2013ApJ...775...88N


Query : 2013ApJ...775...88N

2013ApJ...775...88N - Astrophys. J., 775, 88 (2013/October-1)

Low-velocity shocks traced by extended SiO emission along the W43 ridges: witnessing the formation of young massive clusters.

NGUYEN-LUONG Q., MOTTE F., CARLHOFF P., LOUVET F., LESAFFRE P., SCHILKE P., HILL T., HENNEMANN M., GUSDORF A., DIDELON P., SCHNEIDER N., BONTEMPS S., DUARTE-CABRAL A., MENTEN K.M., MARTIN P.G., WYROWSKI F., BENDO G., ROUSSEL H., BERNARD J.-P., BRONFMAN L., HENNING T., KRAMER C. and HEITSCH F.

Abstract (from CDS):

The formation of high-mass stars is tightly linked to that of their parental clouds. Here, we focus on the high-density parts of W43, a molecular cloud undergoing an efficient event of star formation. Using a column density image derived from Herschel continuum maps, we identify two high-density filamentary clouds, called the W43-MM1 and W43-MM2 ridges. Both have gas masses of 2.1x104 M☉ and 3.5x104 M☉above >1023/cm2 and within areas of ∼6 and ∼14 pc2, respectively. The W43-MM1 and W43-MM2 ridges are structures that are coherent in velocity and gravitationally bound, despite their large velocity dispersion measured by the N2H+ (1-0) lines of the W43-HERO IRAM large program. Another intriguing result is that these ridges harbor widespread (∼10 pc2) bright SiO (2-1) emission, which we interpret to be the result of low-velocity shocks ( ≤ 10 km/s). We measure a significant relationship between the SiO (2-1) luminosity and velocity extent and show that it distinguishes our observations from the high-velocity shocks associated with outflows. We use state-of-the-art shock models to demonstrate that a small percentage (10%) of Si atoms in low-velocity shocks, observed initially in gas phase or in grain mantles, can explain the observed SiO column density in the W43 ridges. The spatial and velocity overlaps between the ridges of high-density gas and the shocked SiO gas suggest that ridges could be forming via colliding flows driven by gravity and accompanied by low-velocity shocks. This mechanism may be the initial conditions for the formation of young massive clusters.

Abstract Copyright: ∼

Journal keyword(s): H II regions - ISM: clouds - ISM: molecules - ISM: structure - stars: formation - stars: protostars

Simbad objects: 23

goto Full paper

goto View the references in ADS

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 - 2026
#notes
1 NAME Sgr A* X 17 45 40.03599 -29 00 28.1699           ~ 4970 3
2 NAME the Brick MoC 17 46 09 -28 43.8           ~ 226 0
3 GAL 001.6-00.025 MoC 17 49 29 -27 36.8           ~ 31 0
4 RAFGL 2046 HII 18 00 32.1 -24 04 03           ~ 380 0
5 [MSL2003] W43-MM22 smm 18 47 27.0 -02 00 36           ~ 2 0
6 W 43 SFR 18 47 32 -01 56.5           ~ 604 0
7 [MSL2003] W43-MM18 smm 18 47 35.6 -02 02 14           ~ 3 0
8 AGAL G030.703-00.067 cor 18 47 36.6 -02 00 54           ~ 87 0
9 AGAL G030.741-00.061 cor 18 47 39.6 -01 58 34           ~ 20 0
10 [MSL2003] W43-MM16 smm 18 47 40.1 -01 53 34           ~ 3 0
11 [MSL2003] W43-MM3 smm 18 47 41.7 -02 00 26           ~ 38 0
12 [MSL2003] W43-MM17 smm 18 47 42.5 -01 59 38           ~ 2 0
13 [MSL2003] W43-MM9 smm 18 47 44.8 -01 54 43           ~ 4 0
14 AGAL G030.818-00.056 cor 18 47 47.0 -01 54 28           ~ 186 0
15 [MSL2003] W43-MM33 smm 18 47 50.2 -01 54 04           ~ 2 0
16 AGAL G030.848-00.081 Y*O 18 47 56 -01 53.5           ~ 36 0
17 RAFGL 2271 SFR 18 53 18.54 +01 14 57.9           ~ 537 0
18 MSXDC G035.39-00.33 MoC 18 57 09.0 +02 07 46           ~ 132 0
19 W 49 SFR 19 10 20 +09 07.7           ~ 601 1
20 W 51 SNR 19 23 50 +14 06.0           ~ 1352 1
21 NAME Cyg X Cld 20 30 04.7973633 +40 51 36.002197           ~ 962 1
22 DR 21 SFR 20 39 01.6 +42 19 38           O4.5 1121 0
23 NAME Galactic Bar reg ~ ~           ~ 1458 0

To bookmark this query, right click on this link: simbad:objects in 2013ApJ...775...88N and select 'bookmark this link' or equivalent in the popup menu