2020A&A...644A..25T


Query : 2020A&A...644A..25T

2020A&A...644A..25T - Astronomy and Astrophysics, volume 644A25-25 (2020/12-1)

Cause and effects of the massive star formation in Messier 8 East.

TIWARI M., MENTEN K.M., WYROWSKI F., GIANNETTI A., LEE M.-Y., KIM W.-J. and PEREZ-BEAUPUITS J.P.

Abstract (from CDS):


Context. Messier 8 (M8), one of the brightest HII regions in our Galaxy, is powered by massive O-type stars and is associated with recent and ongoing massive star formation. Two prominent massive star-forming regions associated with M8 are M8-Main, the particularly bright part of the large-scale HII region (mainly) ionized by the stellar system Herschel 36 (Her 36) and M8 East (M8 E), which is mainly powered by a deeply embedded young stellar object (YSO), the bright infrared (IR) source M8E-IR.
Aims. We study the interaction of the massive star-forming region M8 E with its surroundings using observations of assorted diffuse and dense gas tracers that allow quantifying the kinetic temperatures and volume densities in this region. With a multiwavelength view of M8 E, we investigate the cause of star formation. Moreover, we compare the star-forming environments of M8-Main and M8 E, based on their physical conditions and the abundances of the various observed species toward them.
Methods. We used the Institut de Radioastronomia Millimetrica 30m telescope to perform an imaging spectroscopy survey of the ∼1pc scale molecular environment of M8E-IR and also performed deep integrations toward the source itself. We imaged and analyzed data for the J=1-0 rotational transitions of 12CO, 13CO, N2H+, HCN, H13CN, HCO+, H13CO+, HNC, and HN13C observed for the first time toward M8 E. To visualize the distribution of the dense and diffuse gas in M8 E, we compared our velocity-integrated intensity maps of 12CO, 13CO, and N2H+ with ancillary data taken at IR and submillimeter wavelengths. We used techniques that assume local thermodynamic equilibrium (LTE) and non-LTE to determine column densities of the observed species and constrain the physical conditions of the gas that causes their emission. Examining the class 0/ I and classII YSO populations in M8 E, allows us to explore the observed ionization front (IF) as seen in the high resolution Galactic Legacy Infrared Mid-Plane Survey Extraordinaire (GLIMPSE) 8µm emission image. The difference between the ages of the YSOs and their distribution in M8 E were used to estimate the speed of the IF.
Results. We find that 12CO probes the warm diffuse gas also traced by the GLIMPSE 8µm emission, while N2H+ traces the cool and dense gas following the emission distribution of the APEX Telescope Large Area Survey of the Galaxy 870µm dust continuum. We find that the star-formation in M8 E appears to be triggered by the earlier formed stellar cluster NGC 6530, which powers an HII region giving rise to an IF that is moving at a speed ≥0.26km/s across M8 E. Based on our qualitative and quantitative analysis, the J=1-0 transition lines of N2H+ and HN13C appear to be more direct tracers of dense molecular gas than the J=1-0 transition lines of HCN and HCO+. We derive temperatures of 80 and 30K for the warm and cool gas components, respectively, and constrain the H2 volume densities to be in the range of 104-106cm–3. Comparison of the observed abundances of various species reflects the fact that M8 E is at an earlier stage of massive star formation than M8-Main.

Abstract Copyright: © M. Tiwari et al. 2020

Journal keyword(s): ISM: abundances - ISM: molecules - submillimeter: ISM - stars: formation - ISM: individual objects: M 8

Simbad objects: 32

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Number of rows : 32
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 OMC-1 MoC 05 35 14 -05 22.4           ~ 1249 2
2 NAME Orion Bright Bar reg 05 35 22.30 -05 24 33.0           ~ 1004 0
3 NAME Ori A MoC 05 38 -07.1           ~ 3187 0
4 NAME Ori B MoC 05 41 43.0 -01 54 44           ~ 1498 0
5 NAME Car-Sgr Arm PoG 15 00 -40.0           ~ 581 1
6 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
7 NAME Sgr B2 MoC 17 47 20.4 -28 23 07           ~ 2443 1
8 QSO J1800-241 QSO 18 00 30.3898648512 -24 04 02.807778180           ~ 7 0
9 M 8 OpC 18 03 37 -24 23.2           ~ 644 1
10 NAME Her 36SE Y*O 18 03 40.3201232304 -24 22 42.857540472 10.26 11.022 10.372 10.267   O8V+ 210 0
11 NAME Hourglass Nebula ISM 18 03 41.1 -24 22 37           ~ 79 2
12 * 9 Sgr Y*O 18 03 52.4450051016 -24 21 38.632254012 5.08 5.97 5.97 5.72 5.70 O4V((f))z 563 0
13 NGC 6530 OpC 18 04 31 -24 21.5           ~ 443 0
14 Cl* NGC 6530 SCB 810 Or* 18 04 43.5151983552 -24 27 38.619388476   18.077 16.265   13.938 K2-K3V 17 0
15 2MASS J18044363-2427591 Or* 18 04 43.6183065984 -24 27 59.203818288   20.293 18.509   15.949 ~ 11 0
16 Cl* NGC 6530 WFI 14025 Or* 18 04 46.3886187144 -24 26 07.874030868 21.413 19.047 17.368   15.199 K7-M0V 13 0
17 2MASS J18044709-2427550 Y*? 18 04 47.090 -24 27 55.09           ~ 4 0
18 2MASS J18044804-2427243 Y*? 18 04 48.048 -24 27 24.36           ~ 2 0
19 [KA2010] 0/I 59 Y*? 18 04 48.42 -24 27 53.8           ~ 2 0
20 V* V1803 Sgr Or* 18 04 48.508608 -24 26 40.40016   18.437 17.102 16.36 14.946 ~ 9 0
21 2MASS J18045017-2427590 Y*? 18 04 50.174 -24 27 59.01           ~ 2 0
22 IRAS 18017-2414 Y*? 18 04 50.332 -24 14 25.93           ~ 3 0
23 EM* LkHA 115 Ae* 18 04 50.5999226472 -24 25 42.095461620   12.380 11.949   11.198 B7e 39 0
24 Cl* NGC 6530 WFI 16451 Y*O 18 04 51.52920 -24 24 17.3232   21.437 19.042   15.961 ~ 14 0
25 2MASS J18045155-2426110 Y*? 18 04 51.553 -24 26 11.05           ~ 3 0
26 2MASS J18045263-2427306 Y*? 18 04 52.6200837480 -24 27 30.770608680           ~ 3 0
27 RAFGL 2059 Y*O 18 04 53.1586569336 -24 26 41.642012796 19.905 21.910 18.914   14.078 ~ 146 0
28 2MASS J18045347-2426085 Y*O 18 04 53.4607151184 -24 26 08.711003148   21.913 19.331   15.669 ~ 4 0
29 2MASS J18045677-2427160 Y*? 18 04 56.773 -24 27 16.08           ~ 3 0
30 2MASS J18045878-2426240 Y*? 18 04 58.789 -24 26 24.08           ~ 4 0
31 W 49 SFR 19 10 20 +09 07.7           ~ 601 1
32 W 51 SNR 19 23 50 +14 06.0           ~ 1352 1

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