Dwarf Galaxies and Stellar Clusters Review Articles
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A Revised View of the Canis Major Stellar Overdensity with Decam And
MNRAS 501, 1690–1700 (2021) doi:10.1093/mnras/staa2655 Advance Access publication 2020 October 14 A revised view of the Canis Major stellar overdensity with DECam and Gaia: new evidence of a stellar warp of blue stars Downloaded from https://academic.oup.com/mnras/article/501/2/1690/5923573 by Consejo Superior de Investigaciones Cientificas (CSIC) user on 15 March 2021 Julio A. Carballo-Bello ,1‹ David Mart´ınez-Delgado,2 Jesus´ M. Corral-Santana ,3 Emilio J. Alfaro,2 Camila Navarrete,3,4 A. Katherina Vivas 5 and Marcio´ Catelan 4,6 1Instituto de Alta Investigacion,´ Universidad de Tarapaca,´ Casilla 7D, Arica, Chile 2Instituto de Astrof´ısica de Andaluc´ıa, CSIC, E-18080 Granada, Spain 3European Southern Observatory, Alonso de Cordova´ 3107, Casilla 19001, Santiago, Chile 4Millennium Institute of Astrophysics, Santiago, Chile 5Cerro Tololo Inter-American Observatory, NSF’s National Optical-Infrared Astronomy Research Laboratory, Casilla 603, La Serena, Chile 6Instituto de Astrof´ısica, Facultad de F´ısica, Pontificia Universidad Catolica´ de Chile, Av. Vicuna˜ Mackenna 4860, 782-0436 Macul, Santiago, Chile Accepted 2020 August 27. Received 2020 July 16; in original form 2020 February 24 ABSTRACT We present the Dark Energy Camera (DECam) imaging combined with Gaia Data Release 2 (DR2) data to study the Canis Major overdensity. The presence of the so-called Blue Plume stars in a low-pollution area of the colour–magnitude diagram allows us to derive the distance and proper motions of this stellar feature along the line of sight of its hypothetical core. The stellar overdensity extends on a large area of the sky at low Galactic latitudes, below the plane, and in the range 230◦ <<255◦. -
Complex Stellar Populations in Massive Clusters: Trapping Stars of a Dwarf Disc Galaxy in a Newborn Stellar Supercluster
Mon. Not. R. Astron. Soc. 372, 338–342 (2006) doi:10.1111/j.1365-2966.2006.10867.x Complex stellar populations in massive clusters: trapping stars of a dwarf disc galaxy in a newborn stellar supercluster M. Fellhauer,1,3⋆ P. Kroupa2,3⋆ and N. W. Evans1⋆ 1Institute of Astronomy, University of Cambridge, Madingley Road, Cambridge CB3 0HA 2Argelander Institute for Astronomy, University of Bonn, Auf dem Hug¨ el 71, D-53121 Bonn, Germany 3The Rhine Stellar-Dynamical Network Accepted 2006 July 24. Received 2006 July 21; in original form 2006 April 27 ABSTRACT Some of the most-massive globular clusters of our Milky Way, such as, for example, ω Centauri, show a mixture of stellar populations spanning a few Gyr in age and 1.5 dex in metallicities. In contrast, standard formation scenarios predict that globular and open clusters form in one single starburst event of duration 10 Myr and therefore should exhibit only one age and one metallicity in its stars. Here, we investigate the possibility that a massive stellar supercluster may trap older galactic field stars during its formation process that are later detectable in the cluster as an apparent population of stars with a very different age and metallicity. With a set of numerical N-body simulations, we are able to show that, if the mass of the stellar supercluster is high enough and the stellar velocity dispersion in the cluster is comparable to the dispersion of the surrounding disc stars in the host galaxy, then up to about 40 per cent of its initial mass can be additionally gained from trapped disc stars. -
Introduction to Astronomy from Darkness to Blazing Glory
Introduction to Astronomy From Darkness to Blazing Glory Published by JAS Educational Publications Copyright Pending 2010 JAS Educational Publications All rights reserved. Including the right of reproduction in whole or in part in any form. Second Edition Author: Jeffrey Wright Scott Photographs and Diagrams: Credit NASA, Jet Propulsion Laboratory, USGS, NOAA, Aames Research Center JAS Educational Publications 2601 Oakdale Road, H2 P.O. Box 197 Modesto California 95355 1-888-586-6252 Website: http://.Introastro.com Printing by Minuteman Press, Berkley, California ISBN 978-0-9827200-0-4 1 Introduction to Astronomy From Darkness to Blazing Glory The moon Titan is in the forefront with the moon Tethys behind it. These are two of many of Saturn’s moons Credit: Cassini Imaging Team, ISS, JPL, ESA, NASA 2 Introduction to Astronomy Contents in Brief Chapter 1: Astronomy Basics: Pages 1 – 6 Workbook Pages 1 - 2 Chapter 2: Time: Pages 7 - 10 Workbook Pages 3 - 4 Chapter 3: Solar System Overview: Pages 11 - 14 Workbook Pages 5 - 8 Chapter 4: Our Sun: Pages 15 - 20 Workbook Pages 9 - 16 Chapter 5: The Terrestrial Planets: Page 21 - 39 Workbook Pages 17 - 36 Mercury: Pages 22 - 23 Venus: Pages 24 - 25 Earth: Pages 25 - 34 Mars: Pages 34 - 39 Chapter 6: Outer, Dwarf and Exoplanets Pages: 41-54 Workbook Pages 37 - 48 Jupiter: Pages 41 - 42 Saturn: Pages 42 - 44 Uranus: Pages 44 - 45 Neptune: Pages 45 - 46 Dwarf Planets, Plutoids and Exoplanets: Pages 47 -54 3 Chapter 7: The Moons: Pages: 55 - 66 Workbook Pages 49 - 56 Chapter 8: Rocks and Ice: -
Midwife of the Galactic Zoo
FOCUS 30 A miniature milky way: approximately 40 million light-years away, UGC 5340 is classified as a dwarf galaxy. Dwarf galaxies exist in a variety of forms – elliptical, spheroidal, spiral, or irregular – and originate in small halos of dark matter. Dwarf galaxies contain the oldest known stars. Max Planck Research · 4 | 2020 FOCUS MIDWIFE OF THE GALACTIC ZOO TEXT: THOMAS BÜHRKE 31 IMAGE: NASA, TEAM ESA & LEGUS Stars cluster in galaxies of dramatically different shapes and sizes: elliptical galaxies, spheroidal galaxies, lenticular galaxies, spiral galaxies, and occasionally even irregular galaxies. Nadine Neumayer at the Max Planck Institute for Astronomy in Heidelberg and Ralf Bender at the Max Planck Institute for Extraterrestrial Physics in Garching investigate the reasons for this diversity. They have already identified one crucial factor: dark matter. Max Planck Research · 4 | 2020 FOCUS Nature has bestowed an overwhelming diversity upon our planet. The sheer resourcefulness of the plant and animal world is seemingly inexhaustible. When scien- tists first started to explore this diversity, their first step was always to systematize it. Hence, the Swedish naturalist Carl von Linné established the principles of modern botany and zoology in the 18th century by clas- sifying organisms. In the last century, astronomers have likewise discovered that galaxies can come in an array of shapes and sizes. In this case, it was Edwin Hubble in the mid-1920s who systematized them. The “Hubble tuning fork dia- gram” classified elliptical galaxies according to their ellipticity. The series of elliptical galaxies along the di- PHOTO: PETER FRIEDRICH agram branches off into two arms: spiral galaxies with a compact bulge along the upper branch and galaxies with a central bar on the lower branch. -
Structure of the Outer Galactic Disc with Gaia DR2 Ž
A&A 637, A96 (2020) Astronomy https://doi.org/10.1051/0004-6361/201937289 & c ESO 2020 Astrophysics Structure of the outer Galactic disc with Gaia DR2 Ž. Chrobáková1,2, R. Nagy3, and M. López-Corredoira1,2 1 Instituto de Astrofísica de Canarias, 38205 La Laguna, Tenerife, Spain e-mail: [email protected] 2 Departamento de Astrofísica, Universidad de La Laguna, 38206 La Laguna, Tenerife, Spain 3 Faculty of Mathematics, Physics, and Informatics, Comenius University, Mlynská dolina, 842 48 Bratislava, Slovakia Received 9 December 2019 / Accepted 31 March 2020 ABSTRACT Context. The structure of outer disc of our Galaxy is still not well described, and many features need to be better understood. The second Gaia data release (DR2) provides data in unprecedented quality that can be analysed to shed some light on the outermost parts of the Milky Way. Aims. We calculate the stellar density using star counts obtained from Gaia DR2 up to a Galactocentric distance R = 20 kpc with a deconvolution technique for the parallax errors. Then we analyse the density in order to study the structure of the outer Galactic disc, mainly the warp. Methods. In order to carry out the deconvolution, we used the Lucy inversion technique for recovering the corrected star counts. We also used the Gaia luminosity function of stars with MG < 10 to extract the stellar density from the star counts. Results. The stellar density maps can be fitted by an exponential disc in the radial direction hr = 2:07 ± 0:07 kpc, with a weak dependence on the azimuth, extended up to 20 kpc without any cut-off. -
Arxiv:1802.01493V7 [Astro-Ph.GA] 10 Feb 2021 Ceeainbtti Oe Eoe Rbeai Tselrsae.I Scales
Variable Modified Newtonian Mechanics II: Baryonic Tully Fisher Relation C. C. Wong Department of Electrical and Electronic Engineering, University of Hong Kong. H.K. (Dated: February 11, 2021) Recently we find a single-metric solution for a point mass residing in an expanding universe [1], which apart from the Newtonian acceleration, gives rise to an additional MOND-like acceleration in which the MOND acceleration a0 is replaced by the cosmological acceleration. We study a Milky Way size protogalactic cloud in this acceleration, in which the growth of angular momentum can lead to an end of the overdensity growth. Within realistic redshifts, the overdensity stops growing at a value where the MOND-like acceleration dominates over Newton and the outer mass shell rotational velocity obeys the Baryonic Tully Fisher Relation (BTFR) with a smaller MOND acceleration. As the outer mass shell shrinks to a few scale length distances, the rotational velocity BTFR persists due to the conservation of angular momentum and the MOND acceleration grows to the phenomenological MOND acceleration value a0 at late time. PACS numbers: ?? INTRODUCTION A common response to the non-Newtonian rotational curve of a galaxy is that its ”Newtonian” dynamics requires cold dark matter (DM) particles. However, the small observed scatter of empirical Baryonic Tully-Fisher Relation (BTFR) of gas rich galaxies, see McGaugh [2]-Lelli [3], Milgrom [4] and Sanders [5], continues to motivate the hunt for a non-Newtonian connection between the rotational speeds and the baryon mass. On the modified DM theory front, Khoury [6] proposes a DM Bose-Einstein Condensate (BEC) phase where DM can interact more strongly with baryons. -
The Large Scale Universe As a Quasi Quantum White Hole
International Astronomy and Astrophysics Research Journal 3(1): 22-42, 2021; Article no.IAARJ.66092 The Large Scale Universe as a Quasi Quantum White Hole U. V. S. Seshavatharam1*, Eugene Terry Tatum2 and S. Lakshminarayana3 1Honorary Faculty, I-SERVE, Survey no-42, Hitech city, Hyderabad-84,Telangana, India. 2760 Campbell Ln. Ste 106 #161, Bowling Green, KY, USA. 3Department of Nuclear Physics, Andhra University, Visakhapatnam-03, AP, India. Authors’ contributions This work was carried out in collaboration among all authors. Author UVSS designed the study, performed the statistical analysis, wrote the protocol, and wrote the first draft of the manuscript. Authors ETT and SL managed the analyses of the study. All authors read and approved the final manuscript. Article Information Editor(s): (1) Dr. David Garrison, University of Houston-Clear Lake, USA. (2) Professor. Hadia Hassan Selim, National Research Institute of Astronomy and Geophysics, Egypt. Reviewers: (1) Abhishek Kumar Singh, Magadh University, India. (2) Mohsen Lutephy, Azad Islamic university (IAU), Iran. (3) Sie Long Kek, Universiti Tun Hussein Onn Malaysia, Malaysia. (4) N.V.Krishna Prasad, GITAM University, India. (5) Maryam Roushan, University of Mazandaran, Iran. Complete Peer review History: http://www.sdiarticle4.com/review-history/66092 Received 17 January 2021 Original Research Article Accepted 23 March 2021 Published 01 April 2021 ABSTRACT We emphasize the point that, standard model of cosmology is basically a model of classical general relativity and it seems inevitable to have a revision with reference to quantum model of cosmology. Utmost important point to be noted is that, ‘Spin’ is a basic property of quantum mechanics and ‘rotation’ is a very common experience. -
An Extended Star Formation History in an Ultra-Compact Dwarf
MNRAS 451, 3615–3626 (2015) doi:10.1093/mnras/stv1221 An extended star formation history in an ultra-compact dwarf Mark A. Norris,1‹ Carlos G. Escudero,2,3,4 Favio R. Faifer,2,3,4 Sheila J. Kannappan,5 Juan Carlos Forte4,6 and Remco C. E. van den Bosch1 1Max Planck Institut fur¨ Astronomie, Konigstuhl¨ 17, D-69117 Heidelberg, Germany 2Facultad de Cs. Astronomicas´ y Geof´ısicas, UNLP, Paseo del Bosque S/N, 1900 La Plata, Argentina 3Instituto de Astrof´ısica de La Plata (CCT La Plata – CONICET – UNLP), Paseo del Bosque S/N, 1900 La Plata, Argentina 4Consejo Nacional de Investigaciones Cient´ıficas y Tecnicas,´ Rivadavia 1917, C1033AAJ Ciudad Autonoma´ de Buenos Aires, Argentina 5Department of Physics and Astronomy UNC-Chapel Hill, CB 3255, Phillips Hall, Chapel Hill, NC 27599-3255, USA 6Planetario Galileo Galilei, Secretar´ıa de Cultura, Ciudad Autonoma´ de Buenos Aires, Argentina Accepted 2015 May 29. Received 2015 May 28; in original form 2015 April 2 ABSTRACT Downloaded from There has been significant controversy over the mechanisms responsible for forming compact stellar systems like ultra-compact dwarfs (UCDs), with suggestions that UCDs are simply the high-mass extension of the globular cluster population, or alternatively, the liberated nuclei of galaxies tidally stripped by larger companions. Definitive examples of UCDs formed by either route have been difficult to find, with only a handful of persuasive examples of http://mnras.oxfordjournals.org/ stripped-nucleus-type UCDs being known. In this paper, we present very deep Gemini/GMOS spectroscopic observations of the suspected stripped-nucleus UCD NGC 4546-UCD1 taken in good seeing conditions (<0.7 arcsec). -
Does the Fornax Dwarf Spheroidal Have a Central Cusp Or Core?
Research Collection Journal Article Does the Fornax dwarf spheroidal have a central cusp or core? Author(s): Goerdt, Tobias; Moore, Ben; Read, J.I.; Stadel, Joachim; Zemp, Marcel Publication Date: 2006-05 Permanent Link: https://doi.org/10.3929/ethz-b-000024289 Originally published in: Monthly Notices of the Royal Astronomical Society 368(3), http://doi.org/10.1111/ j.1365-2966.2006.10182.x Rights / License: In Copyright - Non-Commercial Use Permitted This page was generated automatically upon download from the ETH Zurich Research Collection. For more information please consult the Terms of use. ETH Library Mon. Not. R. Astron. Soc. 368, 1073–1077 (2006) doi:10.1111/j.1365-2966.2006.10182.x Does the Fornax dwarf spheroidal have a central cusp or core? , Tobias Goerdt,1 Ben Moore,1 J. I. Read,1 Joachim Stadel1 and Marcel Zemp1 2 1Institute for Theoretical Physics, University of Zurich,¨ Winterthurerstrasse 190, CH-8057 Zurich,¨ Switzerland 2Institute of Astronomy, ETH Zurich,¨ ETH Honggerberg¨ HPF D6, CH-8093 Zurich,¨ Switzerland Accepted 2006 February 8. Received 2006 February 7; in original form 2005 December 21 ABSTRACT The dark matter dominated Fornax dwarf spheroidal has five globular clusters orbiting at ∼1 kpc from its centre. In a cuspy cold dark matter halo the globulars would sink to the centre from their current positions within a few Gyr, presenting a puzzle as to why they survive undigested at the present epoch. We show that a solution to this timing problem is to adopt a cored dark matter halo. We use numerical simulations and analytic calculations to show that, under these conditions, the sinking time becomes many Hubble times; the globulars effectively stall at the dark matter core radius. -
Dusty Star-Forming Galaxies and Supermassive Black Holes at High Redshifts: in Situ Coevolution
SISSA - International School for Advanced Studies Dusty Star-Forming Galaxies and Supermassive Black Holes at High Redshifts: In Situ Coevolution Thesis Submitted for the Degree of “Doctor Philosophiæ” Supervisors Candidate Prof. Andrea Lapi Claudia Mancuso Prof. Gianfranco De Zotti Prof. Luigi Danese October 2016 ii To my fiancè Federico, my sister Ilaria, my mother Ennia, Gaia and Luna, my Big family. "Quando canterai la tua canzone, la canterai con tutto il tuo volume, che sia per tre minuti o per la vita, avrá su il tuo nome." Luciano Ligabue Contents Declaration of Authorship xi Abstract xiii 1 Introduction 1 2 Star Formation in galaxies 9 2.1 Initial Mass Function (IMF) and Stellar Population Synthesis (SPS) . 10 2.1.1 SPS . 12 2.2 Dust in galaxies . 12 2.3 Spectral Energy Distribution (SED) . 15 2.4 SFR tracers . 19 2.4.1 Emission lines . 20 2.4.2 X-ray flux . 20 2.4.3 UV luminosity . 20 2.4.4 IR emission . 21 2.4.5 UV vs IR . 22 2.4.6 Radio emission . 23 3 Star Formation Rate Functions 25 3.1 Reconstructing the intrinsic SFR function . 25 3.1.1 Validating the SFR functions via indirect observables . 29 3.1.2 Validating the SFRF via the continuity equation . 32 3.2 Linking to the halo mass via the abundance matching . 35 4 Hunting dusty star-forming galaxies at high-z 43 4.1 Selecting dusty galaxies in the far-IR/(sub-)mm band . 43 iii iv CONTENTS 4.2 Dusty galaxies are not lost in the UV band . -
THE MAGELLANIC CLOUDS NEWSLETTER an Electronic Publication Dedicated to the Magellanic Clouds, and Astrophysical Phenomena Therein
THE MAGELLANIC CLOUDS NEWSLETTER An electronic publication dedicated to the Magellanic Clouds, and astrophysical phenomena therein No. 115 — 2 February 2012 http://www.astro.keele.ac.uk/MCnews Editor: Jacco van Loon Figure 1: The Small Magellanic Cloud and Galactic globular cluster 47 Tucanae, two of the most beautiful objects in the Southern sky (from Kalirai et al. 2012; South is up and East is to the right). Image courtesy of and c Stephane Guisard, http://www.astrosurf.com/sguisard 1 Editorial Dear Colleagues, It is my pleasure to present you the 115th issue of the Magellanic Clouds Newsletter. There is a lot of attention to star clusters, pulsating stars, binary stars, and the dynamics of the Magellanic System; don’t miss some of the very interesting proceedings papers. It is not yet too late to register for the workshop on mass return from stars to galaxies, at STScI in March, but abstracts need to be in by 3 February (!): http://www.stsci.edu/institute/conference/mass-loss-return The next meeting which should be of interest to readers of this newsletter, is the Magellanic Clouds meeting in Perth, Australia in September – see the announcement at the end of the newsletter for more details. Thanks to those of you who supplied illustrations for this issue. They remain welcome. Also, don’t hesitate to use the ”announcement” type of submission to post results, ideas, requests for observations, et cetera. This is a forum, for discussion and collaboration. The next issue is planned to be distributed on the 1st of April 2012. -
The Milky Way Galaxy Contents Summary
UNESCO EOLSS ENCYCLOPEDIA The Milky Way galaxy James Binney Physics Department Oxford University Key Words: Milky Way, galaxies Contents Summary • Introduction • Recognition of the size of the Milky Way • The Centre • The bulge-bar • History of the bulge Globular clusters • Satellites • The disc • Spiral structure Interstellar gas Moving groups, associations and star clusters The thick disc Local mass density The dark halo • Summary Our Galaxy is typical of the galaxies that dominate star formation in the present Universe. It is a barred spiral galaxy – a still-forming disc surrounds an old and barred spheroid. A massive black hole marks the centre of the Galaxy. The Sun sits far out in the disc and in visible light our view of the Galaxy is limited by interstellar dust. Consequently, the large-scale structure of the Galaxy must be inferred from observations made at infrared and radio wavelengths. The central bar and spiral structure in the stellar disc generate significant non-axisymmetric gravitational forces that make the gas disc and its embedded star formation strongly non-axisymmetric. Molecular hydrogen is more centrally concentrated than atomic hydrogen and much of it is contained in molecular clouds within which stars form. Probably all stars are formed in an association or cluster, and energy released by the more massive stars quickly disperses gas left over from their birth. This dispersal of residual gas usually leads to the dissolution of the association or cluster. The stellar disc can be decomposed to a thin disc, which comprises stars formed over most of the Galaxy’s lifetime, and a thick disc, which contains only stars formed in about the Galaxy’s first gigayear.