2013A&A...550A.116T


Query : 2013A&A...550A.116T

2013A&A...550A.116T - Astronomy and Astrophysics, volume 550A, 116-116 (2013/2-1)

Triggered/sequential star formation ? A multi-phase ISM study around the prominent IRDC G18.93-0.03.

TACKENBERG J., BEUTHER H., PLUME R., HENNING T., STIL J., WALMSLEY M., SCHULLER F. and SCHMIEDEKE A.

Abstract (from CDS):

Triggered star formation has been discussed for many years, and evidence for the formation of stars and cores triggered by HII regions is under debate. We investigate the imprints of an expanding HII region on a pre-existing starless clumps. We selected an infrared dark filament spanning 0.8°. One portion of this filament, G18.93-0.03 is a prominent dust complex, with the molecular clump G18.93/m being IR dark from near-IR wavelength up to 160um. Spitzer composite images show an IR bubble spatially associated with G18.93-0.03. We use GRS 13CO and IRAM 30m H13CO+ data to disentangle the large and small scale spatial structure of the region. From ATLASGAL submm data we calculate the gas mass, while we use the H13CO+ line width to estimate its virial mass. To study the IR properties of G18.93/m we use Herschel data and produce temperature maps from fitting the spectral energy distribution. With the MAGPIS 20cm and SuperCOSMOS Hα data we trace the ionized gas, and the VGPS Hi survey provides information on the atomic hydrogen gas. We show that the bubble is spatially associated with G18.93, located at a kinematic near distance of 3.6kpc. The total gas mass of ∼870um splits up into 6 sub-clumps, of which G18.93/m is the most massive with 280um. The virial analysis shows that it may be gravitationally bound and has neither Spitzer young stellar objects nor mid-IR point sources within. Therefore we call it pre-stellar. Fitting the spectral energy distribution reveals a temperature distribution that decreases towards its center, but heating from the ionizing source puts it above the general ISM temperature. We find that the bubble is filled by HII gas, ionized by an O8.5 star. Between the ionizing source and the IR dark clump G18.93/m we find a layered structure of hydrogen phases, from ionized to atomic to molecular gas, revealing a photon dominated region. Furthermore, we identify an additional velocity component within the bubble's 8um emission rim at the edge of the infrared dark cloud and speculate that it might be shock induced by the expanding HII region. While the elevated temperature allows for the build-up of larger fragments, and the shock induced velocity component may lead to additional turbulent support, the density profile of G18.93/m does not show signatures of the expanding bubble. While the first two signatures favor high-mass star formation, we do not find conclusive evidence that the massive clump G18.93/m is prone to collapse because of the expanding HII region.

Abstract Copyright:

Journal keyword(s): ISM: bubbles - stars: formation - stars: massive - HII regions

Nomenclature: Table 1: [TBP2013] N (Nos 1-5), [TBP2013] main.

Simbad objects: 16

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Number of rows : 16
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 [ABB2014] WISE G018.978+00.030 bub 18 25 28.6 -12 22 37           ~ 5 0
2 [TBP2013] 2 Cld 18 25 30.9 -12 27 29           ~ 1 0
3 [SMC2009] G18.93-0.01 smm 18 25 32.35 -12 26 41.4           ~ 2 0
4 [TBP2013] 1 Cld 18 25 32.40000 -12 26 47.0000           ~ 1 0
5 [ERG2015] 3315 cor 18 25 33.1558 -12 26 52.347           ~ 7 0
6 RAFGL 5487 MIR 18 25 33.756 -12 25 21.18           ~ 5 0
7 IRAS 18227-1227 mul 18 25 35.1 -12 25 20           ~ 5 0
8 SDC G18.928-0.031 DNe 18 25 35.98 -12 27 05.4           ~ 5 0
9 [TBP2013] main Cld 18 25 36.0 -12 26 48           ~ 1 0
10 [TBP2013] 4 Cld 18 25 37.6 -12 26 19           ~ 1 0
11 [TBP2013] 3 Cld 18 25 38.3 -12 26 11           ~ 1 0
12 [TBP2013] 5 Cld 18 25 41.0 -12 25 10           ~ 1 0
13 EGO G019.01-0.03 of? 18 25 44.8 -12 22 46           ~ 23 0
14 [CPA2006] N24 bub 18 26 35.4 -12 36 06           ~ 11 0
15 SNR G030.8-00.0 SNR 18 47 32 -01 56.5           ~ 512 0
16 IRAS 18454-0158 HII 18 48 01.3 -01 54 49           ~ 15 0

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2023.09.21-17:59:33

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