DOCSLIB.ORG

The Low-Metallicity Picture A

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
The Low-Metallicity Picture A Linking dust emission to fundamental properties in galaxies: the low-metallicity picture A. Rémy-Ruyer, S. C. Madden, F. Galliano, V. Lebouteiller, M. Baes, G. J. Bendo, A. Boselli, L. Ciesla, D. Cormier, A. Cooray, et al. To cite this version: A. Rémy-Ruyer, S. C. Madden, F. Galliano, V. Lebouteiller, M. Baes, et al.. Linking dust emission to fundamental properties in galaxies: the low-metallicity picture. Astronomy and Astrophysics - A&A, EDP Sciences, 2015, 582, pp.A121. 10.1051/0004-6361/201526067. cea-01383748 HAL Id: cea-01383748 https://hal-cea.archives-ouvertes.fr/cea-01383748 Submitted on 19 Oct 2016 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. A&A 582, A121 (2015) Astronomy DOI: 10.1051/0004-6361/201526067 & c ESO 2015 Astrophysics Linking dust emission to fundamental properties in galaxies: the low-metallicity picture? A. Rémy-Ruyer1;2, S. C. Madden2, F. Galliano2, V. Lebouteiller2, M. Baes3, G. J. Bendo4, A. Boselli5, L. Ciesla6, D. Cormier7, A. Cooray8, L. Cortese9, I. De Looze3;10, V. Doublier-Pritchard11, M. Galametz12, A. P. Jones1, O. Ł. Karczewski13, N. Lu14, and L. Spinoglio15 1 Institut d’Astrophysique Spatiale, CNRS, UMR 8617, 91405 Orsay, France e-mail: [email protected]; [email protected] 2 Laboratoire AIM, CEA/IRFU/Service d’Astrophysique, Université Paris Diderot, Bât. 709, 91191 Gif-sur-Yvette, France 3 Sterrenkundig Observatorium, Universiteit Gent, Krijgslaan 281 S9, 9000 Gent, Belgium 4 UK ALMA Regional Centre Node, Jodrell Bank Centre for Astrophysics, School of Physics & Astronomy, University of Manchester, Oxford Road, Manchester M13 9PL, UK 5 Laboratoire d’Astrophysique de Marseille – LAM, Université d’Aix-Marseille & CNRS, UMR 7326, 38 rue F. Joliot-Curie, 13388 Marseille Cedex 13, France 6 Department of Physics, University of Crete, 71003 Heraklion, Greece 7 Zentrum für Astronomie der Universität Heidelberg, Institut für Theoretische Astrophysik, Albert-Ueberle-Str. 2, 69120 Heidelberg, Germany 8 Center for Cosmology, Department of Physics and Astronomy, University of California, Irvine, CA 92697, USA 9 Centre for Astrophysics & Supercomputing, Swinburne University of Technology, Mail H30, PO Box 218, Hawthorn VIC 3122, Australia 10 Institute of Astronomy, University of Cambridge, Madingley Road, Cambridge CB3 0HA, UK 11 Max-Planck für Extraterrestrische Physik, Giessenbachstr. 1, 85748 Garching-bei-München, Germany 12 European Southern Observatory, Karl-Schwarzschild-Str. 2, 85748 Garching-bei-München, Germany 13 Department of Physics and Astronomy, University of Sussex, Brighton, BN1 9QH, UK 14 NASA Herschel Science Center, MS 100-22, California Institute of Technology, Pasadena, CA 91125, USA 15 Instituto di Astrofisica e Planetologia Spaziali, INAF-IAPS, Via Fosso del Cavaliere 100, 00133 Roma, Italy Received 10 March 2015 / Accepted 14 July 2015 ABSTRACT Aims. In this work, we aim to provide a consistent analysis of the dust properties from metal-poor to metal-rich environments by linking them to fundamental galactic parameters. Methods. We consider two samples of galaxies: the Dwarf Galaxy Survey (DGS) and the Key Insights on Nearby Galaxies: a Far- Infrared Survey with Herschel (KINGFISH), totalling 109 galaxies, spanning almost 2 dex in metallicity. We collect infrared (IR) to submillimetre (submm) data for both samples and present the complete data set for the DGS sample. We model the observed spectral energy distributions (SED) with a physically-motivated dust model to access the dust properties: dust mass, total-IR luminosity, polycyclic aromatic hydrocarbon (PAH) mass fraction, dust temperature distribution, and dust-to-stellar mass ratio. Results. Using a different SED model (modified black body), different dust composition (amorphous carbon in lieu of graphite), or a different wavelength coverage at submm wavelengths results in differences in the dust mass estimate of a factor two to three, showing that this parameter is subject to non-negligible systematic modelling uncertainties. We find half as much dust with the amorphous carbon dust composition. For eight galaxies in our sample, we find a rather small excess at 500 µm (≤1.5σ). We find that the dust SED of low-metallicity galaxies is broader and peaks at shorter wavelengths compared to more metal-rich systems, a sign of a clumpier medium in dwarf galaxies. The PAH mass fraction and dust temperature distribution are found to be driven mostly by the specific star formation rate, sSFR, with secondary effects from metallicity. The correlations between metallicity and dust mass or total-IR luminosity are direct consequences of the stellar mass-metallicity relation. The dust-to-stellar mass ratios of metal-rich sources follow the well-studied trend of decreasing ratio for decreasing sSFR. The relation is more complex for low-metallicity galaxies with high sSFR, and depends on the chemical evolutionary stage of the source (i.e. gas-to-dust mass ratio). Dust growth processes in the ISM play a key role in the dust mass build-up with respect to the stellar content at high sSFR and low metallicity. Conclusions. We conclude that the evolution of the dust properties from metal-poor to metal-rich galaxies derives from a complex interplay between star formation activity, stellar mass, and metallicity. Key words. dust, extinction – evolution – galaxies: dwarf – galaxies: evolution – infrared: ISM – infrared: galaxies 1. Introduction seeds of this evolution lie in the star formation histories of the galaxies, and in their interaction with their environment through The processes by which galaxies evolve from primordial envi- gas infall, outflows, or mergers. The interstellar medium (ISM) ronments to present-day galaxies are still widely debated, but the plays a key role in this evolution since it is the site of stellar birth ? Figures 12 and 13, Tables 4–9, and Appendices are available in and the repository of stellar ejecta. electronic form at http://www.aanda.org Article published by EDP Sciences A121, page 1 of 42 A&A 582, A121 (2015) Although interstellar dust represents only ∼1% of the to- among which more than half are dwarf galaxies and ∼35% have tal mass of the ISM, it is an important agent in star formation. Z ≤ 1=5 Z . We confirmed with this significant sample of low- Dust absorbs the stellar radiation that would otherwise dissoci- metallicity sources that the dust is warmer at low metallicities ate molecules and thus actively participates in the cooling of the and identified several galaxies with submm excess. This study ISM. It is also a catalyser for molecular gas formation by provid- was conducted using only Herschel data and a modified black ing a surface where atoms can react (Hasegawa & Herbst 1993; body to model the dust emission. In Rémy-Ruyer et al.(2014), Vidali et al. 2004; Le Bourlot et al. 2012; Bron et al. 2014). The we confirmed the higher gas-to-dust mass ratios (G/D) at low presence of dust can increase the H2 formation rate by about two metallicities using the sample of Rémy-Ruyer et al.(2013), and orders of magnitudes compared to H2 formation without dust a semi-empirical spectral energy distribution (SED) model over (Tielens 2005), thus facilitating star formation. the whole IR range. We showed that the G/D is actually higher at Dust forms from the available heavy elements in the explo- low metallicities than that expected from a simple description of sively ejected material from core-collapse supernovæ (SN) and the dust evolution in the ISM. The large scatter in the observed in the quiescent outflows from low-mass stars (Todini & Ferrara G/D is intrinsic to the galaxies and reflects a non-universal dust- 2001; Gomez et al. 2012a,b; Indebetouw et al. 2014; Rowlands to-metal mass ratio (see also Dwek 1998; De Cia et al. 2013; et al. 2014; Matsuura et al. 2015). The refractory dust grains Zafar & Watson 2013; Mattsson et al. 2014a). We showed that may, after their injection into the ISM, grow by accretion or the metallicity was the main driver of the G/D but that the scat- coagulation in dense molecular clouds (Bazell & Dwek 1990; ter was controlled by the different SFHs of the sources. Thus Stepnik et al. 2001, 2003; Köhler et al. 2012, 2015), locking metallicity is not the only parameter shaping the dust properties. even more heavy elements in the solid phase of the ISM (Savage As a follow-up of Rémy-Ruyer et al.(2013, 2014), we aim & Sembach 1996; Whittet 2003). Through destructive processes to provide a consistent picture of the evolution of the dust prop- (such as erosion or sputtering; see Jones et al. 1994, 1996; Serra erties from metal-poor to metal-rich galaxies. On the observa- Díaz-Cano & Jones 2008; Bocchio et al. 2012, 2014), elements tional side, we present the complete catalogue of IR-to-submm are released again into the gas phase. Metallicity, defined as the flux densities for the Dwarf Galaxy Survey (DGS). We use a mass fraction of heavy elements, or “metals”, in the ISM, is thus semi-empirical dust SED model, which accounts for starlight in- a key parameter in studying the evolution of galaxies. tensity mixing in the ISM, to interpret the whole IR-to-submm Understanding how dust properties evolve as a function of observed SEDs. In this work, we extend the range of dust proper- metal enrichment can provide important constraints for galaxy ties and look at the dust mass, the total IR (TIR) luminosity, the evolution studies.
Load more

Recommended publications
  • The HERACLES View of the H -To-HI Ratio in Galaxies
    The HERACLES View of the H2-to-HI Ratio in Galaxies Adam Leroy (NRAO, Hubble Fellow) Fabian Walter, Frank Bigiel, the HERACLES and THINGS teams The Saturday Morning Summary • Star formation rate vs. gas relation on ~kpc scales breaks apart into: A relatively universal CO-SFR relation in nearby disks Systematic environmental scalings in the CO-to-HI ratio • The CO-to-HI ratio is a strong function of radius, total gas, and stellar surface density correlated with ISM properties: dust-to-gas ratio, pressure harder to link to dynamics: gravitational instability, arms • Interpretation: the CO-to-HI ratio traces the efficiency of GMC formation Density and dust can explain much of the observed behavior heracles Fabian Walter Erik Rosolowsky MPIA UBC Frank Bigiel Eva Schinnerer UC Berkeley THINGS plus… MPIA Elias Brinks Antonio Usero Gaelle Dumas U Hertfordshire OAN, Madrid MPIA Erwin de Blok Andreas Schruba Helmut Wiesemeyer U Cape Town IRAM … MPIA Rob Kennicutt Axel Weiss Karl Schuster Cambridge MPIfR IRAM Barry Madore Carsten Kramer Karin Sandstrom Carnegie IRAM MPIA Michele Thornley Daniela Calzetti Kelly Foyle Bucknell UMass MPIA Collaborators The HERA CO-Line Extragalactic Survey First maps Leroy et al. (2009) • IRAM 30m Large Program to map CO J = 2→1 line • Instrument: HERA receiver array operating at 230 GHz • 47 galaxies: dwarfs to starbursts and massive spirals -2 • Very wide-field (~ r25) and sensitive (σ ~ 1-2 Msun pc ) NGS The HI Nearby Galaxy Survey HI Walter et al. (2008), AJ Special Issue (2008) • VLA HI maps of 34 galaxies:
    [Show full text]
  • Arxiv:1904.07129V1 [Astro-Ph.GA] 15 Apr 2019
    Draft version April 16, 2019 Preprint typeset using LATEX style emulateapj v. 12/16/11 SPIRE SPECTROSCOPY OF EARLY TYPE GALAXIES Ryen Carl Lapham and Lisa M. Young Physics Department, New Mexico Institute of Mining and Technology, 801 Leroy Place, Socorro, NM 87801; [email protected], [email protected] Draft version April 16, 2019 ABSTRACT We present SPIRE spectroscopy for 9 early-type galaxies (ETGs) representing the most CO-rich and far-infrared (FIR) bright galaxies of the volume-limited Atlas3D sample. Our data include detections of mid to high J CO transitions (J=4-3 to J=13-12) and the [C I] (1-0) and (2-1) emission lines. CO spectral line energy distributions (SLEDs) for our ETGs indicate low gas excitation, barring NGC 1266. We use the [C I] emission lines to determine the excitation temperature of the neutral gas, as well as estimate the mass of molecular hydrogen. The masses agree well with masses derived from CO, making this technique very promising for high redshift galaxies. We do not find a trend between the [N II] 205 flux and the infrared luminosity, but we do find that the [N II] 205/CO(6-5) line ratio is correlated with the 60/100 µm Infrared Astronomical Satellite (IRAS) colors. Thus the [N II] 205/CO(6-5) ratio can be used to infer a dust temperature, and hence the intensity of the interstellar radiation field (ISRF). Photodissociation region (PDR) models show that use of [C I] and CO lines in addition to the typical [C II], [O I], and FIR fluxes drive the model solutions to higher densities and lower values of G0.
    [Show full text]
  • 198 7Apj. . .312L. .11J the Astrophysical Journal, 312:L11-L15
    .11J The Astrophysical Journal, 312:L11-L15,1987 January 1 .312L. © 1987. The American Astronomical Society. All rights reserved. Printed in U.S.A. 7ApJ. 198 INTERSTELLAR DUST IN SHAPLEY-AMES ELLIPTICAL GALAXIES M. Jura and D. W. Kim Department of Astronomy, University of California, Los Angeles AND G. R. Knapp and P. Guhathakurta Princeton University Observatory Received 1986 August 11; accepted 1986 September 30 ABSTRACT We have co-added the IRAS survey data at the positions of the brightest elliptical galaxies in the Revised Shapley-Ames Catalog to increase the sensitivity over that of the IRAS Point Source Catalog. More than half of 7 8 the galaxies (with Bj< \\ mag) are detected at 100 /xm with flux levels indicating, typically, 10 or 10 M0 of cold interstellar matter. The presence of cold gas in ellipticals thus appears to be the rule rather than the exception. Subject headings: galaxies: general — infrared: sources I. INTRODUCTION infrared emission from the elliptical galaxy in the line of sight. The traditional view of early-type galaxies is that they are Our criteria for a real detection are as follows: essentially free of interstellar matter. However, with advances 1. The optical position of the galaxy and the position of the in instrumental sensitivity, it has become possible to observe IRAS source agree to better than V. (The agreement is usually 21 cm emission (Knapp, Turner, and Cunniffe 1985; Wardle much better than T.) and Knapp 1986), optical dust patches (Sadler and Gerhard 2. The flux is at least 3 times the r.m.s. noise.
    [Show full text]
  • High Resolution HI Distributions and Multi-Wavelength Analyses Of
    High Resolution H I Distributions and Multi-Wavelength Analyses of Magellanic Spirals NGC 4618 and NGC 4625 Jane F. Kaczmarek1& Eric M. Wilcots University of Wisconsin Madison, Department of Astronomy, 475 N. Charter Street, Madison WI 53706 USA [email protected], [email protected] ABSTRACT We present a detailed analysis of high resolution H I observations of the Magellanic spiral galaxies NGC 4618 and NGC 4625. While the H I disk of NGC 4625 is remarkably quiescent with a nearly uniform velocity dispersion and no evidence of H I holes, there is a dynamic interplay between star formation and the distribution of neutral hydrogen in NGC 4618. We calculate the critical density for widespread star formation in each galaxy and find that star formation proceeds even where the surface density of the atomic gas is well below the critical density necessary for global star formation. There are strong spatial correlations in NGC 4618 between UV emission, 1.4 GHz radio continuum emission, and peaks in the H I column density. Despite the apparent overlap of the outer disks of the two galaxies, we find that they are kinematically distinct, indicating that NGC 4618 and NGC 4625 are not interacting. The structure of NGC 4618 and, in particular, the nature of its outer ring, are highly suggestive of an interaction, but the timing and nature of such an interaction remain unclear. Subject headings: galaxies: neutral hydrogen { galaxies: Magellanic spirals { galaxies: individual (NGC 4618 & NGC 4625) 1. Introduction arXiv:1206.4104v1 [astro-ph.CO] 19 Jun 2012 One of the more stunning revelations about the Local Group in the past few years has been the observations of the proper motions of the Magellanic Clouds showing that they are moving at significantly higher velocities than previously thought (e.g.
    [Show full text]
  • Stripped Elliptical Galaxies As Probes of Icm Physics. Ii
    The Astrophysical Journal, 806:104 (15pp), 2015 June 10 doi:10.1088/0004-637X/806/1/104 © 2015. The American Astronomical Society. All rights reserved. STRIPPED ELLIPTICAL GALAXIES AS PROBES OF ICM PHYSICS. II. STIRRED, BUT MIXED? VISCOUS AND INVISCID GAS STRIPPING OF THE VIRGO ELLIPTICAL M89 E. Roediger1,2,5, R. P. Kraft2, P. E. J. Nulsen2, W. R. Forman2, M. Machacek2, S. Randall2, C. Jones2, E. Churazov3, and R. Kokotanekova4 1 Hamburger Sternwarte, Universität Hamburg, Gojensbergsweg 112, D-21029 Hamburg, Germany; [email protected] 2 Harvard/Smithsonian Center for Astrophysics, 60 Garden Street MS-4, Cambridge, MA 02138, USA 3 MPI für Astrophysik, Karl-Schwarzschild-Str. 1, Garching D-85741, Germany 4 AstroMundus Master Programme, University of Innsbruck, Technikerstr. 25/8, 6020 Innsbruck, Austria Received 2014 September 18; accepted 2015 March 29; published 2015 June 10 ABSTRACT Elliptical galaxies moving through the intracluster medium (ICM) are progressively stripped of their gaseous atmospheres. X-ray observations reveal the structure of galactic tails, wakes, and the interface between the galactic gas and the ICM. This fine-structure depends on dynamic conditions (galaxy potential, initial gas contents, orbit in the host cluster), orbital stage (early infall, pre-/post-pericenter passage), as well as on the still ill-constrained ICM plasma properties (thermal conductivity, viscosity, magnetic field structure). Paper I describes flow patterns and stages of inviscid gas stripping. Here we study the effect of a Spitzer-like temperature dependent viscosity corresponding to Reynolds numbers, Re, of 50–5000 with respect to the ICM flow around the remnant atmosphere. Global flow patterns are independent of viscosity in this Reynolds number range.
    [Show full text]
  • 1501.01010V1.Pdf
    Draft version January 7, 2015 Preprint typeset using LATEX style emulateapj v. 5/2/11 JET-ISM INTERACTION IN THE RADIO GALAXY 3C293: JET-DRIVEN SHOCKS HEAT ISM TO POWER X-RAY AND MOLECULAR H2 EMISSION L. Lanz1, P. M. Ogle1, D. Evans2, P. N. Appleton3, P. Guillard4, B. Emonts5 Draft version January 7, 2015 ABSTRACT We present a 70ks Chandra observation of the radio galaxy 3C 293. This galaxy belongs to the class of molecular hydrogen emission galaxies (MOHEGs) that have very luminous emission from warm molecular hydrogen. In radio galaxies, the molecular gas appears to be heated by jet-driven shocks, but exactly how this mechanism works is still poorly understood. With Chandra, we observe X-ray emission from the jets within the host galaxy and along the 100 kpc radio jets. We model the X-ray spectra of the nucleus, the inner jets, and the X-ray features along the extended radio jets. Both the nucleus and the inner jets show evidence of 107 K shock-heated gas. The kinetic power of the jets is more than sufficient to heat the X-ray emitting gas within the host galaxy. The thermal X-ray and warm H2 luminosities of 3C 293 are similar, indicating similar masses of X-ray hot gas and warm molecular gas. This is consistent with a picture where both derive from a multiphase, shocked interstellar medium (ISM). We find that radio-loud MOHEGs that are not brightest cluster galaxies (BCGs), like 3C 293, typically have LH2 /LX ∼ 1 and MH2 /MX ∼ 1, whereas MOHEGs that are BCGs have LH2 /LX ∼ 0.01 and MH2 /MX ∼ 0.01.
    [Show full text]
  • 1. Introduction
    THE ASTROPHYSICAL JOURNAL SUPPLEMENT SERIES, 122:109È150, 1999 May ( 1999. The American Astronomical Society. All rights reserved. Printed in U.S.A. GALAXY STRUCTURAL PARAMETERS: STAR FORMATION RATE AND EVOLUTION WITH REDSHIFT M. TAKAMIYA1,2 Department of Astronomy and Astrophysics, University of Chicago, Chicago, IL 60637; and Gemini 8 m Telescopes Project, 670 North Aohoku Place, Hilo, HI 96720 Received 1998 August 4; accepted 1998 December 21 ABSTRACT The evolution of the structure of galaxies as a function of redshift is investigated using two param- eters: the metric radius of the galaxy(Rg) and the power at high spatial frequencies in the disk of the galaxy (s). A direct comparison is made between nearby (z D 0) and distant(0.2 [ z [ 1) galaxies by following a Ðxed range in rest frame wavelengths. The data of the nearby galaxies comprise 136 broad- band images at D4500A observed with the 0.9 m telescope at Kitt Peak National Observatory (23 galaxies) and selected from the catalog of digital images of Frei et al. (113 galaxies). The high-redshift sample comprises 94 galaxies selected from the Hubble Deep Field (HDF) observations with the Hubble Space Telescope using the Wide Field Planetary Camera 2 in four broad bands that range between D3000 and D9000A (Williams et al.). The radius is measured from the intensity proÐle of the galaxy using the formulation of Petrosian, and it is argued to be a metric radius that should not depend very strongly on the angular resolution and limiting surface brightness level of the imaging data. It is found that the metric radii of nearby and distant galaxies are comparable to each other.
    [Show full text]
  • Southern Arp - AM # Order
    Southern Arp - AM # Order A B C D E F G H I J 1 AM # Constellation Object Name RA DEC Mag. Size Uranom. Uranom. Millenium 2 1st Ed. 2nd Ed. 3 AM 0003-414 Phoenix ESO 293-G034 00h06m19.9s -41d30m00s 13.7 3.2 x 1.0 386 177 430 Vol I 4 AM 0006-340 Sculptor NGC 10 00h08m34.5s -33d51m30s 13.3 2.4 x 1.2 350 159 410 Vol I 5 AM 0007-251 Sculptor NGC 24 00h09m56.5s -24d57m47s 12.4 5.8 x 1.3 305 141 366 Vol I 6 AM 0011-232 Cetus NGC 45 00h14m04.0s -23d10m55s 11.6 8.5 x 5.9 305 141 366 Vol I 7 AM 0027-333 Sculptor NGC 134 00h30m22.0s -33d14m39s 11.4 8.5 x 2.0 351 159 409 Vol I 8 AM 0029-643 Tucana ESO 079- G003 00h32m02.2s -64d15m12s 12.6 2.7 x 0.4 440 204 409 Vol I 9 AM 0031-280B Sculptor NGC 150 00h34m15.5s -27d48m13s 12 3.9 x 1.9 306 141 387 Vol I 10 AM 0031-320 Sculptor NGC 148 00h34m15.5s -31d47m10s 13.3 2 x 0.8 351 159 387 Vol I 11 AM 0033-253 Sculptor IC 1558 00h35m47.1s -25d22m28s 12.6 3.4 x 2.5 306 141 365 Vol I 12 AM 0041-502 Phoenix NGC 238 00h43m25.7s -50d10m58s 13.1 1.9 x 1.6 417 177 449 Vol I 13 AM 0045-314 Sculptor NGC 254 00h47m27.6s -31d25m18s 12.6 2.5 x 1.5 351 176 386 Vol I 14 AM 0050-312 Sculptor NGC 289 00h52m42.3s -31d12m21s 11.7 5.1 x 3.6 351 176 386 Vol I 15 AM 0052-375 Sculptor NGC 300 00h54m53.5s -37d41m04s 9 22 x 16 351 176 408 Vol I 16 AM 0106-803 Hydrus ESO 013- G012 01h07m02.2s -80d18m28s 13.6 2.8 x 0.9 460 214 509 Vol I 17 AM 0105-471 Phoenix IC 1625 01h07m42.6s -46d54m27s 12.9 1.7 x 1.2 387 191 448 Vol I 18 AM 0108-302 Sculptor NGC 418 01h10m35.6s -30d13m17s 13.1 2 x 1.7 352 176 385 Vol I 19 AM 0110-583 Hydrus NGC
    [Show full text]
  • The Globular Cluster System of NGC 1399
    Astronomy & Astrophysics manuscript no. sch1399 c ESO 2018 August 28, 2018 The globular cluster system of NGC 1399 ⋆,⋆⋆ V. dynamics of the cluster system out to 80 kpc Y. Schuberth1,2, T. Richtler2, M. Hilker3, B. Dirsch2, L. P. Bassino4, A. J. Romanowsky5,2, and L. Infante6 1 Argelander-Institut f¨ur Astronomie, Universit¨at Bonn, Auf dem H¨ugel 71, D-53121 Bonn, Germany 2 Universidad de Concepci´on, Departamento de Astronomia, Casilla 160-C, Concepci´on, Chile 3 European Southern Observatory, Karl-Schwarzschild-Str. 2, D-85748 Garching, Germany 4 Facultad de Ciencias Astron´omicas y Geof´ısicas, Universidad Nacional de La Plata, Paseo del Bosque S/N, 1900–La Plata, Argentina; and Instituto de Astrof´ısica de La Plata (CCT La Plata – CONICET – UNLP) 5 UCO/Lick Observatory, University of California, Santa Cruz, CA 95064, USA 6 Departamento de Astronom´ıa y Astrof´ısica, Pontificia Universidad Cat´olica de Chile, Casilla 306, Santiago 22, Chile Received 14 May, 2009; accepted 16 October, 2009 ABSTRACT Globular clusters (GCs) are tracers of the gravitational potential of their host galaxies. Moreover, their kinematic properties may provide clues for understanding the formation of GC systems and their host galaxies. We use the largest set of GC velocities obtained so far of any elliptical galaxy to revise and extend the previous investigations (Richtler et al. 2004) of the dynamics of NGC 1399, the central dominant galaxy of the nearby Fornax cluster of galaxies. The GC velocities are used to study the kinematics, their relation with population properties, and the dark matter halo of NGC 1399.
    [Show full text]
  • 115 Abell Galaxy Cluster # 373
    WINTER Medium-scope challenges 271 # # 115 Abell Galaxy Cluster # 373 Target Type RA Dec. Constellation Magnitude Size Chart AGCS 373 Galaxy cluster 03 38.5 –35 27.0 Fornax – 180 ′ 5.22 Chart 5.22 Abell Galaxy Cluster (South) 373 272 Cosmic Challenge WINTER Nestled in the southeast corner of the dim early winter western suburbs. Deep photographs reveal that NGC constellation Fornax, adjacent to the distinctive triangle 1316 contains many dust clouds and is surrounded by a formed by 6th-magnitude Chi-1 ( ␹ 1), Chi-2 ( ␹ 2), and complex envelope of faint material, several loops of Chi-3 ( ␹ 3) Fornacis, is an attractive cluster of galaxies which appear to engulf a smaller galaxy, NGC 1317, 6 ′ known as Abell Galaxy Cluster – Southern Supplement to the north. Astronomers consider this to be a case of (AGCS) 373. In addition to his research that led to the galactic cannibalism, with the larger NGC 1316 discovery of more than 80 new planetary nebulae in the devouring its smaller companion. The merger is further 1950s, George Abell also examined the overall structure signaled by strong radio emissions being telegraphed of the universe. He did so by studying and cataloging from the scene. 2,712 galaxy clusters that had been captured on the In my 8-inch reflector, NGC 1316 appears as a then-new National Geographic Society–Palomar bright, slightly oval disk with a distinctly brighter Observatory Sky Survey taken with the 48-inch Samuel nucleus. NGC 1317, about 12th magnitude and 2 ′ Oschin Schmidt camera at Palomar Observatory. In across, is visible in a 6-inch scope, although averted 1958, he published the results of his study as a paper vision may be needed to pick it out.
    [Show full text]
  • VLBA Detection of Nuclear Compact Emission in the AGN-Driven Molecular Outflow Candidate NGC 1266
    VLBA Detection of Nuclear Compact Emission in the AGN-Driven Molecular Outflow Candidate NGC 1266 Kristina Nyland New Mexico Tech 2012 New Mexico Symposium Outflows in Galaxies • Can help regulate star formation and SMBH growth • May be responsible for various empirical scaling relations in galaxies (e.g., Faber-Jackson relation) • Driving mechanisms: • Stellar feedback • Radiation pressure • Stellar winds (young O stars, AGB stars) • Supernovae • AGNs • Quasar mode (radiative) • Radio mode (mechanical/kinetic) Starburst-Driven Molecular Outflows M82 (Walter+02) Arp 220 (Sakamoto+09) • Prototypical SB galaxy • ULIRG • Interacting with M81 • merger remnant • Molecular gas entrained in • (But AGN may play a starburst wind see role, Rangwala+11) 8 7 • Moutflow = 3 x 10 Msun • Moutflow = 5 x 10 Msun • dM/dt = 30 Msun/year • dM/dt = 100 Msun/year • voutflow = 100 km/s • voutflow = 100 km/s HST HST AGN-Driven Molecular Outflows • Outflows of neutral/ionized gas relatively common in AGNs • Molecular outflows potentially powered by AGNs are rare • Much of the evidence is circumstantial • e.g., SDSS statistical analyses of timing of starbursts and AGN activity • Many candidates for direct evidence are high-redshift quasars • local candidates needed! AGN-Driven Molecular Outflows Mrk 231 (Feruglio+10) • Nearest quasar host • Interacting system 8 • Moutflow = 5.8 x 10 Msun • dM/dt = 100-700 Msun/yr • v = 700 km/s outflow Gemini NGC 1266: Local Candidate AGN- driven Molecular Outflow Host? • Morphology: S0 • Environment: Field – no evidence of recent major merger • Distance: 29.9 Mpc • MK = -22.93 DSS • σ* = 79 km/s 6 • MBH: ~3.2 x 10 Msun IRAM 30m CO Emission Figures from Alatalo et al.
    [Show full text]
  • The Molecular Gas Reservoir of 6 Low-Metallicity Galaxies from the Herschel Dwarf Galaxy Survey a Ground-Based Follow-Up Survey of CO(1–0), CO(2–1), and CO(3–2)
    A&A 564, A121 (2014) Astronomy DOI: 10.1051/0004-6361/201322096 & c ESO 2014 Astrophysics The molecular gas reservoir of 6 low-metallicity galaxies from the Herschel Dwarf Galaxy Survey A ground-based follow-up survey of CO(1–0), CO(2–1), and CO(3–2) D. Cormier1,S.C.Madden2, V. Lebouteiller2,S.Hony3, S. Aalto4, F. Costagliola4,5, A. Hughes3, A. Rémy-Ruyer2, N. Abel6, E. Bayet7, F. Bigiel1, J. M. Cannon8,R.J.Cumming9, M. Galametz10, F. Galliano2, S. Viti11,andR.Wu2 1 Institut für theoretische Astrophysik, Zentrum für Astronomie der Universität Heidelberg, Albert-Ueberle Str. 2, 69120 Heidelberg, Germany e-mail: [email protected] 2 Laboratoire AIM, CEA/DSM – CNRS – Université Paris Diderot, Irfu/Service d’Astrophysique, CEA Saclay, 91191 Gif-sur-Yvette, France 3 Max-Planck-Institute for Astronomy, Königstuhl 17, 69117 Heidelberg, Germany 4 Department of Earth and Space Sciences, Chalmers University of Technology, Onsala Space Observatory, 439 92 Onsala, Sweden 5 Instituto de Astrofísica de Andalucía, Glorieta de la Astronomía s/n, 18008 Granada, Spain 6 University of Cincinnati, Clermont College, Batavia OH 45103, USA 7 Sub-Dept. of Astrophysics, Dept. of Physics at University of Oxford, Denys Wilkinson Building, Keble Road, Oxford OX1 3RH, UK 8 Department of Physics & Astronomy, Macalester College, 1600 Grand Avenue, Saint Paul MN 55105, USA 9 Onsala Space Observatory, Chalmers University of Technology, 439 92 Onsala, Sweden 10 Institute of Astronomy, University of Cambridge, Madingley Road, Cambridge CB3 0HA, UK 11 Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, UK Received 17 June 2013 / Accepted 17 November 2013 ABSTRACT Context.
    [Show full text]