Abstract:Abstract. We present a study of the LMC compact H ii region N 11A using Hubble Space Telescope imaging observations which resolve N 11A and reveal its unknown nebular and stellar features. The presence of a sharp ionization front extending over more than 4 (1 pc) and fine structure filaments as well as larger loops indicate an environment typical of massive star formation regions, in agreement with high [O iii]/Hβ line ratios. N 11A is a young region, as deduced from its morphology, reddening, and especially h… Show more
“…Three O3 stars have been identified in the LH 10 association ). An even younger compact object, N 11A (IC 2116, Mac Low et al 1998Nazé et al 2001;Heydari-Malayeri et al 2001), occurs in the same area. The location and apparent age difference of LH 10 and LH 9, as well as the gas kinematics, have led to the suggestion that the formation of LH 10 and other stellar groups was triggered by the expanding shells emanating from LH 9 Rosado et al 1996;Barba et al 2003;Hatano et al 2006;Mokiem et al 2007).…”
Context. We study the λ 158 μm [C II] fine-structure line emission from star-forming regions as a function of metallicity. Aims. We have measured and mapped the [C II] emission from the very bright HII region complexes N 11 in the LMC and N 66 in the SMC; as well as the SMC H II regions N 25, N 27, N 83/N 84, and N 88 with the FIFI instrument on the Kuiper Airborne Observatory. Methods. In both LMC and SMC, the ratio of [C II] line to CO line and to the far-infrared continuum emission is much higher than seen almost anywhere else, including Milky Way star-forming regions, and whole galaxies. Results. In the low metallicity, low dust-abundance environment of the LMC and the SMC UV mean free path lengths are much greater than those in the higher-metallicity Milky Way. The increased photoelectric heating efficiencies cause significantly greater relative [C II] line emission strengths. At the same time, similar decreases in PAH abundances have the opposite effect by diminishing photoelectric heating rates. Consequently, in low-metallicity environments relative [C II] strengths are high but exhibit little further dependence on actual metallicity. Relative [C II] strengths are slightly higher in the LMC than in the SMC which has both lower dust and lower PAH abundances.
“…Three O3 stars have been identified in the LH 10 association ). An even younger compact object, N 11A (IC 2116, Mac Low et al 1998Nazé et al 2001;Heydari-Malayeri et al 2001), occurs in the same area. The location and apparent age difference of LH 10 and LH 9, as well as the gas kinematics, have led to the suggestion that the formation of LH 10 and other stellar groups was triggered by the expanding shells emanating from LH 9 Rosado et al 1996;Barba et al 2003;Hatano et al 2006;Mokiem et al 2007).…”
Context. We study the λ 158 μm [C II] fine-structure line emission from star-forming regions as a function of metallicity. Aims. We have measured and mapped the [C II] emission from the very bright HII region complexes N 11 in the LMC and N 66 in the SMC; as well as the SMC H II regions N 25, N 27, N 83/N 84, and N 88 with the FIFI instrument on the Kuiper Airborne Observatory. Methods. In both LMC and SMC, the ratio of [C II] line to CO line and to the far-infrared continuum emission is much higher than seen almost anywhere else, including Milky Way star-forming regions, and whole galaxies. Results. In the low metallicity, low dust-abundance environment of the LMC and the SMC UV mean free path lengths are much greater than those in the higher-metallicity Milky Way. The increased photoelectric heating efficiencies cause significantly greater relative [C II] line emission strengths. At the same time, similar decreases in PAH abundances have the opposite effect by diminishing photoelectric heating rates. Consequently, in low-metallicity environments relative [C II] strengths are high but exhibit little further dependence on actual metallicity. Relative [C II] strengths are slightly higher in the LMC than in the SMC which has both lower dust and lower PAH abundances.
“…#29 and #28, may have been triggered by the eastward expansion of the shell nebula according to the sequential star formation model (Elmegreen & Lada 1977). There are many cases in the literature for which this mechanism has been put forward to explain the observations, in particular that of the SMC H ii region N88A (Heydari-Malayeri et al 1999b).…”
Section: Discussionmentioning
confidence: 99%
“…At the distance of the Magellanic Clouds this corresponds to sizes of more than 50 pc for normal H ii regions and 1 to 3 pc for the blobs. HEBs are in fact associated with young massive stars just leaving their pre-natal molecular cloud (see Heydari-Malayeri et al 1999c for references). Paper I investigated several physical characteristics of N83B-1, such as the emission spectrum, excitation, extinction, gas density, chemical composition, abundances, etc.…”
Abstract. High resolution imaging with the Hubble Space Telescope has uncovered the thus far hidden stellar content and the nebular features of the high excitation compact H ii region N83B in the Large Magellanic Cloud (LMC). We discover that the H ii region is powered by the most recent massive starburst in the OB association LH 5 and the burst has created about 20 blue stars spread over ∼30 on the sky (7.5 pc). Globally N83B displays a turbulent environment typical of newborn massive star formation sites. It contains an impressive ridge, likely created by a shock and a cavity with an estimated age of only ∼30 000 yr, sculpted in the ionized gas by the powerful winds of massive stars. The observations bring to light two compact H ii blobs, N83B-1 and N83B-2, and a small arc-nebula, N83B-3, lying inside the larger H ii region. N83B-1, only ∼2 .8 (0.7 pc) across, is the brightest and most excited part of N83B. It harbors the presumably hottest star of the burst and is also strongly affected by dust with an extinction of AV = 2.5 mag. The second blob, N83B-2, is even more compact, with a size of only ∼1 (0.3 pc). All three features are formed in the border zone between the molecular cloud and the ionized gas possibly in a sequential process triggered by the ionization front of an older H ii region. Our HST imaging presents an interesting and rare opportunity to observe details in the morphology of star formation on very small spatial scales in the LMC which are in agreement with the concept of the fractal structure of molecular star-forming clouds. A scenario which supports hierarchical massive star formation in the LMC OB association LH 5 is presented.
“…These authors proposed that the nebular morphology of N11A is a good example of the champagne model (Tenorio-Tagle 1979;Bodenheimer et al 1979), in the stage when the newborn stars disrupt the molecular cavity. Small nebular emission filaments discovered by Heydari-Malayeri et al (2001) are located on the south-west border of the nebular knot, and show arcs pointing toward the direction where the CO emission has a sharp edge, indicating an abrupt drop of the molecular gas density. This morphology suggests that the compact group of stars could be blowing this side of its stellar nursery, in a similar morphological picture to that seen towards Knot 1 in the 30 Dor Nebula (Rubio et al 1998;Walborn et al 1999a;Walborn, Maíz-Apellániz & Barbá 2002).…”
Section: Comparison Between Molecular Co and Optical Nebular Emissionsmentioning
confidence: 94%
“…In the case of N11A, the optical compact group of stars is visible indicating that the molecular cloud lies behind the stars and that they have evacuated a cavity towards our line of sight. This conclusion is supported by the fact that the O star has a relatively low reddening, A V = 0.6, probably due only to dust mixed with the ionised gas (Heydari-Malayeri et al 2001). These authors proposed that the nebular morphology of N11A is a good example of the champagne model (Tenorio-Tagle 1979;Bodenheimer et al 1979), in the stage when the newborn stars disrupt the molecular cavity.…”
Section: Comparison Between Molecular Co and Optical Nebular Emissionsmentioning
The second largest H II region in the Large Magellanic Cloud, N11B has been surveyed in the near IR. We present JHKs images of the N11B nebula.These images are combined with CO(1 → 0) emission line data and with archival NTT and HST/WFPC2 optical images to address the star formation activity of the region. IR photometry of all the IR sources detected is given. We confirm that a second generation of stars is currently forming in the N11B region. Our IR images show the presence of several bright IR sources which appear located towards the molecular cloud as seen from the CO emission in the area. Several of these sources show IR colours with YSO characteristics and they are prime candidates to be intermediate-mass Herbig Ae/Be stars. For the first time an extragalactic methanol maser is directly associated with IR sources embedded in a molecular core. Two IR sources are found at 2 ′′ (0.5 pc) of the methanol maser reported position. Additionally, we present the association of the N11A compact H II region to the molecular gas where we find that the young massive O stars have eroded a cavity in the parental molecular cloud, typical of a champagne flow. The N11 region turns out to be a very good laboratory for studying the interaction of winds, UV radiation and molecular gas. Several photodissociation regions are found.
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