Lise Deharveng
Aix-Marseille University
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Astronomy and Astrophysics | 2006
A. Zavagno; Lise Deharveng; Fernando Comeron; J. Brand; Fabrizio Massi; James Caplan; D. Russeil
We present SEST-SIMBA 1.2-mm continuum maps and ESO-NTT SOFIJHKS images of the Galactic H ii region RCW 79. The millimetre continuum data reveal the presence of massive fragments located in a dust emission ring surrounding the ionized gas. The two most massive fragments are diametrically opposite each other in the ring. The near-IR data, centred on the compact H ii region located at the south-eastern border of RCW 79, show the presence of an IR-bright cluster containing massive stars along with young stellar objects with near-IR excesses. A bright near- and mid-IR source is detected towards maser emissions, 1.2 pc north-east of the compact H ii region centre. Additional information, extracted from the Spitzer GLIMPSE survey, are used to discuss the nature of the bright IR sources observed towards RCW 79. Twelve luminous Class I sources are identified towards the most massive millimetre fragments. All these facts strongly indicate that the massive-star formation observed at the border of the H ii region RCW 79 has been triggered by its expansion, most probably by the collect and collapse process.
Astronomy and Astrophysics | 2013
D. Russeil; N. Schneider; L. D. Anderson; A. Zavagno; S. Molinari; P. Persi; Sylvain Bontemps; F. Motte; V. Ossenkopf; P. André; D. Arzoumanian; J.-Ph. Bernard; Lise Deharveng; P. Didelon; J. Di Francesco; D. Elia; M. Hennemann; T. Hill; V. Könyves; J. Z. Li; P. G. Martin; Q. Nguyen Luong; Nicolas Peretto; S. Pezzuto; D. Polychroni; H. Roussel; K. L. J. Rygl; L. Spinoglio; L. Testi; J. Tigé
Aims: Fundamental to any theory of high-mass star formation are gravity and turbulence. Their relative importance, which probably changes during cloud evolution, is not known. By investigating the spatial and density structure of the high-mass star-forming complex NGC 6334 we aim to disentangle the contributions of turbulence and gravity. Methods: We used Herschel PACS and SPIRE imaging observations from the HOBYS key programme at wavelengths of 160, 250, 350, and 500 μm to construct dust temperature and column density maps. Using probability distribution functions (PDFs) of the column density determined for the whole complex and for four distinct sub-regions (distinguished on the basis of differences in the column density, temperature, and radiation field), we characterize the density structure of the complex. We investigate the spatial structure using the Δ-variance, which probes the relative amount of structure on different size scales and traces possible energy injection mechanisms into the molecular cloud. Results: The Δ-variance analysis suggests that the significant scales of a few parsec that were found are caused by energy injection due to expanding H ii regions, which are numerous, and by the lengths of filaments seen everywhere in the complex. The column density PDFs have a lognormal shape at low densities and a clearly defined power law at high densities for all sub-regions whose slope is linked to the exponent α of an equivalent spherical density distribution. In particular with α = 2.37, the central sub-region is largly dominated by gravity, caused by individual collapsing dense cores and global collapse of a larger region. The collapse is faster than free-fall (which would lead only to α = 2) and thus requires a more dynamic scenario (external compression, flows). The column density PDFs suggest that the different sub-regions are at different evolutionary stages, especially the central sub-region, which seems to be in a more evolved stage. Herschel is an ESA space observatory with science instruments provided by European-led Principal Investigator consortia and with important participation from NASA.Appendix A is available in electronic form at http://www.aanda.org
Astronomy and Astrophysics | 2012
Lise Deharveng; A. Zavagno; L. D. Anderson; F. Motte; Alain Abergel; P. André; Sylvain Bontemps; G. Leleu; H. Roussel; D. Russeil
W5-E has been observed with the Herschel-PACS and -SPIRE photometers, at 100, 160, 250, 350, and 500 microns. The dust temperature map shows a rather uniform temperature, in the range 17.5-20 K in the dense condensations or filaments, 21-22 K in the photodissociation regions, and 24-31 K in the direction of the ionized regions. The column densities are rather low, everywhere lower than 10^23 cm-2, and of the order of a few 10^21 cm-2 in the PDRs. About 8000 solar masses of neutral material surrounds the ionized region, which is low with respect to the volume of this HII region; we suggest that the exciting stars of the W5-E, W5-W, Sh~201, A and B HII regions formed along a dense filament or sheet rather than inside a more spherical cloud. Fifty point sources have been detected at 100 microns. Most of them are Class 0/I YSOs. The SEDs of their envelopes have been fitted using a modified blackbody model. These envelopes are cold, with a mean temperature of 15.7+-1.8K. Their masses are in the range 1.3-47 solar masses. Eleven of these point sources are candidate Class 0 YSOs. Twelve of these point sources are possibly at the origin of bipolar outflows detected in this region. None of the YSOs contain a massive central object, but a few may form a massive star as they have both a massive envelope and also a high envelope accretion rate. Most of the Class 0/I YSOs are observed in the direction of high column density material, for example in the direction of the massive condensations present at the waist of the bipolar Sh 201 HII region or enclosed by the bright-rimmed cloud BRC14. The overdensity of Class 0/I YSOs on the borders of the HII regions strongly suggests that triggered star formation is at work in this region but, due to insufficient resolution, the exact processes at the origin of the triggering are difficult to determine.
Astronomy and Astrophysics | 2014
M. R. Samal; A. Zavagno; Lise Deharveng; S. Molinari; D. K. Ojha; D. Paradis; J. Tigé; A. K. Pandey; D. Russeil
Aims. We investigate the star formation activity in the molecular complex associated with the Galactic H II region Sh2-90. Methods. We obtain the distribution of the ionized and cold neutral gas using radio-continuum and Herschel observations. We use near-infrared and Spitzer data to investigate the stellar content of the complex. We discuss the evolutionary status of embedded massive young stellar objects (MYSOs) using their spectral energy distribution. Results. The Sh2-90 region presents a bubble morphology in the mid-infrared. Radio observations suggest it is an evolved H II region with an electron density similar to 144 cm(-3), emission measure similar to 6.7 x 10(4) cm(-6) pc and an ionized mass similar to 55 M-circle dot. From Herschel and CO (J = 3-2) observations we found that the H II region is part of an elongated extended molecular cloud (H-2 column density \textgreater= 3 x 10(21) cm(-2) and dust temperature 18-27 K) of total mass = 1 x 10(4) M-circle dot. We identify the ionizing cluster of Sh2-90, the main exciting star being an O8-O9 V star. Five cold dust clumps, four mid-IR blobs around B stars, and a compact H II region are found at the edge of the bubble. The velocity information derived from CO data cubes suggest that most of them are associated with the Sh2-90 region. One hundred and twenty-nine low mass (\textless= 3 M-circle dot) YSOs have been identified, and they are found to be distributed mostly in the regions of high column density. Four candidate Class 0/I MYSOs have been found. We suggest that multi-generation star formation is present in the complex. From evidence of interaction, time scales involved, and evolutionary status of stellar/protostellar sources, we argue that the star formation at the edges of Sh2-90 might have been triggered. However, several young sources in this complex are probably formed by some other processes.
Astronomy and Astrophysics | 2015
Lise Deharveng; A. Zavagno; M. R. Samal; L. D. Anderson; G. Leleu; D. Brevot; A. Duarte-Cabral; S. Molinari; M. Pestalozzi; Jonathan B. Foster; Jill Rathborne; James M. Jackson
Aims. Our goal is to identify bipolar H II regions and to understand their morphology, their evolution, and the role they play in the formation of new generations of stars. Methods. We use the Spitzer-GLIMPSE, -MIPSGAL, and Herschel-Hi-GAL surveys to identify bipolar H II regions, looking for (ionized) lobes extending perpendicular to dense filamentary structures. We search for their exciting star(s) and estimate their distances using near-IR data from the 2MASS or UKIDSS surveys. Dense molecular clumps are detected using Herschel-SPIRE data, and we estimate their temperature, column density, mass, and density. MALT90 observations allow us to ascertain their association with the central H II region (association based on similar velocities). We identify Class 0/I young stellar objects (YSOs) using their Spitzer and Herschel-PACS emissions. These methods will be applied to the entire sample of candidate bipolar H II regions to be presented in a forthcoming paper. Results. This paper focuses on two bipolar H II regions, one that is especially interesting in terms of its morphology, G319.88+00.79, and one in terms of its star formation, G010.32-00.15. Their exciting clusters are identified and their photometric distances estimated to be 2.6 kpc and 1.75 kpc, respectively; thus G010.32-00.15 (known as W31 north) lies much closer than previously assumed. We suggest that these regions formed in dense and flat structures that contain filaments. They have a central ionized region and ionized lobes extending perpendicular to the parental cloud. The remains of the parental cloud appear as dense (more than 10(4) cm(-3)) and cold (14-17 K) condensations. The dust in the photodissociation regions (in regions adjacent to the ionized gas) is warm (19-25 K). Dense massive clumps are present around the central ionized region. G010.32-00.14 is especially remarkable because five clumps of several hundred solar masses surround the central H II region; their peak column density is a few 10(23) cm(-2), and the mean density in their central regions reaches several 10(5) cm(-3). Four of them contain at least one massive YSO (including an ultracompact H II region and a high-luminosity Class I YSO); these clumps also contain extended green objects (EGOs) and Class II methanol masers. This morphology suggests that the formation of a second generation of massive stars has been triggered by the central bipolar H II region. It occurs in the compressed material of the parental cloud.
Astronomy and Astrophysics | 2017
P. Palmeirim; A. Zavagno; D. Elia; T. J. T. Moore; Anthony Peter Whitworth; P. Tremblin; A. Traficante; M. Merello; D. Russeil; S. Pezzuto; L. Cambrésy; Adriano Baldeschi; M. Bandieramonte; Ugo Becciani; M. Benedettini; C. S. Buemi; F. Bufano; A. Bulpitt; Robert Butora; D. Carey; Alessandro Costa; Lise Deharveng; A. M. di Giorgio; D. J. Eden; Ákos Hajnal; M. G. Hoare; Péter Kacsuk; P. Leto; Kenneth A. Marsh; P. Mège
We present a comprehensive statistical analysis of star-forming objects located in the vicinities of 1360 bubble structures throughout the Galactic plane and their local environments. The compilation of ~70 000 star-forming sources, found in the proximity of the ionized (Hii) regions and detected in both Hi-GAL and GLIMPSE surveys, provided a broad overview of the different evolutionary stages of star-formation in bubbles, from prestellar objects to more evolved young stellar objects (YSOs). Surface density maps of star-forming objects clearly reveal an evolutionary trend where more evolved star-forming objects (Class II YSO candidates) are found spatially located near the center, while younger star-forming objects are found at the edge of the bubbles. We derived dynamic ages for a subsample of 182 H ii regions for which kinematic distances and radio continuum flux measurements were available. We detect approximately 80% more star-forming sources per unit area in the direction of bubbles than in the surrounding fields. We estimate the clump formation efficiency (CFE) of Hi-GAL clumps in the direction of the shell of the bubbles to be ~15%, around twice the value of the CFE in fields that are not affected by feedback effects. We find that the higher values of CFE are mostly due to the higher CFE of protostellar clumps, in particular in younger bubbles, whose density of the bubble shells is higher. We argue that the formation rate from prestellar to protostellar phase is probably higher during the early stages of the (H ii) bubble expansion. Furthermore, we also find a higher fraction of massive YSOs (MYSOs) in bubbles at the early stages of expansion ( < 2 Myr) than older bubbles. Evaluation of the fragmentation time inside the shell of bubbles advocates the preexistence of clumps in the medium before the bubble expansion in order to explain the formation of MYSOs in the youngest H ii regions ( < 1 Myr), as supported by numerical simulations. Approximately 23% of the Hi-GAL clumps are found located in the direction of a bubble, with 15% for prestellar clumps and 41% for protostellar clumps. We argue that the high fraction of protostellar clumps may be due to the acceleration of the star-formation process cause by the feedback of the (Hii) bubbles.
Astronomy and Astrophysics | 2017
Hong-Li Liu; M. Figueira; A. Zavagno; T. Hill; N. Schneider; Alexander Men’shchikov; D. Russeil; F. Motte; J. Tigé; Lise Deharveng; L. D. Anderson; J. Z. Li; Yuefang Wu; Jing-Hua Yuan; M. Huang
Context. Triggered star formation around H ii regions could be an important process. The Galactic H ii region RCW 79 is a prototypical object for triggered high-mass star formation. Aims. We aim to obtain a census of the young stellar population observed at the edges of the H ii region and to determine the properties of the young sources in order to characterize the star formation processes that take place at the edges of this ionized region. Methods. We take advantage of Herschel data from the surveys HOBYS, “Evolution of Interstellar Dust”, and Hi-Gal to extract compact sources. We use the algorithm getsources . We complement the Herschel data with archival 2MASS, Spitzer , and WISE data to determine the physical parameters of the sources (e.g., envelope mass, dust temperature, and luminosity) by fitting the spectral energy distribution. Results. We created the dust temperature and column density maps along with the column density probability distribution function (PDF) for the entire RCW 79 region. We obtained a sample of 50 compact sources in this region, 96% of which are situated in the ionization-compressed layer of cold and dense gas that is characterized by the column density PDF with a double-peaked lognormal distribution. The 50 sources have sizes of ~ 0.1−0.4 pc with a typical value of ~ 0.2 pc, temperatures of ~ 11−26 K, envelope masses of ~ 6−760 M ⊙ , densities of ~ 0.1−44 × 10 5 cm -3 , and luminosities of ~ 19−12 712 L ⊙ . The sources are classified into 16 class 0, 19 intermediate, and 15 class I objects. Their distribution follows the evolutionary tracks in the diagram of bolometric luminosity versus envelope mass ( L bol − M env ) well. A mass threshold of 140 M ⊙ , determined from the L bol − M env diagram, yields 12 candidate massive dense cores that may form high-mass stars. The core formation efficiency (CFE) for the 8 massive condensations shows an increasing trend of the CFE with density. This suggests that the denser the condensation, the higher the fraction of its mass transformation into dense cores, as previously observed in other high-mass star-forming regions.
Publications of the Astronomical Society of Japan | 2018
Anthony Peter Whitworth; Oliver David Lomax; Scott Balfour; Pierre Mège; A. Zavagno; Lise Deharveng
We suggest that Bipolar H{\sc ii} Regions may be the aftermath of collisions between clouds. Such a collision will produce a shock-compressed layer, and a star cluster can then condense out of the dense gas near the centre of the layer. If the clouds are sufficiently massive, the star cluster is likely to contain at least one massive star, which emits ionising radiation, and excites an H{\sc ii} region, which then expands, sweeping up the surrounding neutral gas. Once most of the matter in the clouds has accreted onto the layer, expansion of the H{\sc ii} Region meets little resistance in directions perpendicular to the mid-plane of the layer, and so it expands rapidly to produce two lobes of ionised gas, one on each side of the layer. Conversely, in directions parallel to the mid-plane of the layer, expansion of the H{\sc ii} Region stalls due to the ram-pressure of the gas that continues to fall towards the star cluster from the outer parts of the layer; a ring of dense neutral gas builds up around the waist of the Bipolar H{\sc ii} Region, and may spawn a second generation of star formation. In this paper we present a dimensionless model for the flow of ionised gas in a Bipolar H{\sc ii} Region created according to the above scenario, and predict the characteristics of the resulting freefree continuum and recombination-line emission. This dimensionless model can be scaled to the physical parameters of any particular system. Our intention is that these predictions will be useful in testing the scenario outlined above, and thereby providing indirect support for the role of cloud/cloud collisions in triggering star formation.
Eas Publications Series | 2011
F. Wyrowski; F. Schuller; K. M. Menten; L. Bronfman; T. Henning; C. M. Walmsley; H. Beuther; Sylvain Bontemps; R. Cesaroni; Y. Contreras; Lise Deharveng; Guido Garay; Fabrice Herpin; B. Lefloch; H. Linz; Diego Mardones; V. Minier; S. Molinari; F. Motte; Q. Nguyen Luong; L.-Å. Nyman; V. Reveret; Christophe Risacher; D. Russeil; P. Schilke; N. Schneider; J. Tackenberg; L. Testi; T. Troost; T. Vasyunina
Submillimeter dust continuum emission traces high molecular column densities and, thus, dense cloud regions in which new stars are forming. Surveys of the Galactic plane in such emission have the potential of delivering an unbiased view of high-mass star formation throughout the Milky Way. The location of the APEX telescope on the Chajnantor plateau in Chile is ideally suited for mapping the inner Galaxy. ATLASGAL, The APEX Telescope Large Area Survey of the Galaxy at 870 μm, is a survey of the Galactic plane using the Large APEX Bolometer Camera (LABOCA), in the Galactic longitude and latitude ranges of ±60 and ±1.5°, respectively. This survey is providing an unbiased sample of cold dusty clumps in the Galaxy at submillimeter wavelength and a variety of molecular line follow-up observations have been started to characterize the physical and chemical conditions in the newly found clumps. Here, first results from this survey and its follow-up programs are described.
Astronomy and Astrophysics | 2018
M. R. Samal; Lise Deharveng; A. Zavagno; L. D. Anderson; S. Molinari; D. Russeil
Aims.We aim to identify bipolar Galactic HIIregions and to understand their parental cloud structures, morphologies, evolution, andimpact on the formation of new generations of stars. Methods.We use theSpitzer-GLIMPSE,Spitzer-MIPSGAL, andHerschel-Hi-GAL surveys to identify bipolar HIIregions and toexamine their morphologies. We search for their exciting star(s) using NIR data from the 2MASS, UKIDSS, and VISTA surveys.Massive molecular clumps are detected near these bipolar nebulae, and we estimate their temperatures, column densities, masses, anddensities. We locate Class 0/I young stellar objects (YSOs) in their vicinities using theSpitzerandHerschel-PACS emission. Results.Numerical simulations suggest bipolar HIIregions form and evolve in a two-dimensional flat- or sheet-like molecular cloud.We identified 16 bipolar nebulae in a zone of the Galactic plane between`±60◦and|b|< 1◦. This small number, when comparedwith the 1377 bubble HIIregions in the same area, suggests that most HIIregions form and evolve in a three-dimensional medium.We present the catalogue of the 16 bipolar nebulae and a detailed investigation for six of these. Our results suggest that these regionsformed in dense and flat structures that contain filaments. We find that bipolar HIIregions have massive clumps in their surroundings.The most compact and massive clumps are always located at the waist of the bipolar nebula, adjacent to the ionised gas. These massiveclumps are dense, with a mean density in the range of 105cm−3to several 106cm−3in their centres. Luminous Class 0/I sources ofseveral thousand solar luminosities, many of which have associated maser emission, are embedded inside these clumps. We suggestthat most, if not all, massive 0/I YSO formation has probably been triggered by the expansion of the central bipolar nebula, but theprocesses involved are still unknown. Modelling of such nebula is needed to understand the star formation processes at play