197 6Apj. . .206. .883V the Astrophysical Journal, 206:883-887

Total Page:16

File Type:pdf, Size:1020Kb

197 6Apj. . .206. .883V the Astrophysical Journal, 206:883-887 .883V .206. The Astrophysical Journal, 206:883-887, 1976 June 15 . © 1976. The American Astronomical Society. All rights reserved. Printed in U.S.A. 6ApJ. 197 A NEW CLASSIFICATION SYSTEM FOR GALAXIES* Sidney van den Bergh| David Dunlap Observatory, University of Toronto Received 1975 October 6 ABSTRACT 1) A new galaxy classification system is proposed in which normal spirals and lenticulars form parallel sequences within which “early” and “late” systems are distinguished by means of their disk-to-bulge ratios. 2) A sequence of “anemic spirals,” which occur most frequently in rich clusters, is found to have characteristics that are intermediate between those of vigorous gas-rich normal spirals and gas-poor systems of type SO. 3) The differences between normal spirals (Sa-Sb-Sc), anemic spirals (Aa-Ab-Ac), and lenticulars (S0a-S0b-S0c) are tentatively interpreted in terms of the influence of environment on thé evolution of flattened galaxies. Subject heading: galaxies: structure I. WHY A NEW CLASSIFICATION SYSTEM IS NEEDED galaxies such as NGC 4866 {Hubble Atlas, p. 11) which have a very small nuclear bulge. The only feature Current thinking on galaxy classification has its common to all of these diverse types of objects is that roots in the classical paper of Hubble (1926). Much of the simple beauty of the classification scheme pro- star formation is not proceeding very vigorously. posed in that paper was lost when Hubble (1936) c) Effects of Luminosity introduced a more or less hypothetical transitional stage, which he called type SO, between elliptical and The Hubble (1936) classification system for spirals spiral galaxies. The subsequent evolution of this SO was defined in terms of supergiant galaxies. This bias classification type in the hands of Hubble and Sandage of the Hubble system has, to some extent, been over- is described in The Hubble Atlas of Galaxies (Sandage come by van den Bergh (1960a, b, c), who extended 1961). the original Hubble classification scheme to include In attempting to apply the Hubble-Sandage system the effects of differing galaxy luminosity. to the classification of galaxies I have, for many years, had the feeling that some types of galaxies do not fit d) Effects of the Cluster Environment naturally into the framework provided by this scheme. The large homogeneous sample of galaxy photo- The main problem areas appear to be the following: graphs provided by the glass copies of The Palomar Sky Survey has made it clear that the appearance of a) Lenticulars many galaxies in rich clusters differs from that of field The classification sequence from SOi to S03 (Sandage galaxies of similar Hubble type. No account is taken 1961) is not a sequence of increasing flattening. The of such differences in any of the major galaxy classifi- SOi galaxy NGC 4762 {Hubble Atlas, p. 8) is one of the cation schemes that are presently in use. flattest edge-on galaxies known. A counterexample is provided by NGC 5866 {Hubble Atlas, p. 6) which is II. PROPOSED REVISION OF THE HUBBLE-SANDAGE SYSTEM an edge-on system of type S03 which, in the absence of a thin absorption lane, would have been classified From a detailed study of the flattening of SO E5orE6. galaxies and of spirals Sandage, Freeman, and Stokes (1970) conclude that spiral and lenticular galaxies b) Galaxies of type Sa have the same distribution of true axial ratios. This The classification type Sa has become a repository important result suggests that normal spirals, which for galaxies with very different physical characteristics. exhibit a strong display of Population I, and SO On the one hand this class comprises objects similar galaxies (which contain few if any young stars) form to NGC 1302 {Hubble Atlas, p. 9), which have quite parallel sequences. These two sequences differ large nuclear bulges, and on the other it contains primarily in their total gas content and hence in the mean age of their stellar populations. The existence * Based, in part, on a review presented at the Tercentenary of both highly flattened gas-free systems and similarly celebrations of the Royal Greenwich Observatory. flattened gas-rich galaxies suggests that there might t Guest observer, 1975, Kitt Peak National Observatory. KPNO is operated by AURA Inc. under contract with the exist a class of flattened objects with characteristics National Science Foundation of the U.S.A. that are intermediate between those of SO galaxies and 883 © American Astronomical Society • Provided by the NASA Astrophysics Data System .883V .206. 884 VAN DEN BERGH Vol. 206 . Objects which, on the prints of the Hubble Atlas, 6ApJ. have apparent disk-to-bulge ratios in the range 1 to 3 have been classified Sa; those with disk-to-bulge ratios 197 of 3 to 10 were classified Sb; and those with disk-to- bulge ratios larger than 10 as Sc. An analogous defini- tion was used to define the anemic spirals of type Aa, Ab, and Ac. Similarly SO galaxies were also divided into types SOa, SOb, and SOc. It should be emphasized that this subdivision of galaxies of class SO is in no way PROPOSED CLASSIFICATION SYSTEM related to the Hubble-Sandage classification S0l5 S02, and S03, which does not depend on the relative im- portance of the central bulge and of the disk sub- systems. Many of the galaxies of Hubble-Sandage type EO E3 E6 z' "n Sa Sb Sc S0i fall on the S0a-S0b-S0c sequence in Figures 1 and i 1 T (so)—h H h 2. Most of the galaxies which have Hubble-Sandage type S03 are probably more closely related to the HUBBLE CLASSIFICATION SYSTEM anemic spirals than they are to true SO systems. Fig. 1.—Comparison of the provisional classification system The positions of the Sa-Sb-Sc, Aa-Ab-Ac, and proposed in this paper with that of Hubble (1936). The new S0a-S0b-S0c sequences in a diagram of color versus system comprises parallel sequences of normal spirals disk-to-bulge ratio are shown in Figure 3. (Sa-Sb-Sc), anemic spirals (Aa-Ab-Ac), and gas-free lentic- It should perhaps be emphasized that the role of SO ulars (S0a-S0b-S0c). galaxies in the classification system outlined above is very different from that originally envisaged by Hubble normal spirals. Such gas-poor objects, in which not (1936). Hubble thought of SO galaxies as a transitional much star formation is presently taking place, will be type between ellipticals and spirals. In the scheme referred to as “anemic” spirals. illustrated in Figures 1, 2, and 3, lenticular galaxies A new classification scheme for galaxies, which and spirals form parallel sequences which differ only incorporates a sequence of anemic spirals, is shown in in their gas content and hence in their rate of star Figures 1 and 2. In this provisional system, galaxies formation. without a disk component are called ellipticals In order to better define the new classification (E0-E6). The conventional Hubble classification of scheme proposed in this paper, all of the NGC normal spirals is replaced by a system which is based galaxies in The Hubble Atlas of Galaxies (Sandage entirely on their disk-to-bulge ratios. These disk-to- 1961) have been reclassified in the new system des- bulge ratios are, in a very crude way, related to the cribed above. The classifications were made using both relative importance of the two main components in the photographs in the Hubble Atlas and glass copies galaxies, i.e., the inner spheroidal component and the of the blue plates of the Palomar Sky Survey. These outer exponential disk (de Vaucouleurs 1959; Free- classifications, which are listed in Table 1, will be taken man 1970; Sándage, Freeman, and Stokes 1970). The to define the Revised David Dunlap Observatory disk-to-bulge ' ratio is also related to the nuclear (RDDO) system. concentration of light, which Morgan (1958, 1959) It should probably be emphasized that some features has used as a classification parameter. of this system are still quite provisional. In particular SOa SOb SOc Fig. 2.—Schematic representation of the proposed new galaxy classification system © American Astronomical Society • Provided by the NASA Astrophysics Data System .883V .206. No. 3, 1976 NEW CLASSIFICATION SYSTEM FOR GALAXIES 885 . it is not yet entirely clear how the sequence of barred and SO galaxies in very dense clusters such as Coma has 6ApJ. SO systems of differing disk-to-bulge ratio can be been known for many years (cf. Spitzer and Baade unambiguously classified. In Table 1 all classifications 1951). The differences between galaxies in more open 197 of SBO galaxies have therefore been placed in paren- clusters, such as Virgo, and those in the general field theses. are somewhat more subtle. The transition from type SO to type A is a continuous one. For purposes of classification both dusty and dust- a) Gas in Spirals free galaxies without evidence for a patchy distribu- tion of Population I have been assigned to the The following systematic differences are observed S0a-S0b-S0c sequence. Flattened objects, in which between spiral galaxies in the Virgo cluster and their some young Population I stars seemed to be present, counterparts in the field : were assigned to the Aa-Ab-Ac sequence. i) The average surface density of neutral hydrogen gas in Virgo spirals of a given type is only 0.5 ±0.1 III. GAS DEPLETION IN CLUSTER GALAXIES times that observed in noncluster spirals of the same type (Davies and Lewis 1973). A number of lines of evidence suggest that the ii) At a given disk-to-bulge ratio, Virgo spirals are galaxian population of rich clusters differs significantly systematically redder by 0.04 mag than are similar from that of field galaxies.
Recommended publications
  • The Puzzle of the Strange Galaxy Made of 99.9% Dark Matter Is Solved 13 October 2020
    The puzzle of the strange galaxy made of 99.9% dark matter is solved 13 October 2020 The galaxy Dragonfly 44 was discovered in a deep survey of the Coma cluster, a cluster with several thousand galaxies. From the start, the galaxy was considered remarkable by the researchers because the quantity of dark matter they inferred was almost as much as that in the Milky Way, the equivalent of a billion solar masses. However, instead of containing around a hundred thousand million stars, as has the Milky Way, DF44 has only a hundred million stars, a thousand times Image and amplification (in color) of the ultra-diffuse fewer. This means that the amount of dark matter galaxy Dragonfly 44 taken with the Hubble space was ten thousand times greater than that of its telescope. Credit: Teymoor Saifollahi and NASA/HST. stars. If this had been true, it would have been a unique object, with almost 100 times as much dark matter as that expected from the number of its stars. At present, the formation of galaxies is difficult to understand without the presence of a ubiquitous, Nevertheless, by an exhaustive analysis of the but mysterious component, termed dark matter. system of globular cluster around Dragonfly 44, the Astronomers have measure how much dark matter researchers have detected that the total number of there is around galaxies, and have found that it globular clusters is only 20, and that the total varies between 10 and 300 times the quantity of quantity of dark matter is around 300 times that of visible matter.
    [Show full text]
  • Infrared Spectroscopy of Nearby Radio Active Elliptical Galaxies
    The Astrophysical Journal Supplement Series, 203:14 (11pp), 2012 November doi:10.1088/0067-0049/203/1/14 C 2012. The American Astronomical Society. All rights reserved. Printed in the U.S.A. INFRARED SPECTROSCOPY OF NEARBY RADIO ACTIVE ELLIPTICAL GALAXIES Jeremy Mould1,2,9, Tristan Reynolds3, Tony Readhead4, David Floyd5, Buell Jannuzi6, Garret Cotter7, Laura Ferrarese8, Keith Matthews4, David Atlee6, and Michael Brown5 1 Centre for Astrophysics and Supercomputing Swinburne University, Hawthorn, Vic 3122, Australia; [email protected] 2 ARC Centre of Excellence for All-sky Astrophysics (CAASTRO) 3 School of Physics, University of Melbourne, Melbourne, Vic 3100, Australia 4 Palomar Observatory, California Institute of Technology 249-17, Pasadena, CA 91125 5 School of Physics, Monash University, Clayton, Vic 3800, Australia 6 Steward Observatory, University of Arizona (formerly at NOAO), Tucson, AZ 85719 7 Department of Physics, University of Oxford, Denys, Oxford, Keble Road, OX13RH, UK 8 Herzberg Institute of Astrophysics Herzberg, Saanich Road, Victoria V8X4M6, Canada Received 2012 June 6; accepted 2012 September 26; published 2012 November 1 ABSTRACT In preparation for a study of their circumnuclear gas we have surveyed 60% of a complete sample of elliptical galaxies within 75 Mpc that are radio sources. Some 20% of our nuclear spectra have infrared emission lines, mostly Paschen lines, Brackett γ , and [Fe ii]. We consider the influence of radio power and black hole mass in relation to the spectra. Access to the spectra is provided here as a community resource. Key words: galaxies: elliptical and lenticular, cD – galaxies: nuclei – infrared: general – radio continuum: galaxies ∼ 1. INTRODUCTION 30% of the most massive galaxies are radio continuum sources (e.g., Fabbiano et al.
    [Show full text]
  • A High Stellar Velocity Dispersion and ~100 Globular Clusters for the Ultra
    San Jose State University From the SelectedWorks of Aaron J. Romanowsky 2016 A High Stellar Velocity Dispersion and ~100 Globular Clusters for the Ultra-Diffuse Galaxy Dragonfly 44 Pieter van Dokkum, Yale University Roberto Abraham, University of Toronto Jean P. Brodie, University of California Observatories Charlie Conroy, Harvard-Smithsonian Center for Astrophysics Shany Danieli, Yale University, et al. Available at: https://works.bepress.com/aaron_romanowsky/117/ The Astrophysical Journal Letters, 828:L6 (6pp), 2016 September 1 doi:10.3847/2041-8205/828/1/L6 © 2016. The American Astronomical Society. All rights reserved. A HIGH STELLAR VELOCITY DISPERSION AND ∼100 GLOBULAR CLUSTERS FOR THE ULTRA-DIFFUSE GALAXY DRAGONFLY 44 Pieter van Dokkum1, Roberto Abraham2, Jean Brodie3, Charlie Conroy4, Shany Danieli1, Allison Merritt1, Lamiya Mowla1, Aaron Romanowsky3,5, and Jielai Zhang2 1 Astronomy Department, Yale University, New Haven, CT 06511, USA 2 Department of Astronomy & Astrophysics, University of Toronto, 50 St. George Street, Toronto, ON M5S 3H4, Canada 3 University of California Observatories, 1156 High Street, Santa Cruz, CA 95064, USA 4 Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA, USA 5 Department of Physics and Astronomy, San José State University, San Jose, CA 95192, USA Received 2016 June 20; revised 2016 July 14; accepted 2016 July 15; published 2016 August 25 ABSTRACT Recently a population of large, very low surface brightness, spheroidal galaxies was identified in the Coma cluster. The apparent survival of these ultra-diffuse galaxies (UDGs) in a rich cluster suggests that they have very high masses. Here, we present the stellar kinematics of Dragonfly44, one of the largest Coma UDGs, using a 33.5 hr fi +8 -1 integration with DEIMOS on the Keck II telescope.
    [Show full text]
  • Radio Continuum and CO Emission in Star-Forming Galaxies
    A&A 385, 412–424 (2002) Astronomy DOI: 10.1051/0004-6361:20020140 & c ESO 2002 Astrophysics Radio continuum and CO emission in star-forming galaxies M. Murgia1,A.Crapsi1,2, L. Moscadelli3, and L. Gregorini1,4 1 Istituto di Radioastronomia del CNR, Via Gobetti 101, 40129, Bologna, Italy 2 Osservatorio Astrofisico di Arcetri, Largo E. Fermi 5, 50125, Firenze, Italy 3 Osservatorio Astronomico di Cagliari, Loc. Poggio dei Pini, Strada 54, 09012 Capoterra (CA), Italy 4 Dipartimento di Fisica, Universit`a di Bologna, Via B. Pichat 6/2, 40127 Bologna, Italy Received 30 October 2001 / Accepted 23 January 2002 Abstract. We combine the radio continuum images from the NRAO VLA Sky Survey with the CO-line observations from the extragalactic CO survey of the Five College Radio Astronomy Observatory to study the relationship between molecular gas and the star formation rate within the disks of 180 spiral galaxies at 4500 resolution. We find a tight correlation between these quantities. On average, the ratio between the radio continuum and the CO emission is constant, within a factor of 3, both inside the same galaxy and from galaxy to galaxy. The mean star formation efficiency deduced from the radio continuum corresponds to convert 3.5% of the available molecular gas into stars on a time scale of 108 yr and depends weakly on general galaxy properties, such as Hubble type or nuclear activity. A comparison is made with another similar analysis performed using the Hα luminosity as star formation indicator. The overall agreement we find between the two studies reinforces the use of the radio luminosity as star formation rate indicator not only on global but also on local scales.
    [Show full text]
  • Stellar Tidal Streams As Cosmological Diagnostics: Comparing Data and Simulations at Low Galactic Scales
    RUPRECHT-KARLS-UNIVERSITÄT HEIDELBERG DOCTORAL THESIS Stellar Tidal Streams as Cosmological Diagnostics: Comparing data and simulations at low galactic scales Author: Referees: Gustavo MORALES Prof. Dr. Eva K. GREBEL Prof. Dr. Volker SPRINGEL Astronomisches Rechen-Institut Heidelberg Graduate School of Fundamental Physics Department of Physics and Astronomy 14th May, 2018 ii DISSERTATION submitted to the Combined Faculties of the Natural Sciences and Mathematics of the Ruperto-Carola-University of Heidelberg, Germany for the degree of DOCTOR OF NATURAL SCIENCES Put forward by GUSTAVO MORALES born in Copiapo ORAL EXAMINATION ON JULY 26, 2018 iii Stellar Tidal Streams as Cosmological Diagnostics: Comparing data and simulations at low galactic scales Referees: Prof. Dr. Eva K. GREBEL Prof. Dr. Volker SPRINGEL iv NOTE: Some parts of the written contents of this thesis have been adapted from a paper submitted as a co-authored scientific publication to the Astronomy & Astrophysics Journal: Morales et al. (2018). v NOTE: Some parts of this thesis have been adapted from a paper accepted for publi- cation in the Astronomy & Astrophysics Journal: Morales, G. et al. (2018). “Systematic search for tidal features around nearby galaxies: I. Enhanced SDSS imaging of the Local Volume". arXiv:1804.03330. DOI: 10.1051/0004-6361/201732271 vii Abstract In hierarchical models of galaxy formation, stellar tidal streams are expected around most galaxies. Although these features may provide useful diagnostics of the LCDM model, their observational properties remain poorly constrained. Statistical analysis of the counts and properties of such features is of interest for a direct comparison against results from numeri- cal simulations. In this work, we aim to study systematically the frequency of occurrence and other observational properties of tidal features around nearby galaxies.
    [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]
  • Radio Sources in Low-Luminosity Active Galactic Nuclei
    A&A 392, 53–82 (2002) Astronomy DOI: 10.1051/0004-6361:20020874 & c ESO 2002 Astrophysics Radio sources in low-luminosity active galactic nuclei III. “AGNs” in a distance-limited sample of “LLAGNs” N. M. Nagar1, H. Falcke2,A.S.Wilson3, and J. S. Ulvestad4 1 Arcetri Observatory, Largo E. Fermi 5, Florence 50125, Italy 2 Max-Planck-Institut f¨ur Radioastronomie, Auf dem H¨ugel 69, 53121 Bonn, Germany e-mail: [email protected] 3 Department of Astronomy, University of Maryland, College Park, MD 20742, USA Adjunct Astronomer, Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD 21218, USA e-mail: [email protected] 4 National Radio Astronomy Observatory, PO Box 0, Socorro, NM 87801, USA e-mail: [email protected] Received 23 January 2002 / Accepted 6 June 2002 Abstract. This paper presents the results of a high resolution radio imaging survey of all known (96) low-luminosity active galactic nuclei (LLAGNs) at D ≤ 19 Mpc. We first report new 2 cm (150 mas resolution using the VLA) and 6 cm (2 mas resolution using the VLBA) radio observations of the previously unobserved nuclei in our samples and then present results on the complete survey. We find that almost half of all LINERs and low-luminosity Seyferts have flat-spectrum radio cores when observed at 150 mas resolution. Higher (2 mas) resolution observations of a flux-limited subsample have provided a 100% (16 of 16) detection rate of pc-scale radio cores, with implied brightness temperatures ∼>108 K. The five LLAGNs with the highest core radio fluxes also have pc-scale “jets”.
    [Show full text]
  • April Constellations of the Month
    April Constellations of the Month Leo Small Scope Objects: Name R.A. Decl. Details M65! A large, bright Sa/Sb spiral galaxy. 7.8 x 1.6 arc minutes, magnitude 10.2. Very 11hr 18.9m +13° 05’ (NGC 3623) high surface brighness showing good detail in medium sized ‘scopes. M66! Another bright Sb galaxy, only 21 arc minutes from M65. Slightly brighter at mag. 11hr 20.2m +12° 59’ (NGC 3627) 9.7, measuring 8.0 x 2.5 arc minutes. M95 An easy SBb barred spiral, 4 x 3 arc minutes in size. Magnitude 10.5, with 10hr 44.0m +11° 42’ a bright central core. The bar and outer ring of material will require larger (NGC 3351) aperature and dark skies. M96 Another bright Sb spiral, about 42 arc minutes east of M95, but larger and 10hr 46.8m +11° 49’ (NGC 3368) brighter. 6 x 4 arc minutes, magnitude 10.1. Located about 48 arc minutes NNE of M96. This small elliptical galaxy measures M105 only 2 x 2.1 arc minutes, but at mag. 10.3 has very high surface brightness. 10hr 47.8m +12° 35’ (NGC 3379) Look for NGC 3384! (110NGC) and NGC 3389 (mag 11.0 and 12.2) which form a small triangle with M105. NGC 3384! 10hr 48.3m +12° 38’ See comment for M105. The brightest galaxy in Leo, this Sb/Sc spiral galaxy shines at mag. 9.5. Look for NGC 2903!! 09hr 32.2m +21° 30’ a hazy patch 11 x 4.7 arc minutes in size 1.5° south of l Leonis.
    [Show full text]
  • Spatially Resolved Stellar Kinematics of the Ultra-Diffuse Galaxy Dragonfly 44
    The Astrophysical Journal, 880:91 (26pp), 2019 August 1 https://doi.org/10.3847/1538-4357/ab2914 © 2019. The American Astronomical Society. All rights reserved. Spatially Resolved Stellar Kinematics of the Ultra-diffuse Galaxy Dragonfly 44. I. Observations, Kinematics, and Cold Dark Matter Halo Fits Pieter van Dokkum1 , Asher Wasserman2 , Shany Danieli1 , Roberto Abraham3 , Jean Brodie2 , Charlie Conroy4 , Duncan A. Forbes5, Christopher Martin6, Matt Matuszewski6, Aaron J. Romanowsky2,7 , and Alexa Villaume2 1 Astronomy Department, Yale University, 52 Hillhouse Avenue, New Haven, CT 06511, USA 2 University of California Observatories, 1156 High Street, Santa Cruz, CA 95064, USA 3 Department of Astronomy & Astrophysics, University of Toronto, 50 St. George Street, Toronto, ON M5S 3H4, Canada 4 Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA, USA 5 Centre for Astrophysics and Supercomputing, Swinburne University, Hawthorn, VIC 3122, Australia 6 Cahill Center for Astrophysics, California Institute of Technology, 1216 East California Boulevard, Mail Code 278-17, Pasadena, CA 91125, USA 7 Department of Physics and Astronomy, San José State University, San Jose, CA 95192, USA Received 2019 March 31; revised 2019 May 25; accepted 2019 June 5; published 2019 July 30 Abstract We present spatially resolved stellar kinematics of the well-studied ultra-diffuse galaxy (UDG) Dragonfly44, as determined from 25.3 hr of observations with the Keck Cosmic Web Imager. The luminosity-weighted dispersion +3 −1 within the half-light radius is s12= 33-3 km s , lower than what we had inferred before from a DEIMOS spectrum in the Hα region. There is no evidence for rotation, with Vmax áñ<s 0.12 (90% confidence) along the major axis, in possible conflict with models where UDGs are the high-spin tail of the normal dwarf galaxy distribution.
    [Show full text]
  • The Dynamical State of the Coma Cluster with XMM-Newton?
    A&A 400, 811–821 (2003) Astronomy DOI: 10.1051/0004-6361:20021911 & c ESO 2003 Astrophysics The dynamical state of the Coma cluster with XMM-Newton? D. M. Neumann1,D.H.Lumb2,G.W.Pratt1, and U. G. Briel3 1 CEA/DSM/DAPNIA Saclay, Service d’Astrophysique, L’Orme des Merisiers, Bˆat. 709, 91191 Gif-sur-Yvette, France 2 Science Payloads Technology Division, Research and Science Support Dept., ESTEC, Postbus 299 Keplerlaan 1, 2200AG Noordwijk, The Netherlands 3 Max-Planck Institut f¨ur extraterrestrische Physik, Giessenbachstr., 85740 Garching, Germany Received 19 June 2002 / Accepted 13 December 2002 Abstract. We present in this paper a substructure and spectroimaging study of the Coma cluster of galaxies based on XMM- Newton data. XMM-Newton performed a mosaic of observations of Coma to ensure a large coverage of the cluster. We add the different pointings together and fit elliptical beta-models to the data. We subtract the cluster models from the data and look for residuals, which can be interpreted as substructure. We find several significant structures: the well-known subgroup connected to NGC 4839 in the South-West of the cluster, and another substructure located between NGC 4839 and the centre of the Coma cluster. Constructing a hardness ratio image, which can be used as a temperature map, we see that in front of this new structure the temperature is significantly increased (higher or equal 10 keV). We interpret this temperature enhancement as the result of heating as this structure falls onto the Coma cluster. We furthermore reconfirm the filament-like structure South-East of the cluster centre.
    [Show full text]
  • Ram Pressure Stripping and Galaxy Orbits: the Case of the Virgo Cluster
    Ram pressure stripping and galaxy orbits: The case of the Virgo cluster B. Vollmer Max-Planck-Institut f¨ur Radioastronomie, Bonn, Germany and Observatoire de Paris, Meudon, France. V. Cayatte, C. Balkowski Observatoire de Paris, DAEC, UMR 8631, CNRS et Universit´e Paris 7, F-92195 Meudon Cedex, France. and W.J. Duschl1 Institut f¨ur Theoretische Astrophysik der Universit¨at Heidelberg, Tiergartenstraße 15, D-69121 Heidelberg, Germany. ABSTRACT We investigate the role of ram pressure stripping in the Virgo cluster using N-body simulations. Radial orbits within the Virgo cluster’s gravitational potential are modeled and analyzed with respect to ram pressure stripping. The N-body model consists of 10 000 gas cloud complexes which can have inelastic collisions. Ram pressure is modeled as an additional acceleration on the clouds located at the surface of the gas distribution in the direction of the galaxy’s motion within the cluster. We made several simulations changing the orbital parameters in order to recover different stripping scenarios using realistic temporal ram pressure profiles. We investigate systematically the influence of the inclination angle between the disk and the orbital plane of the galaxy on the gas dynamics. We show that ram pressure can lead to a temporary increase of the central gas surface density. In some cases a considerable part of the total atomic gas mass (several 108 M ) can fall back onto the galactic disk after the stripping event. A quantitative relation between the orbit parameters and the resulting Hi deficiency is derived containing explicitly the inclination angle between the disk and the orbital plane.
    [Show full text]
  • And Ecclesiastical Cosmology
    GSJ: VOLUME 6, ISSUE 3, MARCH 2018 101 GSJ: Volume 6, Issue 3, March 2018, Online: ISSN 2320-9186 www.globalscientificjournal.com DEMOLITION HUBBLE'S LAW, BIG BANG THE BASIS OF "MODERN" AND ECCLESIASTICAL COSMOLOGY Author: Weitter Duckss (Slavko Sedic) Zadar Croatia Pусскй Croatian „If two objects are represented by ball bearings and space-time by the stretching of a rubber sheet, the Doppler effect is caused by the rolling of ball bearings over the rubber sheet in order to achieve a particular motion. A cosmological red shift occurs when ball bearings get stuck on the sheet, which is stretched.“ Wikipedia OK, let's check that on our local group of galaxies (the table from my article „Where did the blue spectral shift inside the universe come from?“) galaxies, local groups Redshift km/s Blueshift km/s Sextans B (4.44 ± 0.23 Mly) 300 ± 0 Sextans A 324 ± 2 NGC 3109 403 ± 1 Tucana Dwarf 130 ± ? Leo I 285 ± 2 NGC 6822 -57 ± 2 Andromeda Galaxy -301 ± 1 Leo II (about 690,000 ly) 79 ± 1 Phoenix Dwarf 60 ± 30 SagDIG -79 ± 1 Aquarius Dwarf -141 ± 2 Wolf–Lundmark–Melotte -122 ± 2 Pisces Dwarf -287 ± 0 Antlia Dwarf 362 ± 0 Leo A 0.000067 (z) Pegasus Dwarf Spheroidal -354 ± 3 IC 10 -348 ± 1 NGC 185 -202 ± 3 Canes Venatici I ~ 31 GSJ© 2018 www.globalscientificjournal.com GSJ: VOLUME 6, ISSUE 3, MARCH 2018 102 Andromeda III -351 ± 9 Andromeda II -188 ± 3 Triangulum Galaxy -179 ± 3 Messier 110 -241 ± 3 NGC 147 (2.53 ± 0.11 Mly) -193 ± 3 Small Magellanic Cloud 0.000527 Large Magellanic Cloud - - M32 -200 ± 6 NGC 205 -241 ± 3 IC 1613 -234 ± 1 Carina Dwarf 230 ± 60 Sextans Dwarf 224 ± 2 Ursa Minor Dwarf (200 ± 30 kly) -247 ± 1 Draco Dwarf -292 ± 21 Cassiopeia Dwarf -307 ± 2 Ursa Major II Dwarf - 116 Leo IV 130 Leo V ( 585 kly) 173 Leo T -60 Bootes II -120 Pegasus Dwarf -183 ± 0 Sculptor Dwarf 110 ± 1 Etc.
    [Show full text]