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The Astrophysical Journal | 2015

THE 2014 ALMA LONG BASELINE CAMPAIGN: FIRST RESULTS FROM HIGH ANGULAR RESOLUTION OBSERVATIONS TOWARD THE HL TAU REGION

Crystal Lee Brogan; Laura M. Pérez; Todd R. Hunter; William R. F. Dent; A. S. Hales; Richard E. Hills; Stuartt A. Corder; Edward B. Fomalont; C. Vlahakis; Yoshiharu Asaki; Denis Barkats; A. Hirota; J. A. Hodge; C. M. V. Impellizzeri; R. Kneissl; E. Liuzzo; R. Lucas; N. Marcelino; Satoki Matsushita; K. Nakanishi; N. Phillips; A. M. S. Richards; I. Toledo; R. Aladro; D. Broguiere; J. R. Cortes; Paulo C. Cortes; Daniel Espada; F. Galarza; D. Garcia Appadoo

We present Atacama Large Millimeter/submillimeter Array (ALMA) observations from the 2014 Long Baseline Campaign in dust continuum and spectral line emission from the HL Tau region. The continuum images at wavelengths of 2.9, 1.3, and 0.87 mm have unprecedented angular resolutions of 0. ′′ 075 (10 AU) to 0. ′′ 025 (3.5 AU), revealing an astonishing level of detail in the cir cumstellar disk surrounding the young solar analogue HL Tau, with a pattern of bright and dark rings observed at all wavelengths. By fitting ellipses to the most distinct rings, we measure precise values for the disk inclination (46.72 ◦ ± 0.05 ◦ ) and position angle (+138.02 ◦ ± 0.07 ◦ ). We obtain a high-fidelity image of the 1.0 mm spectral index (�), which ranges from � � 2.0 in the optically-thick central peak and two brightest ring s, increasing to 2.3-3.0 in the dark rings. The dark rings are not devoid of emission, and we estimate a grain emissivity index of 0.8 for the innermost dark ring and lower for subsequent dark rings, consistent with some degree of grain growth and evolution. Additional clues that the rings arise from planet formation incl ude an increase in their central offsets with radius and the presence of numerous orbital resonances. At a resolution of 35 AU, we resolve the molecular component of the disk in HCO + (1-0) which exhibits a pattern over LSR velocities from 2-12 km s -1 consistent with Keplerian motion around a �1.3M⊙ star, although complicated by absorption at low blue-shifted velocities. We also serendipitously detect and resolve the nearby protost ars XZ Tau (A/B) and LkH�358 at 2.9 mm. Subject headings: stars: individual (HL Tau, XZ Tau, LkH�358) — protoplanetary disks — stars: formation — submillimeter: planetary systems — techniques: interferometric


Astronomy and Astrophysics | 2013

Herschel view of the Taurus B211/3 filament and striations: Evidence of filamentary growth?

P. Palmeirim; P. André; Jason M. Kirk; Derek Ward-Thompson; D. Arzoumanian; V. Könyves; P. Didelon; N. Schneider; M. Benedettini; Sylvain Bontemps; J. Di Francesco; D. Elia; Matthew Jason Griffin; M. Hennemann; T. Hill; P. G. Martin; A. Men’shchikov; S. Molinari; F. Motte; Q. Nguyen Luong; D. Nutter; Nicolas Peretto; S. Pezzuto; A. Roy; K. L. J. Rygl; L. Spinoglio; G. L. White

We present first results from the Herschel Gould Belt survey for the B211/L1495 region in the Taurus molecular cloud. Thanks to their high sensitivity and dynamic range, the Herschel images reveal the structure of the dense, star-forming filament B211 with unprecedented detail, along with the presence of striations perpendicular to the filament and generally oriented along the magnetic field direction as traced by optical polarization vectors. Based on the column density and dust temperature maps derived from the Herschel data, we find that the radial density profile of the B211 filament approaches power-law behavior, ρ ∝ r−2.0± 0.4, at large radii and that the temperature profile exhibits a marked drop at small radii. The observed density and temperature profiles of the B211 filament are in good agreement with a theoretical model of a cylindrical filament undergoing gravitational contraction with a polytropic equation of state: P ∝ ργ and T ∝ ργ−1, with γ = 0.97 ± 0.01 < 1 (i.e., not strictly isothermal). The morphology of the column density map, where some of the perpendicular striations are apparently connected to the B211 filament, further suggests that the material may be accreting along the striations onto the main filament. The typical velocities expected for the infalling material in this picture are ~0.5–1 km s-1, which are consistent with the existing kinematical constraints from previous CO observations.


Astronomy and Astrophysics | 2010

The Aquila prestellar core population revealed by Herschel

V. Könyves; P. André; A. Men'shchikov; N. Schneider; D. Arzoumanian; Sylvain Bontemps; M. Attard; F. Motte; P. Didelon; A. Maury; Alain Abergel; B. Ali; J.-P. Baluteau; J.-Ph. Bernard; L. Cambrésy; P. Cox; J. Di Francesco; A. M. di Giorgio; Matthew Joseph Griffin; Peter Charles Hargrave; M. Huang; Jason M. Kirk; J. Z. Li; Peter G. Martin; V. Minier; S. Molinari; G. Olofsson; S. Pezzuto; D. Russeil; Helene Roussel

The origin and possible universality of the stellar initial mass function (IMF) is a major issue in astrophysics. One of the main objectives of the Herschel Gould Belt Survey is to clarify the link between the prestellar core mass function (CMF) and the IMF. We present and discuss the core mass function derived from Herschel data for the large population of prestellar cores discovered with SPIRE and PACS in the Aquila Rift cloud complex at d ~ 260 pc. We detect a total of 541 starless cores in the entire ~11 deg^2 area of the field imaged at 70-500 micron with SPIRE/PACS. Most of these cores appear to be gravitationally bound, and thus prestellar in nature. Our Herschel results confirm that the shape of the prestellar CMF resembles the stellar IMF, with much higher quality statistics than earlier submillimeter continuum ground-based surveys.


Astronomy and Astrophysics | 2012

Cluster-formation in the Rosette molecular cloud at the junctions of filaments (Corrigendum)

N. Schneider; T. Csengeri; M. Hennemann; F. Motte; P. Didelon; Christoph Federrath; Sylvain Bontemps; J. Di Francesco; D. Arzoumanian; V. Minier; P. André; T. Hill; A. Zavagno; Q. Nguyen-Luong; M. Attard; J.-Ph. Bernard; D. Elia; C. Fallscheer; Matthew Joseph Griffin; Jason M. Kirk; Ralf S. Klessen; V. Könyves; P. G. Martin; A. Men'shchikov; P. Palmeirim; Nicolas Peretto; M. Pestalozzi; D. Russeil; S. Sadavoy; T. Sousbie

For many years feedback processes generated by OB-stars in molecular clouds, including expanding ionization fronts, stellar winds, or UV-radiation, have been proposed to trigger subsequent star formation. However, hydrodynamic models including radiation and gravity show that UV-illumination has little or no impact on the global dynamical evolution of the cloud. The Rosette molecular cloud, irradiated by the NGC2244 cluster, is a template region for triggered star-formation, and we investigated its spatial and density structure by applying a curvelet analysis, a filament-tracing algorithm (DisPerSE), and probability density functions (PDFs) on Herschel column density maps, obtained within the HOBYS key program. The analysis reveals not only the filamentary structure of the cloud but also that all known infrared clusters except one lie at junctions of filaments, as predicted by turbulence simulations. The PDFs of sub-regions in the cloud show systematic differences. The two UV-exposed regions have a double-peaked PDF we interprete as caused by shock compression. The deviations of the PDF from the log-normal shape typically associated with low- and high-mass star-forming regions at Av~3-4m and 8-10m, respectively, are found here within the very same cloud. This shows that there is no fundamental difference in the density structure of low- and high-mass star-forming regions. We conclude that star-formation in Rosette - and probably in high-mass star-forming clouds in general - is not globally triggered by the impact of UV-radiation. Moreover, star formation takes place in filaments that arose from the primordial turbulent structure built up during the formation of the cloud. Clusters form at filament mergers, but star formation can be locally induced in the direct interaction zone between an expanding HII--region and the molecular cloud.


Astronomy and Astrophysics | 2010

Filamentary structures and compact objects in the Aquila and Polaris clouds observed by Herschel

A. Men'shchikov; P. André; P. Didelon; V. Könyves; N. Schneider; F. Motte; Sylvain Bontemps; D. Arzoumanian; M. Attard; Alain Abergel; J.-P. Baluteau; J.-Ph. Bernard; L. Cambrésy; P. Cox; J. Di Francesco; A. M. di Giorgio; Matthew Joseph Griffin; Peter Charles Hargrave; M. Huang; Jason M. Kirk; J. Z. Li; P. G. Martin; V. Minier; M.-A. Miville-Deschênes; S. Molinari; G. Olofsson; S. Pezzuto; H. Roussel; D. Russeil; P. Saraceno

Our PACS and SPIRE images of the Aquila Rift and part of the Polaris Flare regions, taken during the science demonstration phase of Herschel discovered fascinating, omnipresent filamentary structures that appear to be physically related to compact cores. We briefly describe a new multi-scale, multi-wavelength source extraction method used to detect objects and measure their parameters in our Herschel images. All of the extracted starless cores (541 in Aquila and 302 in Polaris) appear to form in the long and very narrow filaments. With its combination of the far-IR resolution and sensitivity, Herschel directly reveals the filaments in which the dense cores are embedded; the filaments are resolved and have deconvolved widths of 35 arcsec in Aquila and 59 arcsec in Polaris (9000 AU in both regions). Our first results of observations with Herschel enable us to suggest that in general dense cores may originate in a process of fragmentation of complex networks of long, thin filaments, likely formed as a result of an interplay between gravity, interstellar turbulence, and magnetic fields. To unravel the roles of the processes, one has to obtain additional kinematic and polarization information; these follow-up observations are planned.


Astronomy and Astrophysics | 2010

Initial highlights of the HOBYS key program, the Herschel imaging survey of OB young stellar objects

F. Motte; A. Zavagno; Sylvain Bontemps; N. Schneider; M. Hennemann; J. Di Francesco; P. André; P. Saraceno; Matthew Joseph Griffin; A. Marston; Derek Ward-Thompson; G. J. White; V. Minier; A. Men'shchikov; T. Hill; Alain Abergel; L. D. Anderson; H. Aussel; Zoltan Balog; J.-P. Baluteau; J.-Ph. Bernard; P. Cox; T. Csengeri; L. Deharveng; P. Didelon; A. M. di Giorgio; Peter Charles Hargrave; M. Huang; Jason M. Kirk; S. J. Leeks

We present the initial highlights of the HOBYS key program, which are based on Herschel images of the Rosette molecular complex and maps of the RCW120 H ii region. Using both SPIRE at 250/350/500 μm and PACS at 70/160 μm or 100/160 μm, the HOBYS survey provides an unbiased and complete census of intermediate- to high-mass young stellar objects, some of which are not detected by Spitzer. Key core properties, such as bolometric luminosity and mass (as derived from spectral energy distributions), are used to constrain their evolutionary stages. We identify a handful of high-mass prestellar cores and show that their lifetimes could be shorter in the Rosette molecular complex than in nearby low-mass star-forming regions. We also quantify the impact of expanding H ii regions on the star formation process acting in both Rosette and RCW 120.


The Astrophysical Journal | 2013

WHAT DETERMINES THE DENSITY STRUCTURE OF MOLECULAR CLOUDS? A CASE STUDY OF ORION B WITH HERSCHEL ∗

N. Schneider; P. André; V. Könyves; Sylvain Bontemps; F. Motte; Christoph Federrath; Derek Ward-Thompson; D. Arzoumanian; M. Benedettini; E. Bressert; P. Didelon; J. Di Francesco; Matthew Joseph Griffin; M. Hennemann; T. Hill; P. Palmeirim; S. Pezzuto; Nicolas Peretto; A. Roy; K. L. J. Rygl; L. Spinoglio; G. J. White

A key parameter to the description of all star formation processes is the density structure of the gas. In this letter, we make use of probability distribution functions (PDFs) of Herschel column density maps of Orion B, Aquila, and Polaris, obtained with the Herschel Gould Belt survey (HGBS). We aim to understand which physical processes influence the PDF shape, and with which signatures. The PDFs of Orion B (Aquila) show a lognormal distribution for low column densities until Av 3 (6), and a power-law tail for high column densities, consistent with a rho r^-2 profile for the equivalent spherical density distribution. The PDF of Orion B is broadened by external compression due to the nearby OB stellar aggregates. The PDF of a quiescent subregion of the non-star-forming Polaris cloud is nearly lognormal, indicating that supersonic turbulence governs the density distribution. But we also observe a deviation from the lognormal shape at Av>1 for a subregion in Polaris that includes a prominent filament. We conclude that (i) the point where the PDF deviates from the lognormal form does not trace a universal Av-threshold for star formation, (ii) statistical density fluctuations, intermittency and magnetic fields can cause excess from the lognormal PDF at an early cloud formation stage, (iii) core formation and/or global collapse of filaments and a non-isothermal gas distribution lead to a power-law tail, and (iv) external compression broadens the column density PDF, consistent with numerical simulations.A key parameter to the description of all star formation processes is the density structure of the gas. In this Letter, we make use of probability distribution functions (PDFs) of Herschel column density maps of Orion B, Aquila, and Polaris, obtained with the Herschel Gould Belt survey (HGBS). We aim to understand which physical processes influence the PDF shape, and with which signatures. The PDFs of Orion B (Aquila) show a lognormal distribution for low column densities until A V 3 (6), and a power-law tail for high column densities, consistent with a ρr -2 profile for the equivalent spherical density distribution. The PDF of Orion B is broadened by external compression due to the nearby OB stellar aggregates. The PDF of a quiescent subregion of the non-star-forming Polaris cloud is nearly lognormal, indicating that supersonic turbulence governs the density distribution. But we also observe a deviation from the lognormal shape at A V > 1 for a subregion in Polaris that includes a prominent filament. We conclude that (1) the point where the PDF deviates from the lognormal form does not trace a universal A V -threshold for star formation, (2) statistical density fluctuations, intermittency, and magnetic fields can cause excess from the lognormal PDF at an early cloud formation stage, (3) core formation and/or global collapse of filaments and a non-isothermal gas distribution lead to a power-law tail, and (4) external compression broadens the column density PDF, consistent with numerical simulations.


Astronomy and Astrophysics | 2012

The spine of the swan: a Herschel study of the DR21 ridge and filaments in Cygnus X

M. Hennemann; F. Motte; N. Schneider; P. Didelon; T. Hill; D. Arzoumanian; Sylvain Bontemps; T. Csengeri; P. André; V. Könyves; F. Louvet; A. Marston; A. Men’shchikov; V. Minier; Q. Nguyen Luong; P. Palmeirim; Nicolas Peretto; Marc Sauvage; A. Zavagno; L. D. Anderson; J.-Ph. Bernard; J. Di Francesco; D. Elia; J. Z. Li; P. G. Martin; S. Molinari; S. Pezzuto; D. Russeil; K. L. J. Rygl; E. Schisano

In order to characterise the cloud structures responsible for the formation of high-mass stars, we present Herschel observations of the DR21 environment. Maps of the column density and dust temperature unveil the structure of the DR21 ridge and several connected filaments. The ridge has column densities larger than 1e23/cm^2 over a region of 2.3 pc^2. It shows substructured column density profiles and branching into two major filaments in the north. The masses in the studied filaments range between 130 and 1400 Msun whereas the mass in the ridge is 15000 Msun. The accretion of these filaments onto the DR21 ridge, suggested by a previous molecular line study, could provide a continuous mass inflow to the ridge. In contrast to the striations seen in e.g., the Taurus region, these filaments are gravitationally unstable and form cores and protostars. These cores formed in the filaments potentially fall into the ridge. Both inflow and collisions of cores could be important to drive the observed high-mass star formation. The evolutionary gradient of star formation running from DR21 in the south to the northern branching is traced by decreasing dust temperature. This evolution and the ridge structure can be explained by two main filamentary components of the ridge that merged first in the south.


Astronomy and Astrophysics | 2010

The Herschel ? first look at protostars in the Aquila Rift ??

Sylvain Bontemps; P. André; V. Könyves; A. Men'shchikov; N. Schneider; A. Maury; Nicolas Peretto; D. Arzoumanian; M. Attard; F. Motte; V. Minier; P. Didelon; P. Saraceno; Alain Abergel; J.-P. Baluteau; J.-Ph. Bernard; L. Cambrésy; P. Cox; J. Di Francesco; A. M. Di Giorgo; Matthew Joseph Griffin; Peter Charles Hargrave; M. Huang; Jason M. Kirk; J. Z. Li; P. G. Martin; Bruno Merín; S. Molinari; G. Olofsson; S. Pezzuto

As part of the science demonstration phase of the Herschel mission of the Gould Belt Key Program, the Aquila Rift molecular complex has been observed. The complete ~ 3.3deg x 3.3deg imaging with SPIRE 250/350/500 micron and PACS 70/160 micron allows a deep investigation of embedded protostellar phases, probing of the dust emission from warm inner regions at 70 and 160 micron to the bulk of the cold envelopes between 250 and 500 micron. We used a systematic detection technique operating simultaneously on all Herschel bands to build a sample of protostars. Spectral energy distributions are derived to measure luminosities and envelope masses, and to place the protostars in an M_env - L_bol evolutionary diagram. The spatial distribution of protostars indicates three star-forming sites in Aquila, with W40/Sh2-64 HII region by far the richest. Most of the detected protostars are newly discovered. For a reduced area around the Serpens South cluster, we could compare the Herschel census of protostars with Spitzer results. The Herschel protostars are younger than in Spitzer with 7 Class 0 YSOs newly revealed by Herschel. For the entire Aquila field, we find a total of ~ 45-60 Class 0 YSOs discovered by Herschel. This confirms the global statistics of several hundred Class~0 YSOs that should be found in the whole Gould Belt survey.


Astronomy and Astrophysics | 2015

A census of dense cores in the Aquila cloud complex: SPIRE/PACS observations from the Herschel Gould Belt survey

V. Könyves; P. André; A. Men'shchikov; P. Palmeirim; D. Arzoumanian; N. Schneider; A. Roy; P. Didelon; A. Maury; Yoshito Shimajiri; J. Di Francesco; Sylvain Bontemps; Nicolas Peretto; M. Benedettini; J.-Ph. Bernard; D. Elia; Matthew James Griffin; T. Hill; Jason Matthew Kirk; B. Ladjelate; Kenneth A. Marsh; P. G. Martin; F. Motte; Q. Nguyen Luong; S. Pezzuto; H. Roussel; K. L. J. Rygl; S. Sadavoy; E. Schisano; L. Spinoglio

We present and discuss the results of the Herschel Gould Belt survey (HGBS) observations in an ~11 deg2 area of the Aquila molecular cloud complex at d ~ 260 pc, imaged with the SPIRE and PACS photometric cameras in parallel mode from 70 μm to 500 μm. Using the multi-scale, multi-wavelength source extraction algorithm getsources, we identify a complete sample of starless dense cores and embedded (Class 0-I) protostars in this region, and analyze their global properties and spatial distributions. We find a total of 651 starless cores, ~60% ± 10% of which are gravitationally bound prestellar cores, and they will likely form stars inthe future. We also detect 58 protostellar cores. The core mass function (CMF) derived for the large population of prestellar cores is very similar in shape to the stellar initial mass function (IMF), confirming earlier findings on a much stronger statistical basis and supporting the view that there is a close physical link between the stellar IMF and the prestellar CMF. The global shift in mass scale observed between the CMF and the IMF is consistent with a typical star formation efficiency of ~40% at the level of an individual core. By comparing the numbers of starless cores in various density bins to the number of young stellar objects (YSOs), we estimate that the lifetime of prestellar cores is ~1 Myr, which is typically ~4 times longer than the core free-fall time, and that it decreases with average core density. We find a strong correlation between the spatial distribution of prestellar cores and the densest filaments observed in the Aquila complex. About 90% of the Herschel-identified prestellar cores are located above a background column density corresponding to AV ~ 7, and ~75% of them lie within filamentary structures with supercritical masses per unit length ≳16 M⊙/pc. These findings support a picture wherein the cores making up the peak of the CMF (and probably responsible for the base of the IMF) result primarily from the gravitational fragmentation of marginally supercritical filaments. Given that filaments appear to dominate the mass budget of dense gas at AV> 7, our findings also suggest that the physics of prestellar core formation within filaments is responsible for a characteristic “efficiency” for the star formation process in dense gas.

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Sylvain Bontemps

Centre national de la recherche scientifique

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N. Schneider

Centre national de la recherche scientifique

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