David Allan Thilker
Johns Hopkins University
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Featured researches published by David Allan Thilker.
The Astrophysical Journal | 2005
Daniela Calzetti; Robert C. Kennicutt; Luciana Bianchi; David Allan Thilker; Daniel A. Dale; C. W. Engelbracht; Claus Leitherer; Martin Meyer; Megan L. Sosey; Maximilian J. Mutchler; Michael W. Regan; Michele D. Thornley; Lee Armus; G. J. Bendo; S. Boissier; A. Boselli; B. T. Draine; Karl D. Gordon; G. Helou; David J. Hollenbach; Lisa J. Kewley; Barry F. Madore; D. C. Martin; E. J. Murphy; G. H. Rieke; Marcia J. Rieke; H. Roussel; Kartik Sheth; J. D. Smith; Frederick M. Walter
(Abridged) Far ultraviolet to far infrared images of the nearby galaxy NGC5194, from Spitzer, GALEX, Hubble Space Telescope and ground--based data, are used to investigate local and global star formation, and the impact of dust extinction in HII-emitting knots. In the IR/UV-UV color plane, the NGC5194 HII knots show the same trend observed for normal star-forming galaxies, having a much larger dispersion than starburst galaxies. We identify the dispersion as due to the UV emission predominantly tracing the evolved, non-ionizing stellar population, up to ages 50-100 Myr. While in starbursts the UV light traces the current SFR, in NGC5194 it traces a combination of current and recent-past SFR. Unlike the UV emission, the monochromatic 24 micron luminosity is an accurate local SFR tracer for the HII knots in NGC5194; this suggests that the 24 micron emission carriers are mainly heated by the young, ionizing stars. However, preliminary results show that the ratio of the 24 micron emission to the SFR varies by a factor of a few from galaxy to galaxy. While also correlated with star formation, the 8 micron emission is not directly proportional to the number of ionizing photons. This confirms earlier suggestions that the carriers of the 8 micron emission are heated by more than one mechanism.
The Astrophysical Journal | 2007
Daniel A. Dale; A. Gil de Paz; Karl D. Gordon; H. M. Hanson; Lee Armus; G. J. Bendo; Luciana Bianchi; Miwa Block; S. Boissier; A. Boselli; Brent Alan Buckalew; V. Buat; D. Burgarella; Daniela Calzetti; John M. Cannon; C. W. Engelbracht; G. Helou; David J. Hollenbach; T. H. Jarrett; Robert C. Kennicutt; Claus Leitherer; Aigen Li; Barry F. Madore; D. C. Martin; Martin Meyer; E. J. Murphy; Michael W. Regan; Helene Roussel; J. D. Smith; Megan L. Sosey
The ultraviolet-to-radio continuum spectral energy distributions are presented for all 75 galaxies in the Spitzer Infrared Nearby Galaxies Survey (SINGS). A principal component analysis of the sample shows that most of the samples spectral variations stem from two underlying components, one representative of a galaxy with a low infrared-to-ultraviolet ratio and one representative of a galaxy with a high infrared-to-ultraviolet ratio. The influence of several parameters on the infrared-to-ultraviolet ratio is studied (e.g., optical morphology, disk inclination, far-infrared color, ultraviolet spectral slope, and star formation history). Consistent with our understanding of normal star-forming galaxies, the SINGS sample of galaxies in comparison to more actively star-forming galaxies exhibits a larger dispersion in the infrared-to-ultraviolet versus ultraviolet spectral slope correlation. Early-type galaxies, exhibiting low star formation rates and high optical surface brightnesses, have the most discrepant infrared-to-ultraviolet correlation. These results suggest that the star formation history may be the dominant regulator of the broadband spectral variations between galaxies. Finally, a new discovery shows that the 24 μm morphology can be a useful tool for parameterizing the global dust temperature and ultraviolet extinction in nearby galaxies. The dust emission in dwarf/irregular galaxies is clumpy and warm accompanied by low ultraviolet extinction, while in spiral galaxies there is typically a much larger diffuse component of cooler dust and average ultraviolet extinction. For galaxies with nuclear 24 μm emission, the dust temperature and ultraviolet extinction are relatively high compared to disk galaxies.
Monthly Notices of the Royal Astronomical Society | 2010
Barbara Catinella; David Schiminovich; Guinevere Kauffmann; Silvia Fabello; Jing Wang; Cameron B. Hummels; Jenna Lemonias; Sean M. Moran; Ronin Wu; Riccardo Giovanelli; Martha P. Haynes; Timothy M. Heckman; Antara R. Basu-Zych; Michael R. Blanton; Jarle Brinchmann; Tamas Budavari; Thiago S. Goncalves; Benjamin D. Johnson; Robert C. Kennicutt; Barry F. Madore; Christopher D. Martin; Michael R. Rich; L. J. Tacconi; David Allan Thilker; Vivienne Wild; Ted K. Wyder
We introduce the GALEX Arecibo SDSS Survey (GASS), an on-going large programme that is gathering high quality H i-line spectra using the Arecibo radio telescope for an unbiased sample of ~1000 galaxies with stellar masses greater than 10^(10) M_⊙ and redshifts 0.025 < z < 0.05 , selected from the Sloan Digital Sky Survey (SDSS) spectroscopic and Galaxy Evolution Explorer (GALEX) imaging surveys. The galaxies are observed until detected or until a low gas mass fraction limit (1.5–5 per cent) is reached. This paper presents the first Data Release, consisting of ~20 per cent of the final GASS sample. We use this data set to explore the main scaling relations of the H i gas fraction with galaxy structure and NUV−r colour. A large fraction (~60 per cent) of the galaxies in our sample are detected in H i. Even at stellar masses above 10^(11) M_⊙, the detected fraction does not fall below ~40 per cent. We find that the atomic gas fraction M_(HI)/M★ decreases strongly with stellar mass, stellar surface mass density and NUV−r colour, but is only weakly correlated with the galaxy bulge-to-disc ratio (as measured by the concentration index of the r-band light). We also find that the fraction of galaxies with significant (more than a few per cent) H I decreases sharply above a characteristic stellar surface mass density of 10^(8.5) M_⊙ kpc^(−2). The fraction of gas-rich galaxies decreases much more smoothly with stellar mass. One of the key goals of GASS is to identify and quantify the incidence of galaxies that are transitioning between the blue, star-forming cloud and the red sequence of passively evolving galaxies. Likely transition candidates can be identified as outliers from the mean scaling relations between M_(HI)/M★ and other galaxy properties. We have fitted a plane to the two-dimensional relation between the H I mass fraction, stellar surface mass density and NUV−r colour. Interesting outliers from this plane include gas-rich red sequence galaxies that may be in the process of regrowing their discs, as well as blue, but gas-poor spirals.
Astrophysical Journal Supplement Series | 2007
David Allan Thilker; Luciana Bianchi; Gerhardt R. Meurer; Armando Gil de Paz; S. Boissier; Barry F. Madore; A. Boselli; Annette M. N. Ferguson; J. C. Muñoz-Mateos; Greg J. Madsen; Salman Hameed; Roderik Overzier; Karl Forster; Peter G. Friedman; D. Christopher Martin; Patrick Morrissey; Susan G. Neff; David Schiminovich; Mark Seibert; Todd Small; Ted K. Wyder; Jose Donas; Timothy M. Heckman; Young-Wook Lee; Bruno Milliard; R. Michael Rich; Alexander S. Szalay; Barry Y. Welsh; Sukyoung K. Yi
We have initiated a search for extended ultraviolet disk (XUV-disk) galaxies in the local universe. Here we compare GALEX UV and visible-NIR images of 189 nearby (D < 40 Mpc) S0-Sm galaxies included in the GALEX Atlas of Nearby Galaxies and present the first catalog of XUV-disk galaxies. We find that XUV-disk galaxies are surprisingly common but have varied relative (UV/optical) extent and morphology. Type 1 objects (≳20% incidence) have structured, UV-bright/optically faint emission features in the outer disk, beyond the traditional star formation threshold. Type 2 XUV-disk galaxies (~10% incidence) exhibit an exceptionally large, UV-bright/optically low surface brightness (LSB) zone having blue UV-K_s outside the effective extent of the inner, older stellar population, but not reaching extreme galactocentric distance. If the activity occurring in XUV-disks is episodic, a higher fraction of present-day spirals could be influenced by such outer disk star formation. Type 1 disks are associated with spirals of all types, whereas Type 2 XUV-disks are predominantly found in late-type spirals. Type 2 XUV-disks are forming stars quickly enough to double their (currently low) stellar mass in the next Gyr (assuming a constant star formation rate). XUV-disk galaxies of both types are systematically more gas-rich than the general galaxy population. Minor external perturbation may stimulate XUV-disk incidence, at least for Type 1 objects. XUV-disks are the most actively evolving galaxies growing via inside-out disk formation in the current epoch, and may constitute a segment of the galaxy population experiencing significant, continued gas accretion from the intergalactic medium or neighboring objects.
The Astrophysical Journal | 2009
Gerhardt R. Meurer; O. I. Wong; J. H. Kim; D.J. Hanish; Timothy M. Heckman; Jessica K. Werk; Joss Bland-Hawthorn; Michael A. Dopita; M. A. Zwaan; B. Koribalski; Mark Seibert; David Allan Thilker; Henry C. Ferguson; R. L. Webster; Mary E. Putman; Patricia M. Knezek; Marianne T. Doyle; Michael J. Drinkwater; Charles G. Hoopes; Virginia A. Kilborn; Martin Meyer; Emma V. Ryan-Weber; Ryan Christopher Smith; Lister Staveley-Smith
Many of the results in modern astrophysics rest on the notion that the initial mass function (IMF) is universal. Our observations of a sample of H i selected galaxies in the light of Hα and the far-ultraviolet (FUV) challenge this result. The extinction-corrected flux ratio FHα/f FUV from these two tracers of star formation shows strong correlations with the surface brightness in Hα and the R band: low surface brightness (LSB) galaxies have lower FHα/f FUV ratios compared to high surface brightness galaxies as well as compared to expectations from equilibrium models of constant star formation rate (SFR) using commonly favored IMF parameters. Weaker but significant correlations of FHα/f FUV with luminosity, rotational velocity, and dynamical mass as well as a systematic trend with morphology, are found. The correlated variations of FHα/f FUV with other global parameters are thus part of the larger family of galaxy scaling relations. The FHα/f FUV correlations cannot be due to residual extinction correction errors, while systematic variations in the star formation history (SFH) cannot explain the trends with both Hα and R surface brightness nor with other global properties. The possibility that LSB galaxies have a higher escape fraction of ionizing photons seems inconsistent with their high gas fraction, and observations of color–magnitude diagrams (CMDs) of a few systems which indicate a real deficit of O stars. The most plausible explanation for the correlations is the systematic variations of the upper mass limit Mu and/or the slope γ which define the upper end of the IMF. We outline a scenario of pressure driving the correlations by setting the efficiency of the formation of the dense star clusters where the highest mass stars preferentially form. Our results imply that the SFR measured in a galaxy is highly sensitive to the tracer used in the measurement. A nonuniversal IMF would also call into question the interpretation of metal abundance patterns in dwarf galaxies as well as SFHs derived from CMDs.
The Astrophysical Journal | 2005
David Allan Thilker; Luciana Bianchi; S. Boissier; Armando Gil de Paz; Barry F. Madore; D. Christopher Martin; Gerhardt R. Meurer; Susan G. Neff; R. Michael Rich; David Schiminovich; Mark Seibert; Ted K. Wyder; Tom A. Barlow; Yong Ik Byun; Jose Donas; Karl Forster; Peter G. Friedman; Timothy M. Heckman; Patrick Jelinsky; Young-Wook Lee; Roger F. Malina; Bruno Milliard; Patrick Morrissey; Oswald H. W. Siegmund; Todd Small; Alexander S. Szalay; Barry Y. Welsh
Ultraviolet imaging with the Galaxy Evolution Explorer (GALEX) has revealed an extensive sample of UV-bright stellar complexes in the extreme outer disk of M83, extending to about 4 times the radius at which the majority of H II regions are detected (R = 51, or 6.6 kpc). These sources are typically associated with large-scale filamentary H I structures in the warped outer disk of M83 and are distributed beyond the galactocentric radii at which molecular interstellar medium has yet been detected. We present measured properties of these stellar complexes, including far-UV and near-UV magnitudes and local gas surface density. Only a subset of the outer-disk UV sources have corresponding H II regions detected in Hα imaging, consistent with a sample of mixed age in which some sources are a few megayears old and others are much more evolved (~108 yr).
The Astrophysical Journal | 2014
Armin Rest; D. Scolnic; Ryan J. Foley; M. Huber; Ryan Chornock; Gautham S. Narayan; John L. Tonry; Edo Berger; Alicia M. Soderberg; Christopher W. Stubbs; Adam G. Riess; Robert P. Kirshner; S. J. Smartt; Edward F. Schlafly; Steven A. Rodney; M. T. Botticella; D. Brout; Peter M. Challis; Ian Czekala; Maria Rebecca Drout; Michael J. Hudson; R. Kotak; C. Leibler; R. Lunnan; G. H. Marion; M. McCrum; D. Milisavljevic; Andrea Pastorello; Nathan Edward Sanders; K. W. Smith
We present griz P1 light curves of 146 spectroscopically confirmed Type Ia supernovae (SNe Ia; 0.03 < z < 0.65) discovered during the first 1.5 yr of the Pan-STARRS1 Medium Deep Survey. The Pan-STARRS1 natural photometric system is determined by a combination of on-site measurements of the instrument response function and observations of spectrophotometric standard stars. We find that the systematic uncertainties in the photometric system are currently 1.2% without accounting for the uncertainty in the Hubble Space Telescope Calspec definition of the AB system. A Hubble diagram is constructed with a subset of 113 out of 146 SNe Ia that pass our light curve quality cuts. The cosmological fit to 310 SNe Ia (113 PS1 SNe Ia + 222 light curves from 197 low-z SNe Ia), using only supernovae (SNe) and assuming a constant dark energy equation of state and flatness, yields . When combined with BAO+CMB(Planck)+H 0, the analysis yields and including all identified systematics. The value of w is inconsistent with the cosmological constant value of –1 at the 2.3σ level. Tension endures after removing either the baryon acoustic oscillation (BAO) or the H 0 constraint, though it is strongest when including the H 0 constraint. If we include WMAP9 cosmic microwave background (CMB) constraints instead of those from Planck, we find , which diminishes the discord to <2σ. We cannot conclude whether the tension with flat ΛCDM is a feature of dark energy, new physics, or a combination of chance and systematic errors. The full Pan-STARRS1 SN sample with ~three times as many SNe should provide more conclusive results.
The Astrophysical Journal | 2009
R. Braun; David Allan Thilker; Rene A. M. Walterbos; Edvige Corbelli
We have undertaken a deep, wide-field H I imaging survey of M31, reaching a maximum resolution of about 50 pc and 2 km s–1 across a 95 × 48 kpc region. The H I mass and brightness sensitivity at 100 pc resolution for a 25 km s–1 wide spectral feature is 1500 M ☉ and 0.28 K. Our study reveals ubiquitous H I self-opacity features, discernible in the first instance as filamentary local minima in images of the peak H I brightness temperature. Local minima are organized into complexes of more than kpc length and are particularly associated with the leading edge of spiral arm features. Just as in the Galaxy, there is only patchy correspondence of self-opaque features with CO(1-0) emission. We have produced images of the best-fit physical parameters: spin temperature, opacity-corrected column density, and nonthermal velocity dispersion, for the brightest spectral feature along each line of sight in the M31 disk. Spectroscopically opaque atomic gas is organized into filamentary complexes and isolated clouds down to 100 pc. Localized opacity corrections to the column density exceed an order of magnitude in many cases and add globally to a 30% increase in the atomic gas mass over that inferred from the integrated brightness under the usual assumption of negligible self-opacity. Opaque atomic gas first increases from 20 to 60 K in spin temperature with radius to 12 kpc but then declines again to 20 K beyond 25 kpc. We have extended the resolved star formation law down to physical scales more than an order of magnitude smaller in area and mass than has been possible previously. The relation between total gas mass and star formation rate density is significantly tighter than that with molecular mass and is fully consistent in both slope and normalization with the power-law index of 1.56 found in the molecule-dominated disk of M51 at 500 pc resolution. Below a gas mass density of about 5 M ☉ pc–2, there is a downturn in star formation rate density which may represent a real local threshold for massive star formation at a cloud mass of about 5 × 104 M ☉.
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).
The Astrophysical Journal | 2006
Karl D. Gordon; Jeremy Bailin; C. W. Engelbracht; G. H. Rieke; Karl Anthony Misselt; William B. Latter; Eric T. Young; Matthew L. N. Ashby; Pauline Barmby; Brad K. Gibson; Dean C. Hines; Joannah L. Hinz; Oliver Krause; Deborah A. Levine; Francine Roxanne Marleau; Alberto Noriega-Crespo; Susan Renee Stolovy; David Allan Thilker; M. Werner
New images of M31 at 24, 70, and 160 μm taken with the Multiband Imaging Photometer for Spitzer (MIPS) reveal the morphology of the dust in this galaxy. This morphology is well represented by a composite of two logarithmic spiral arms and a circular ring (radius ~10 kpc) of star formation offset from the nucleus. The two spiral arms appear to start at the ends of a bar in the nuclear region and extend beyond the star-forming ring. As has been found in previous work, the spiral arms are not continuous, but composed of spiral segments. The star-forming ring is very circular except for a region near M32 where it splits. The lack of well-defined spiral arms and the prominence of the nearly circular ring suggest that M31 has been distorted by interactions with its satellite galaxies. Using new dynamical simulations of M31 interacting with M32 and NGC 205, we find that, qualitatively, such interactions can produce an offset, split ring like that seen in the MIPS images.