Abundance Patterns in the Draco, Sextans and Ursa Minor Dwarf
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												  Astronomie in Theorie Und Praxis 8. Auflage in Zwei Bänden Erik WischnewskiAstronomie in Theorie und Praxis 8. Auflage in zwei Bänden Erik Wischnewski Inhaltsverzeichnis 1 Beobachtungen mit bloßem Auge 37 Motivation 37 Hilfsmittel 38 Drehbare Sternkarte Bücher und Atlanten Kataloge Planetariumssoftware Elektronischer Almanach Sternkarten 39 2 Atmosphäre der Erde 49 Aufbau 49 Atmosphärische Fenster 51 Warum der Himmel blau ist? 52 Extinktion 52 Extinktionsgleichung Photometrie Refraktion 55 Szintillationsrauschen 56 Angaben zur Beobachtung 57 Durchsicht Himmelshelligkeit Luftunruhe Beispiel einer Notiz Taupunkt 59 Solar-terrestrische Beziehungen 60 Klassifizierung der Flares Korrelation zur Fleckenrelativzahl Luftleuchten 62 Polarlichter 63 Nachtleuchtende Wolken 64 Haloerscheinungen 67 Formen Häufigkeit Beobachtung Photographie Grüner Strahl 69 Zodiakallicht 71 Dämmerung 72 Definition Purpurlicht Gegendämmerung Venusgürtel Erdschattenbogen 3 Optische Teleskope 75 Fernrohrtypen 76 Refraktoren Reflektoren Fokus Optische Fehler 82 Farbfehler Kugelgestaltsfehler Bildfeldwölbung Koma Astigmatismus Verzeichnung Bildverzerrungen Helligkeitsinhomogenität Objektive 86 Linsenobjektive Spiegelobjektive Vergütung Optische Qualitätsprüfung RC-Wert RGB-Chromasietest Okulare 97 Zusatzoptiken 100 Barlow-Linse Shapley-Linse Flattener Spezialokulare Spektroskopie Herschel-Prisma Fabry-Pérot-Interferometer Vergrößerung 103 Welche Vergrößerung ist die Beste? Blickfeld 105 Lichtstärke 106 Kontrast Dämmerungszahl Auflösungsvermögen 108 Strehl-Zahl Luftunruhe (Seeing) 112 Tubusseeing Kuppelseeing Gebäudeseeing Montierungen 113 Nachführfehler
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												  A Search for Ionized Gas in the Draco and Ursa Minor Dwarf Spheroidal GalaxiesView metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server A Search for Ionized Gas in the Draco and Ursa Minor Dwarf Spheroidal Galaxies J.S. Gallagher, G. J. Madsen, R. J. Reynolds Department of Astronomy, University of Wisconsin–Madison, 475 North Charter Street, Madison, WI 53706-1582; [email protected], [email protected], [email protected] E. K. Grebel Max-Planck Institute for Astronomy, K¨onigstuhl 17, D-69117 Heidelberg, Germany; [email protected] T. A. Smecker-Hane Department of Physics & Astronomy, 4129 Frederick Reines Hall, University of California, Irvine, CA 92697-4575; [email protected] ABSTRACT The Wisconsin Hα Mapper has been used to set the first deep upper limits on the intensity of diffuse Hα emission from warm ionized gas in the Draco and Ursa Minor dwarf spheroidal 1 galaxies. Assuming a velocity dispersion of 15 km s− for the ionized gas, we set limits of IHα 0:024R and IHα 0:021R for the Draco and Ursa Minor dSphs, respectively, averaged ≤ ≤ over our 1◦ circular beam. Adopting a simple model for the ionized interstellar medium, these limits translate to upper bounds on the mass of ionized gas of .10% of the stellar mass, or 10 times the upper limits for the mass of neutral hydrogen. Note that the Draco and Ursa Minor∼ dSphs could contain substantial amounts of interstellar gas, equivalent to all of the gas injected by dying stars since the end of their main star forming episodes &8 Gyr in the past, without violating these limits on the mass of ionized gas.
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												  Plotting Variable Stars on the H-R Diagram ActivityPulsating Variable Stars and the Hertzsprung-Russell Diagram The Hertzsprung-Russell (H-R) Diagram: The H-R diagram is an important astronomical tool for understanding how stars evolve over time. Stellar evolution can not be studied by observing individual stars as most changes occur over millions and billions of years. Astrophysicists observe numerous stars at various stages in their evolutionary history to determine their changing properties and probable evolutionary tracks across the H-R diagram. The H-R diagram is a scatter graph of stars. When the absolute magnitude (MV) – intrinsic brightness – of stars is plotted against their surface temperature (stellar classification) the stars are not randomly distributed on the graph but are mostly restricted to a few well-defined regions. The stars within the same regions share a common set of characteristics. As the physical characteristics of a star change over its evolutionary history, its position on the H-R diagram The H-R Diagram changes also – so the H-R diagram can also be thought of as a graphical plot of stellar evolution. From the location of a star on the diagram, its luminosity, spectral type, color, temperature, mass, age, chemical composition and evolutionary history are known. Most stars are classified by surface temperature (spectral type) from hottest to coolest as follows: O B A F G K M. These categories are further subdivided into subclasses from hottest (0) to coolest (9). The hottest B stars are B0 and the coolest are B9, followed by spectral type A0. Each major spectral classification is characterized by its own unique spectra.
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												  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.
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												  Variable Star Section CircularBritish Astronomical Association Variable Star Section Circular No 82, December 1994 CONTENTS A New Director 1 Credit for Observations 1 Submission of 1994 Observations 1 Chart Problems 1 Recent Novae Named 1 Z Ursae Minoris - A New R CrB Star? 2 The February 1995 Eclipse of 0¼ Geminorum 2 Computerisation News - Dave McAdam 3 'Stella Haitland, or Love and the Stars' - Philip Hurst 4 The 1994 Outburst of UZ Bootis - Gary Poyner 5 Observations of Betelgeuse by the SPA-VSS - Tony Markham 6 The AAVSO and the Contribution of Amateurs to VS Research Suspected Variables - Colin Henshaw 8 From the Literature 9 Eclipsing Binary Predictions 11 Summaries of IBVS's Nos 4040 to 4092 14 The BAA Instruments and Imaging Section Newsletter 16 Light-curves (TZ Per, R CrB, SV Sge, SU Tau, AC Her) - Dave McAdam 17 ISSN 0267-9272 Office: Burlington House, Piccadilly, London, W1V 9AG Section Officers Director Tristram Brelstaff, 3 Malvern Court, Addington Road, READING, Berks, RG1 5PL Tel: 0734-268981 Section Melvyn D Taylor, 17 Cross Lane, WAKEFIELD, Secretary West Yorks, WF2 8DA Tel: 0924-374651 Chart John Toone, Hillside View, 17 Ashdale Road, Cressage, Secretary SHREWSBURY, SY5 6DT Tel: 0952-510794 Computer Dave McAdam, 33 Wrekin View, Madeley, TELFORD, Secretary Shropshire, TF7 5HZ Tel: 0952-432048 E-mail: COMPUSERV 73671,3205 Nova/Supernova Guy M Hurst, 16 Westminster Close, Kempshott Rise, Secretary BASINGSTOKE, Hants, RG22 4PP Tel & Fax: 0256-471074 E-mail: [email protected] [email protected] Pro-Am Liaison Roger D Pickard, 28 Appletons, HADLOW, Kent TN11 0DT Committee Tel: 0732-850663 Secretary E-mail: [email protected] KENVAD::RDP Eclipsing Binary See Director Secretary Circulars Editor See Director Telephone Alert Numbers Nova and First phone Nova/Supernova Secretary.
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												  National Optical Astronomy ObservatoriesE NATIONAL OPTICAL ASTRONOMY OBSERVATORIES Preprint Series NOAO Preprint No. 834 WFPC2 OBSERVATIONS OF THE URSA MINOR DWARF SPHEROIDAL GALAXY KENNETH J. MIGHELL CHRISTOPHER J. BURKE To Appear In: The Astrophysical Journal March 1999 Operated for the National Science Foundation by the Association of Universities for Research in Astronomy, Inc. To appear in the Astronomical Journal (accepted 1999 March 1) WFPC2 OBSERVATIONS OF THE URSA MINOR DWARF SPHEROIDAL GALAXY 1 KENNETH J. _'IIGHELL 2 AND CHRISTOPHER J. BURKE 3'4 Kitt Peak National Observatory, National Optical Astronomy Observatories 5, P. O. Box 2673:2, Tucson, AZ 85726 mighell@noao, edu, chrislopt_ r. burk_ @yale.cdu 1Based on observations made with tile NASA/ESA Hubble Space Telescope, obtained fl'om the data archive at the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc. under NASA contract NAS5-26555. 2Guest User, Canadian Astronomy Data Centre, which is operated by the Dominion Astrophysical Observatory for the National Research Council of Canada's Herzberg Institute of Astrophysics. ZBased on research conducted at. NOAO as part of the Research Experiences for Undergraduates program. 4 Current address: Department of Astronomy, Yale University, P. O. Box 208101, New ttaven, CT 06520-8101 SNOAO is operated by the Association of Universilies for I/esearch in Astronomy, Inc., under cooperative agreelnent with the National Science Foundation. _ ABSTRACT \Ve present our analysis of archival Hubble Space Telescope Wide Field Planetary Canlera 2 (WFPC2) observations in F555W (,-_V) and F814W (_I) of the central region of the Ursa Minor dwarf spheroidal galaxy.
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												  Dark Matter Searches Targeting Dwarf Spheroidal Galaxies with the Fermi Large Area TelescopeDoctoral Thesis in Physics Dark Matter searches targeting Dwarf Spheroidal Galaxies with the Fermi Large Area Telescope Maja Garde Lindholm Oskar Klein Centre for Cosmoparticle Physics and Cosmology, Particle Astrophysics and String Theory Department of Physics Stockholm University SE-106 91 Stockholm Stockholm, Sweden 2015 Cover image: Top left: Optical image of the Carina dwarf galaxy. Credit: ESO/G. Bono & CTIO. Top center: Optical image of the Fornax dwarf galaxy. Credit: ESO/Digitized Sky Survey 2. Top right: Optical image of the Sculptor dwarf galaxy. Credit:ESO/Digitized Sky Survey 2. Bottom images are corresponding count maps from the Fermi Large Area Tele- scope. Figures 1.1a, 1.2, 1.3, and 4.2 used with permission. ISBN 978-91-7649-224-6 (pp. i{xxii, 1{120) pp. i{xxii, 1{120 c Maja Garde Lindholm, 2015 Printed by Publit, Stockholm, Sweden, 2015. Typeset in pdfLATEX Abstract In this thesis I present our recent work on gamma-ray searches for dark matter with the Fermi Large Area Telescope (Fermi-LAT). We have tar- geted dwarf spheroidal galaxies since they are very dark matter dominated systems, and we have developed a novel joint likelihood method to com- bine the observations of a set of targets. In the first iteration of the joint likelihood analysis, 10 dwarf spheroidal galaxies are targeted and 2 years of Fermi-LAT data is analyzed. The re- sulting upper limits on the dark matter annihilation cross-section range 26 3 1 from about 10− cm s− for dark matter masses of 5 GeV to about 5 10 23 cm3 s 1 for dark matter masses of 1 TeV, depending on the × − − annihilation channel.
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												  Constraints on the Parameters of Radiatively Decaying Dark Matter from the Dark Matter Halos of the Milky Way and Ursa MinorA&A 471, 51–57 (2007) Astronomy DOI: 10.1051/0004-6361:20066774 & c ESO 2007 Astrophysics Constraints on the parameters of radiatively decaying dark matter from the dark matter halos of the Milky Way and Ursa Minor A. Boyarsky1,2,3, J. Nevalainen4, and O. Ruchayskiy5,2 1 CERN, PH-TH, 1211 Geneve 23, Switzerland e-mail: [email protected] 2 École Polytechnique Fédérale de Lausanne, Institute of Theoretical Physics, FSB/ITP/LPPC, BSP 720, 1015 Lausanne, Switzerland 3 On leave of absence from Bogolyubov Institute of Theoretical Physics, Kyiv, Ukraine 4 Helsinki University Observatory, Finland e-mail: [email protected] 5 Institut des Hautes Études Scientifiques, 91440 Bures-sur-Yvette, France e-mail: [email protected] Received 20 November 2006 / Accepted 19 April 2007 ABSTRACT Aims. We improve the earlier restrictions on parameters of the warm dark matter (DM) in the form of a sterile neutrinos. Methods. The results were obtained from not observing the DM decay line in the X-ray spectrum of the Milky Way (using the recent XMM-Newton PN blank sky data). We also present a similar constraint coming from the recent XMM-Newton observation of Ursa Minor – dark, X-ray quiet dwarf spheroidal galaxy. Results. The new Milky way data improve on (by as much as the order of magnitude at masses ∼3.5 keV) existing constraints. Although the observation of Ursa Minor has relatively poor statistics, the constraints are comparable to those recently obtained using observations of the Large Magellanic Cloud or M 31. This confirms a recent proposal that dwarf satellites of the MW are very interesting candidates for the DM search and dedicated studies should be made to this purpose.
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												  A Search for Ionized Gas in the Draco and Ursa Minor Dwarf Spheroidal Galaxies JThe Astrophysical Journal, 588:326–330, 2003 May 1 # 2003. The American Astronomical Society. All rights reserved. Printed in U.S.A. A SEARCH FOR IONIZED GAS IN THE DRACO AND URSA MINOR DWARF SPHEROIDAL GALAXIES J. S. Gallagher, G. J. Madsen, and R. J. Reynolds Department of Astronomy, University of Wisconsin, 475 North Charter Street, Madison, WI 53706-1582; [email protected], [email protected], [email protected] E. K. Grebel Max-Planck-Institut fu¨r Astronomie, Ko¨nigstuhl 17, D-69117 Heidelberg, Germany; [email protected] and T. A. Smecker-Hane Department of Physics and Astronomy, 4129 Frederick Reines Hall, University of California, Irvine, CA 92697-4575; [email protected] Received 2002 December 6; accepted 2003 January 13 ABSTRACT The Wisconsin H Mapper has been used to set the first deep upper limits on the intensity of diffuse H emission from warm ionized gas in the Draco and Ursa Minor dwarf spheroidal galaxies (dSphs). Assuming À1 a velocity dispersion of 15 km s for the ionized gas, we set limits of IH 0:024 R and IH 0:021 R for the Draco and Ursa Minor dSphs, respectively, averaged over our 1 circular beam. Adopting a simple model for the ionized interstellar medium, these limits translate to upper bounds on the mass of ionized gas of d10% of the stellar mass, or 10 times the upper limits for the mass of neutral hydrogen. Note that the Draco and Ursa Minor dSphs could contain substantial amounts of interstellar gas, equivalent to all of the gas injected by dying stars since the end of their main star-forming episodes e8 Gyr in the past, without violating these limits on the mass of ionized gas.
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												  Supernova-Driven Outflows and Chemical Evolution of Dwarf Spheroidal GalaxiesSupernova-driven outflows and chemical evolution of dwarf spheroidal galaxies Yong-Zhong Qiana,1 and G. J. Wasserburgb,1 aSchool of Physics and Astronomy, University of Minnesota, Minneapolis, MN 55455; and bThe Lunatic Asylum, Division of Geological and Planetary Sciences, California Institute of Technology, Pasadena, CA 91125 Contributed by G. J. Wasserburg, January 30, 2012 (sent for review October 13, 2011) We present a general phenomenological model for the metallicity Recent observations (14) give results for eight dSphs with rather distribution (MD) in terms of ½Fe∕H for dwarf spheroidal galaxies detailed structure of their MDs and provide a basis for exploring (dSphs). These galaxies appear to have stopped accreting gas from models of their chemical evolution (e.g., ref. 15). Among the key the intergalactic medium and are fossilized systems with their stars issues that we try to address are MDs exhibited by stellar popula- undergoing slow internal evolution. For a wide variety of infall his- tions of dSphs. Our general approach follows that of Lynden-Bell tories of unprocessed baryonic matter to feed star formation, most described in his incisive and excellent article on “theories” of the of the observed MDs can be well described by our model. The key chemical evolution of galaxies (16). It will be shown that the me- requirement is that the fraction of the gas mass lost by supernova- tallicity at which the MD peaks is directly related to the efficiency driven outflows is close to unity. This model also predicts a relation- of SN-driven outflows and that the MD of a dSph and the rela- ship between the total stellar mass and the mean metallicity for tionship between the stellar mass and the mean metallicity for dSphs in accord with properties of their dark matter halos.
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												  Kinematics of the Dwarf Spheroidal Galaxies Draco and Ursa MinorUniversity of Groningen Kapteyn Astronomical Institute Kinematics of the dwarf spheroidal galaxies Draco and Ursa Minor MSc Thesis in Astronomy by Johanna Hartke Groningen, August 14, 2015 Supervisors Second Reader Prof. Dr. Eline Tolstoy Prof. Dr. Scott Trager Dr. Shoko Jin Dr. Maarten Breddels Abstract The aim of this thesis is to study the kinematics of the Local Group dwarf spheroidal galaxies Ursa Minor and Draco. These two galaxies are an interesting pair to study, since they are similar in terms of mass, extent, and distance. However, while Draco appears to have a perfect, undisturbed stellar distribution, Ursa Minor shows signs of tidal disturbance. We use new optical spectroscopy of individual red gi- ant branch stars from the AF2-WYFFOS fiber spectrograph on the William Herschel Telescope. We observed several hundred stars in the CaII triplet region. The data have been pipeline-processed at CASU in Cambridge using prototype WEAVE pro- cessing. We combine our dataset of Draco with data published by Walker, Olszewski & Mateo (2015) and apply orbit-based Schwarzschild modeling to the velocity data in order to constrain the dwarf spheroidal's (dark) matter distribution. We are able to determine the dark matter halo mass distribution for a NFW and a cored profile. Page 1 of 58 Contents 1 Introduction 4 1.1 Galaxy Formation . .5 1.2 Local Group dSph galaxies . .6 1.2.1 Draco . .7 1.2.2 Ursa Minor . .8 1.3 Dynamical modeling . .8 1.3.1 Early attempts to model dSphs . .8 1.3.2 Jeans modeling . .9 1.3.3 Schwarzschild modeling .
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												  The Milky Way the Milky Way's NeighbourhoodThe Milky Way What Is The Milky Way Galaxy? The.Milky.Way.is.the.galaxy.we.live.in..It.contains.the.Sun.and.at.least.one.hundred.billion.other.stars..Some.modern. measurements.suggest.there.may.be.up.to.500.billion.stars.in.the.galaxy..The.Milky.Way.also.contains.more.than.a.billion. solar.masses’.worth.of.free-floating.clouds.of.interstellar.gas.sprinkled.with.dust,.and.several.hundred.star.clusters.that. contain.anywhere.from.a.few.hundred.to.a.few.million.stars.each. What Kind Of Galaxy Is The Milky Way? Figuring.out.the.shape.of.the.Milky.Way.is,.for.us,.somewhat.like.a.fish.trying.to.figure.out.the.shape.of.the.ocean.. Based.on.careful.observations.and.calculations,.though,.it.appears.that.the.Milky.Way.is.a.barred.spiral.galaxy,.probably. classified.as.a.SBb.or.SBc.on.the.Hubble.tuning.fork.diagram. Where Is The Milky Way In Our Universe’! The.Milky.Way.sits.on.the.outskirts.of.the.Virgo.supercluster..(The.centre.of.the.Virgo.cluster,.the.largest.concentrated. collection.of.matter.in.the.supercluster,.is.about.50.million.light-years.away.).In.a.larger.sense,.the.Milky.Way.is.at.the. centre.of.the.observable.universe..This.is.of.course.nothing.special,.since,.on.the.largest.size.scales,.every.point.in.space. is.expanding.away.from.every.other.point;.every.object.in.the.cosmos.is.at.the.centre.of.its.own.observable.universe.. Within The Milky Way Galaxy, Where Is Earth Located’? Earth.orbits.the.Sun,.which.is.situated.in.the.Orion.Arm,.one.of.the.Milky.Way’s.66.spiral.arms..(Even.though.the.spiral.