A/584/A67): list.dat fits/*>

Nomenclature: Table 1: [BRJ2015] NN (Nos 1-12).

Simbad objects: 25

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Number of rows : 25
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 Taurus Complex SFR 04 41.0 +25 52           ~ 4971 0
2 3C 279 Bla 12 56 11.16657958 -05 47 21.5251510   18.01 17.75 15.87   ~ 3205 2
3 4C 38.41 Bla 16 35 15.49297809 +38 08 04.5005995   18.14 17.97 17.25   ~ 906 1
4 3C 345 Bla 16 42 58.80997043 +39 48 36.9939552   16.81 16.59 16.84   ~ 1808 3
5 QSO B1730-130 Bla 17 33 02.70578907 -13 04 49.5482119   18 19.50 18.78 17.39 ~ 1198 1
6 QSO B1741-038 Bla 17 43 58.85613537 -03 50 04.6167326     20.40 17.98   ~ 583 1
7 [CCE98b] 011.11-0.12 Cld 18 10.5 -19 23           ~ 119 2
8 [BRJ2015] 12 cor 18 25 06.94 -12 45 56.7           ~ 1 0
9 NAME IRDC 18223-3 Y*O 18 25 08 -12 45.5           ~ 80 0
10 [BRJ2015] 11 cor 18 25 08.49 -12 45 22.0           ~ 1 0
11 [BRJ2015] 10 cor 18 25 09.09 -12 44 52.0           ~ 1 0
12 SSTGLMC G018.6188-00.0711 Y*? 18 25 09.12480 -12 44 37.1364           ~ 6 0
13 [BRJ2015] 8 cor 18 25 09.31 -12 44 26.4           ~ 1 0
14 SSTGLMC G018.6400-00.0630 Y*? 18 25 09.781 -12 43 15.56           ~ 4 0
15 [BRJ2015] 3 cor 18 25 09.99 -12 42 56.1           ~ 1 0
16 SSTGLMC G018.6274-00.0705 Y*O 18 25 10.0397930400 -12 44 08.557501272           ~ 30 0
17 [BRJ2015] 6 cor 18 25 10.04 -12 43 43.6           ~ 1 0
18 [BRJ2015] 5 cor 18 25 10.21 -12 43 24.2           ~ 1 0
19 [BRJ2015] 2 cor 18 25 10.61 -12 42 25.0           ~ 1 0
20 IRAS 18223-1243 Y*O 18 25 10.9307288448 -12 42 15.754722912           ~ 67 1
21 [BRJ2015] 1 cor 18 25 11.11 -12 41 52.8           ~ 1 0
22 NAME Serpens Cloud SFR 18 29 49 +01 14.8           ~ 1195 1
23 MSXDC G035.39-00.33 MoC 18 57 09.0 +02 07 46           ~ 132 0
24 EM* MWC 349 ** 20 32 45.499080 +40 39 36.74124   15.88 13.15 12.13   Bep 837 0
25 NAME BL Lac BLL 22 02 43.2913536816 +42 16 39.979416792   15.66 14.72     ~ 2397 1

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