J. A. D. L. Blommaert
Katholieke Universiteit Leuven
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Astronomy and Astrophysics | 2010
A. Poglitsch; C. Waelkens; N. Geis; Helmut Feuchtgruber; B. Vandenbussche; L. Rodriguez; O. Krause; E. Renotte; C. Van Hoof; P. Saraceno; J. Cepa; Franz Kerschbaum; P. Agnèse; B. Ali; B. Altieri; Paola Andreani; J.-L. Augueres; Zoltan Balog; L. Barl; O. H. Bauer; N. Belbachir; M. Benedettini; N. Billot; Olivier Boulade; Horst Bischof; J. A. D. L. Blommaert; E. Callut; C. Cara; R. Cerulli; D. Cesarsky
The Photodetector Array Camera and Spectrometer (PACS) is one of the three science instruments on ESAs far infrared and submil- limetre observatory. It employs two Ge:Ga photoconductor arrays (stressed and unstressed) with 16 × 25 pixels, each, and two filled silicon bolometer arrays with 16 × 32 and 32 × 64 pixels, respectively, to perform integral-field spectroscopy and imaging photom- etry in the 60−210 μm wavelength regime. In photometry mode, it simultaneously images two bands, 60−85 μ mo r 85−125 μ ma nd 125−210 μm, over a field of view of ∼1.75 � × 3.5 � , with close to Nyquist beam sampling in each band. In spectroscopy mode, it images afi eld of 47 �� × 47 �� , resolved into 5 × 5 pixels, with an instantaneous spectral coverage of ∼ 1500 km s −1 and a spectral resolution of ∼175 km s −1 . We summarise the design of the instrument, describe observing modes, calibration, and data analysis methods, and present our current assessment of the in-orbit performance of the instrument based on the performance verification tests. PACS is fully operational, and the achieved performance is close to or better than the pre-launch predictions.
The Astrophysical Journal | 2012
Matthew William L. Smith; Stephen Anthony Eales; Haley Louise Gomez; Julia Roman-Duval; J. Fritz; R. Braun; M. Baes; G. J. Bendo; J. A. D. L. Blommaert; M. Boquien; A. Boselli; D. L. Clements; A. Cooray; Luca Cortese; I. De Looze; G.P. Ford; Walter Kieran Gear; Gianfranco Gentile; Karl D. Gordon; Jason M. Kirk; V. Lebouteiller; S. Madden; E. Mentuch; B. O’Halloran; Mat Page; B. Schulz; L. Spinoglio; J. Verstappen; C. D. Wilson; David Allan Thilker
We present an analysis of the dust and gas in Andromeda, using Herschel images sampling the entire far-infrared peak. We fit a modified-blackbody model to similar to 4000 quasi-independent pixels with spatial resolution of similar to 140 pc and find that a variable dust-emissivity index (beta) is required to fit the data. We find no significant long-wavelength excess above this model, suggesting there is no cold dust component. We show that the gas-to-dust ratio varies radially, increasing from similar to 20 in the center to similar to 70 in the star-forming ring at 10 kpc, consistent with the metallicity gradient. In the 10 kpc ring the average beta is similar to 1.9, in good agreement with values determined for the Milky Way (MW). However, in contrast to the MW, we find significant radial variations in beta, which increases from 1.9 at 10 kpc to similar to 2.5 at a radius of 3.1 kpc and then decreases to 1.7 in the center. The dust temperature is fairly constant in the 10 kpc ring (ranging from 17 to 20 K), but increases strongly in the bulge to similar to 30 K. Within 3.1 kpc we find the dust temperature is highly correlated with the 3.6 mu m flux, suggesting the general stellar population in the bulge is the dominant source of dust heating there. At larger radii, there is a weak correlation between the star formation rate and dust temperature. We find no evidence for “dark gas” in M31 in contrast to recent results for the MW. Finally, we obtained an estimate of the CO X-factor by minimizing the dispersion in the gas-to-dust ratio, obtaining a value of (1.9 +/- 0.4) x 10(20) cm(-2) [K km s(-1)](-1).
Monthly Notices of the Royal Astronomical Society | 2006
Albert A. Zijlstra; Mikako Matsuura; Peter R. Wood; G. C. Sloan; E. Lagadec; Jacco Th. van Loon; M. A. T. Groenewegen; M. W. Feast; John W. Menzies; Patricia A. Whitelock; J. A. D. L. Blommaert; M-R.L. Cioni; Harm Jan Habing; Sacha Hony; C. Loup; L. B. F. M. Waters
We present a Spitzer Space Telescopespectroscopic survey of mass-losing carbon stars (and one oxygen-rich star) in the Large Magellanic Cloud. The stars represent the superwind phase on the Asymptotic Giant Branch, which forms a major source of dust for the interstellar medium in galaxies. The spectra cover the wavelength range 5‐38� m. They show varying combinations of dust continuum, dust emission features (SiC, MgS) and molecular absorption bands (C2H2, HCN). A set of four narrow bands, dubbed the Manchester system, is used to define the infrared continuum for dusty carbon stars. The r elations between the continuum colours and the strength of the dust and molecular features are studied, and are compared to Galactic stars of similar colours. The circumstellar 7-� m C2H2 band is found to be stronger at lower metallicity, from a comparison of stars in the Galaxy, the LMC and the SMC. This is explained by dredge-up of carbon, causing higher C/O ratios at low metallicity (less O). A possible 10-� m absorption feature seen in our spectra may be due to C3. This band has also been identified with interstellar silicate or silicon-nitr ite dust. We investigate the strength and central wavelength of the SiC and MgS dust bands as function of colour and metallicity. The line-to-continuum ratio of these bands shows some indication of being lower at low metallicity. The MgS band is only seen at dust temperatures below 600 K. We discuss the selection of carbon versus oxygen-rich AGB stars using the J K vs. K A colours, and show that these colours are relatively insensitive to chemical type. Metal -poor carbon stars form amorphous carbon dust from self-produced carbon. This type of dust forms more readily in the presence of a higher C/O ratio. Low metallicity carbon dust may contain a smaller fraction of SiC and MgS constituents, which do depend on metallicity. The formation efficiency of oxygen-rich dust depends more strongly on metallicity. We suggest that in lower-metallicity environments, the dust input into the Interstellar Medium by AGB stars is efficient but may be strongly biassed towards carbonaceous dust, as compared to the Galaxy.
Astronomy and Astrophysics | 2012
B. Acke; M. Min; C. Dominik; B. Vandenbussche; B. Sibthorpe; C. Waelkens; G. Olofsson; P. Degroote; K. Smolders; E. Pantin; M. J. Barlow; J. A. D. L. Blommaert; Alexis Brandeker; W. De Meester; W. R. F. Dent; Katrina Exter; J. Di Francesco; M. Fridlund; Walter Kieran Gear; Adrian M. Glauser; J. S. Greaves; Paul M. Harvey; Th. Henning; M. R. Hogerheijde; Wayne S. Holland; R. Huygen; R. J. Ivison; C. Jean; R. Liseau; David A. Naylor
Context. Fomalhaut is a young (2 ± 1 × 10 8 years), nearby (7.7 pc), 2 Mstar that is suspected to harbor an infant planetary system, interspersed with one or more belts of dusty debris. Aims. We present far-infrared images obtained with the Herschel Space Observatory with an angular resolution between 5.7 �� and 36.7 �� at wave- lengths between 70 μm and 500 μm. The images show the main debris belt in great detail. Even at high spatial resolution, the belt appears smooth. The region in between the belt and the central star is not devoid of material; thermal emission is observed here as well. Also at the location of the star, excess emission is detected. We aim to construct a consistent image of the Fomalhaut system. Methods. We use a dynamical model together with radiative-transfer tools to derive the parameters of the debris disk. We include detailed models of the interaction of the dust grains with radiation, for both the radiation pressure and the temperature determination. Comparing these models to the spatially resolved temperature information contained in the images allows us to place strong constraints on the presence of grains that will be blown out of the system by radiation pressure. We use this to derive the dynamical parameters of the system. Results. The appearance of the belt points toward a remarkably active system in which dust grains are produced at a very high rate by a collisional cascade in a narrow region filled with dynamically excited planetesimals. Dust particles with sizes below the blow-out size are abundantly present. The equivalent of 2000 one-km-sized comets are destroyed every day, out of a cometary reservoir amounting to 110 Earth masses. From compar- ison of their scattering and thermal properties, we find evidence that the dust grains are fluffy aggregates, which indicates a cometary origin. The excess emission at the location of the star may be produced by hot dust with a range of temperatures, but may also be due to gaseous free-free emission from a stellar wind.
Monthly Notices of the Royal Astronomical Society | 2007
E. Lagadec; Albert A. Zijlstra; G. C. Sloan; Mikako Matsuura; Peter R. Wood; Jacco Th. van Loon; Gregory J. Harris; J. A. D. L. Blommaert; Sacha Hony; M. A. T. Groenewegen; M. W. Feast; Patricia A. Whitelock; John W. Menzies; M-R.L. Cioni
We present Spitzer Space telescopespectroscopic observations of 14 carbon-rich AGB stars in the Small Magellanic Cloud. SiC dust is seen in most of the carbon-rich stars but it is weak compared to LMC stars. The SiC feature is strong only for stars with significant dust excess, opposite to what is observed for Galactic stars. We argue that in the SMC, SiC forms at lower temperature than graphite dust, whereas the reverse situation occurs in the Galaxy where SiC condenses at higher temperatures and forms first. Dust input into the interstellar medium by AGB stars consists mostly of carbonaceous dust, with little SiC or silicate dust. Only the two coolest stars show a 30-micron band due to MgS dust. We suggest that this is due to the fact that, in the SMC, mass-losing AGB stars generally have low circumstellar (dust) optical depth and therefore effective heating of dust by the central star does not allow temperatures below the 650 K necessary for MgS to exist as a solid. Gas phase C2H2 bands are stronger in the SMC than in the LMC or Galaxy. This is attributed to an increasing C/O ratio at low metallicity. We present a colour-colour diagram based on Spitzer IRAC and MIPS colours to discriminate between O- and C-rich stars. We show that AGB stars in the SMC become carbon stars early in the thermal-pulsing AGB evolution, and remain optically visible for � 6 × 10 5 yr. For the LMC, this lifetime is � 3 × 10 5 yr. The superwind phase traced with Spitzer lasts for � 10 4 yr. Spitzer spectra of a K supergiant and a compact HII region are also given.
Nature | 2010
Leen Decin; M. Agúndez; M. J. Barlow; F. Daniel; J. Cernicharo; R. Lombaert; E. De Beck; P. Royer; B. Vandenbussche; R. Wesson; E. T. Polehampton; J. A. D. L. Blommaert; W. De Meester; K. Exter; Helmut Feuchtgruber; Walter Kieran Gear; Haley Louise Gomez; M. A. T. Groenewegen; M. Guélin; Peter Charles Hargrave; R. Huygen; P. Imhof; R. J. Ivison; C. Jean; C. Kahane; F. Kerschbaum; S. J. Leeks; T. Lim; Mikako Matsuura; G. Olofsson
The detection of circumstellar water vapour around the ageing carbon star IRC +10216 challenged the current understanding of chemistry in old stars, because water was predicted to be almost absent in carbon-rich stars. Several explanations for the water were postulated, including the vaporization of icy bodies (comets or dwarf planets) in orbit around the star, grain surface reactions, and photochemistry in the outer circumstellar envelope. With a single water line detected so far from this one carbon-rich evolved star, it is difficult to discriminate between the different mechanisms proposed. Here we report the detection of dozens of water vapour lines in the far-infrared and sub-millimetre spectrum of IRC +10216 using the Herschel satellite. This includes some high-excitation lines with energies corresponding to ∼1,000 K, which can be explained only if water is present in the warm inner sooty region of the envelope. A plausible explanation for the warm water appears to be the penetration of ultraviolet photons deep into a clumpy circumstellar envelope. This mechanism also triggers the formation of other molecules, such as ammonia, whose observed abundances are much higher than hitherto predicted.
Astronomy and Astrophysics | 2005
M. A. T. Groenewegen; J. A. D. L. Blommaert
The 222 000 I-band light curves of variable stars detected by the OGLE-II survey in the direction of the Galactic Bulge have been fitted and also correlated with the DENIS and 2MASS all-sky release databases and with lists of known objects. Lightcurves and the results of the lightcurve fitting (periods and amplitudes) and DENIS and 2MASS data are presented for 2691 objects with I-band semi-amplitude larger than 0.45 mag, corresponding to classical Mira variables. That the Mira period distribution of 6 fields at similar longitude but spanning latitudes from -1.2 to -5.8 are statistically indistinguishable indicates similar populations with initial masses of 1.5-2 M ○. , corresponding to ages of 1-3 Gyr. A field at similar longitude at b = -0.05 from Glass et al. (2001, MNRAS, 321, 77; erratum: 2002, MNRAS, 336, 1390) does show a significantly different period distribution, indicating the presence of a younger population of 2.5-3 M ○. and ages below 1 Gyr. The K-band period-luminosity relation is presented for the whole sample and for sub-fields. The zero point depends on Galactic longitude. Simulations are carried out to show that the observed dependence of the zero point with l, and the number of stars per field are naturally explained using the model of disk and bulge stars of Binney et al. (1997, MNRAS, 288, 365), for a viewing angle (major-axis Bar - axis perpendicular to the line-of-sight to the Galactic Centre) of 43 ± 17 degrees. The simulations also show that biases in the observed zero point are small, <0.02 mag. A comparison is made with similar objects in the Magellanic Clouds. The slope of the PL-relation in the Bulge and the MCs agree within the errorbars. Assuming the zero point does not depend on metallicity, distance modulus difference of 3.72 between Bulge and LMC is derived. This implies a LMC DM of 18.21 for an assumed distance to the Galactic Centre (GC) of 7.9 kpc, or, assuming a LMC DM of 18.50, a distance to the GC of 9.0 kpc. From the results in Groenewegen (2004, A&A, 425, 595) it is found for carbon-rich Miras that the PL-relation implies a relative SMC-LMC DM of 0.38, assuming no metallicity dependence. This is somewhat smaller than the often quoted value near 0.50. Following theoretical work by Wood (1990, in From Miras to Planetary Nebulae, ed. M. 0. Mennessier, & A. Omont (Gif-sur-Yvette: Editions Frontieres), 67) a metallicity term of the form M K ∼ log Z is introduced. If a relative SMC-LMC DM of 0.50 is imposed, β = 0.4 is required, and for that value the distance to the GC becomes 8.6 ± 0.7 kpc (for a LMC DM of 18.50), within the errorbar of the geometric determination of 7.9 ± 0.4 kpc. An independent estimate leads to a distance estimate to the GC of 8.8 ± 0.4 kpc.
The Astrophysical Journal | 2001
C. Alard; J. A. D. L. Blommaert; Catherine J. Cesarsky; N. Epchtein; Marcello Felli; P. Fouqué; Shashikiran Ganesh; Paul Gatenby; Gerard Gilmore; I. S. Glass; Harm Jan Habing; A. Omont; M. Perault; Stephan D. Price; A. C. Robin; Mathias Schultheis; Gerard Simon; Jacco Th. van Loon; C. Alcock; Robyn A. Allsman; David Randall Alves; Tim Axelrod; Andrew Cameron Becker; D. P. Bennett; Kem Holland Cook; Andrew J. Drake; Kenneth C. Freeman; Marla Geha; Kim Griest; M J Lehner
By cross-correlating the results of two recent large-scale surveys, the general properties of a well-defined sample of semiregular variable stars have been determined. ISOGAL mid-infrared photometry (7 and 15 ?m) and MACHO V and R light curves are assembled for approximately 300 stars in the Baades windows of low extinction toward the Galactic bulge. These stars are mainly giants of late M spectral type, evolving along the asymptotic giant branch (AGB). They are found to possess a wide and continuous distribution of pulsation periods and to obey an approximate log P-Mbol relation or set of such relations. Approximate mass-loss rates in the range of ~1 ? 10-8 to 5 ? 10-7 M? yr-1 are derived from ISOGAL mid-infrared photometry and models of stellar spectra adjusted for the presence of optically thin circumstellar silicate dust. Mass-loss rates depend on luminosity and pulsation period. Some stars lose mass as rapidly as short-period Mira variables but do not show Mira-like amplitudes. A period of 70 days or longer is a necessary but not sufficient condition for mass loss to occur. For AGB stars in the mass-loss ranges that we observe, the functional dependence of mass-loss rate on temperature and luminosity can be expressed as T?L?, where ? = -8.80 and ? = +1.74, in agreement with recent theoretical predictions. If we include our mass-loss rates with a sample of extreme mass-losing AGB stars in the Large Magellanic Cloud and ignore T as a variable, we get the general result for AGB stars that L2.7, valid for AGB stars with 10-8 < < 10-4 M? yr-1.
Astronomy and Astrophysics | 2010
E. Lellouch; Paul Hartogh; Helmut Feuchtgruber; B. Vandenbussche; T. de Graauw; R. Moreno; C. Jarchow; T. Cavalié; Glenn S. Orton; M. Banaszkiewicz; M. I. Blecka; Dominique Bockelee-Morvan; Jacques Crovisier; Thérèse Encrenaz; T. Fulton; M. Küppers; L. M. Lara; Dariusz C. Lis; Alexander S. Medvedev; Miriam Rengel; Hideo Sagawa; B. M. Swinyard; S. Szutowicz; F. Bensch; Edwin A. Bergin; F. Billebaud; N. Biver; Geoffrey A. Blake; J. A. D. L. Blommaert; J. Cernicharo
We report on the initial analysis of a Herschel-PACS full range spectrum of Neptune, covering the 51–220 μm range with a mean resolving power of ~3000, and complemented by a dedicated observation of CH_4 at 120 μm. Numerous spectral features due to HD (R(0) and R(1)), H_(2)O, CH_4, and CO are present, but so far no new species have been found. Our results indicate that (i) Neptunes mean thermal profile is warmer by ~3 K than inferred from the Voyager radio-occultation; (ii) the D/H mixing ratio is (4.5 ± 1) × 10^(-5), confirming the enrichment of Neptune in deuterium over the protosolar value (~2.1 × 10^(-5)); (iii) the CH_4 mixing ratio in the mid stratosphere is (1.5 ± 0.2) × 10^(-3), and CH_4 appears to decrease in the lower stratosphere at a rate consistent with local saturation, in agreement with the scenario of CH_4 stratospheric injection from Neptunes warm south polar region; (iv) the H_(2)O stratospheric column is (2.1 ± 0.5) × 10^(14) cm^(-2) but its vertical distribution is still to be determined, so the H_(2)O external flux remains uncertain by over an order of magnitude; and (v) the CO stratospheric abundance is about twice the tropospheric value, confirming the dual origin of CO suspected from ground-based millimeter/submillimeter observations.
Astronomy and Astrophysics | 2003
M-R.L. Cioni; J. A. D. L. Blommaert; M. A. T. Groenewegen; Harm Jan Habing; J. Hron; Franz Kerschbaum; C. Loup; A. Omont; van Loon; Patricia A. Whitelock; Albert A. Zijlstra
This article presents the study of the light-curves extracted from the MACHO database of a sample of stars observed by the Infrared Space Observatory in the Small Magellanic Cloud. These stars belong to the ISO-Mini-Survey catalogue of the Magellanic Clouds (ISO-MCMS, Loup et al. in preparation). Most of them are in the asymptotic giant branch (AGB) and supergiant phases. The dominant period and amplitude of pulsation have been derived and the stars have been classified as Mira or Semi-Regular pulsators. Furthermore, the cross-identification with near-infrared DENIS and 2MASS magnitudes available within the ISO-MCMS allowed us: (i) to investigate the properties of these stars in the combined near- and mid-infrared colour-magnitude diagrams, (ii) to derive the bolometric magnitude by integrating the spectral energy distribution and (iii) to estimate the mass-loss rate. The stars have been divided into carbon- (C-) and oxygen-rich (O-rich) using the (J − KS , KS ) colour-magnitude diagram and their period and amplitude distributions have been compared. C-rich AGB stars have a sharp peak in their period distribution at about 250 days and have on average a larger amplitude than O-rich AGB stars. This effect, not previously detected from the study of similar stars in the Large Magellanic Cloud and in the Baades window, might be closely related to the metallicity of the environment in which the stars have formed.