The Star-Forming Complex LMC-N79 As a Future Rival to 30 Doradus
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The Parkes H I Survey of the Magellanic System
A&A 432, 45–67 (2005) Astronomy DOI: 10.1051/0004-6361:20040321 & c ESO 2005 Astrophysics The Parkes H I Survey of the Magellanic System C. Brüns1,J.Kerp1, L. Staveley-Smith2, U. Mebold1,M.E.Putman3,R.F.Haynes2, P. M. W. Kalberla1,E.Muller4, and M. D. Filipovic2,5 1 Radioastronomisches Institut, Universität Bonn, Auf dem Hügel 71, 53121 Bonn, Germany e-mail: [email protected] 2 Australia Telescope National Facility, CSIRO, PO Box 76, Epping NSW 1710, Australia 3 Department of Astronomy, University of Michigan, Ann Arbor, MI 48109, USA 4 Arecibo Observatory, HC3 Box 53995, Arecibo, PR 00612, USA 5 University of Western Sydney, Locked Bag 1797, Penrith South, DC, NSW 1797, Australia Received 24 February 2004 / Accepted 27 October 2004 Abstract. We present the first fully and uniformly sampled, spatially complete H survey of the entire Magellanic System with high velocity resolution (∆v = 1.0kms−1), performed with the Parkes Telescope. Approximately 24 percent of the southern skywascoveredbythissurveyona≈5 grid with an angular resolution of HPBW = 14.1. A fully automated data-reduction scheme was developed for this survey to handle the large number of H spectra (1.5 × 106). The individual Hanning smoothed and polarization averaged spectra have an rms brightness temperature noise of σ = 0.12 K. The final data-cubes have an rms noise of σrms ≈ 0.05 K and an effective angular resolution of ≈16 . In this paper we describe the survey parameters, the data- reduction and the general distribution of the H gas. The Large Magellanic Cloud (LMC) and the Small Magellanic Cloud (SMC) are associated with huge gaseous features – the = Magellanic Bridge, the Interface Region, the Magellanic Stream, and the Leading Arm – with a total H mass of M(H ) 8 2 4.87 × 10 M d/55 kpc ,ifallH gas is at the same distance of 55 kpc. -
VMC – the VISTA Survey of the Magellanic System Metallicity Of
Dr Maria‐Rosa Cioni VMC – the VISTA survey of the Magellanic System (Gal-Exgal survey) Metallicity of stellar populaons Moon of stellar populaons ESO spectroscopic survey workshop ESO-Garching, Germany, 9-10 March 2009 The VISTA survey of the Magellanic System ESO Public Survey 2009-2014 The most sensive near‐IR survey across the LMC, SMC, The team Bridge and part of the Stream M. Cioni, K. Bekki, G. Clemenni, W. de Blok, J. Emerson, C. Evans, R. de Grijs, B. Gibson, L. Girardi, M. Groenewegen, 4m Telescope V. Ivanov, M. Marconi, C. Mastropietro, B. Moore, R. Napiwotzki, T. Naylor, J. Oliveira, V. Ripepi, J. van Loon, M. Wilkinson, P. Wood 1.5 deg2 FOV United Kingdom, Italy, Belgium, Chile, France, Switzerland, South Africa, Australia http://star.herts.ac.uk/~mcioni/vmc/ 0. Observe the Magellanic System 2 ≈180 deg 3 filters ‐ YJKs 15 epochs (12 in KS and 3 in YJ; once simultaneous colours) S/N=10 at: Y=21.9, J=21.4, Ks=20.3 (Ks≈19 single epoch) Seeing 0.8 arcsec – average Spaal resoluon 0.34 pix/arcsec (0.51 arcsec instrument PSF) Service mode observing 1840 hours / 240 nights http://star.herts.ac.uk/~mcioni/vmc/ I. Derive the spaally resolved SFH Synthec diagram of a typical LMC stellar field as expected from VMC data. This field covers 1 VISTA detector! Accuracy: metallicity S/N=10 0.1 dex and age 20% in 0.1 deg2 Kerber et al 2009 http://star.herts.ac.uk/~mcioni/vmc/ II. Trace the 3D structure as a funcon of me The LMC is a few kpc thick and the SMC up to 20 kpc RR Lyrae stars are excellent distance indicators in the near‐IR First applicaon to the LMC bar to derive the LMC distance (Szewczyk et al 2008) – 0.2 kpc accuracy The structure of the Magellanic System will be measured using Cepheid variables, the red clump luminosity, the p of the red giant brach, etc. -
The AAVSO DSLR Observing Manual
The AAVSO DSLR Observing Manual AAVSO 49 Bay State Road Cambridge, MA 02138 email: [email protected] Version 1.2 Copyright 2014 AAVSO Foreword This manual is a basic introduction and guide to using a DSLR camera to make variable star observations. The target audience is first-time beginner to intermediate level DSLR observers, although many advanced observers may find the content contained herein useful. The AAVSO DSLR Observing Manual was inspired by the great interest in DSLR photometry witnessed during the AAVSO’s Citizen Sky program. Consumer-grade imaging devices are rapidly evolving, so we have elected to write this manual to be as general as possible and move the software and camera-specific topics to the AAVSO DSLR forums. If you find an area where this document could use improvement, please let us know. Please send any feedback or suggestions to [email protected]. Most of the content for these chapters was written during the third Citizen Sky workshop during March 22-24, 2013 at the AAVSO. The persons responsible for creation of most of the content in the chapters are: Chapter 1 (Introduction): Colin Littlefield, Paul Norris, Richard (Doc) Kinne, Matthew Templeton Chapter 2 (Equipment overview): Roger Pieri, Rebecca Jackson, Michael Brewster, Matthew Templeton Chapter 3 (Software overview): Mark Blackford, Heinz-Bernd Eggenstein, Martin Connors, Ian Doktor Chapters 4 & 5 (Image acquisition and processing): Robert Buchheim, Donald Collins, Tim Hager, Bob Manske, Matthew Templeton Chapter 6 (Transformation): Brian Kloppenborg, Arne Henden Chapter 7 (Observing program): Des Loughney, Mike Simonsen, Todd Brown Various figures: Paul Valleli Clear skies, and Good Observing! Arne Henden, Director Rebecca Turner, Operations Director Brian Kloppenborg, Editor Matthew Templeton, Science Director Elizabeth Waagen, Senior Technical Assistant American Association of Variable Star Observers Cambridge, Massachusetts June 2014 i Index 1. -
Hubble Space Telescope Observer’S Guide Winter 2021
HUBBLE SPACE TELESCOPE OBSERVER’S GUIDE WINTER 2021 In 2021, the Hubble Space Telescope will celebrate 31 years in operation as a powerful observatory probing the astrophysics of the cosmos from Solar system studies to the high-redshift universe. The high-resolution imaging capability of HST spanning the IR, optical, and UV, coupled with spectroscopic capability will remain invaluable through the middle of the upcoming decade. HST coupled with JWST will enable new innovative science and be will be key for multi-messenger investigations. Key Science Threads • Properties of the huge variety of exo-planetary systems: compositions and inventories, compositions and characteristics of their planets • Probing the stellar and galactic evolution across the universe: pushing closer to the beginning of galaxy formation and preparing for coordinated JWST observations • Exploring clues as to the nature of dark energy ACS SBC absolute re-calibration (Cycle 27) reveals 30% greater • Probing the effect of dark matter on the evolution sensitivity than previously understood. More information at of galaxies http://www.stsci.edu/contents/news/acs-stans/acs-stan- • Quantifying the types and astrophysics of black holes october-2019 of over 7 orders of magnitude in size WFC3 offers high resolution imaging in many bands ranging from • Tracing the distribution of chemicals of life in 2000 to 17000 Angstroms, as well as spectroscopic capability in the universe the near ultraviolet and infrared. Many different modes are available for high precision photometry, astrometry, spectroscopy, mapping • Investigating phenomena and possible sites for and more. robotic and human exploration within our Solar System COS COS2025 initiative retains full science capability of COS/FUV out to 2025 (http://www.stsci.edu/hst/cos/cos2025). -
The Central Density of R136 in 30 Doradus
A&A 552, A94 (2013) Astronomy DOI: 10.1051/0004-6361/201220396 & c ESO 2013 Astrophysics The central density of R136 in 30 Doradus F. J. Selman and J. Melnick European Southern Observatory, Alonso de Cordova 3107 Vitacura Casilla 7630355, Santiago, Chile e-mail: [email protected] Received 18 September 2012 / Accepted 13 February 2013 ABSTRACT The central density, ρ0, of a stellar cluster is an important physical parameter for determining its evolutionary and dynamical state. How much mass segregation there is or whether the cluster has undergone core collapse both depend on ρ0. We reanalyze the results of a previous paper that gives the mass density profile of R136 and combine them with both a conservative upper limit for the core parameter and a more uncertain recent measurement. We thus place a lower limit on ρ0 under reasonable and defensible assumptions 4 3 about the IMF, finding ρ0 ≥ 1.5 × 10 M/pc for the conservative assumption a < 0.4 pc for the cluster core parameter. If we use the 7 3 lower, but more uncertain value a = 0.025 pc, the central density estimate becomes greater than 10 M/pc . A mechanism based on the destruction of a large number of circumstellar disks is posited to explain the hitherto unexplained increase in reddening presented in that same work. Key words. circumstellar matter – galaxies: clusters: individual: R 136 – stars: luminosity function, mass function – Magellanic Clouds – dust, extinction 1. Introduction therein). The cluster R136 has been claimed to have the char- acteristics of a PCC cluster: a cuspy density profile (Mackey Owing to its nearness and extreme nature, Radcliffe 136 (Feast & Gilmore 2003), and a large number of runaway stars (see et al. -
Chapter 8.Pdf
CHAeTER 8 INFLUENCE OF PULSARS ON SUPERNOVAE In recent years there has been a great deal of effort to understand in detail the observed light curves of type I1 supernovae. In the standard approach, the observed light curve is to be understood in terms of an initial deposition of thermal energy by the blast wave; and a more gradual input of thermal energy due to radioactive decay of iron-peak elements is invoked to explain the behaviour at later times. The consensus is that the light curves produced by these models are in satisfactory agreement with those observed. In this chapter we discuss the characteristics of the expected light curve, if in addition to the abovementioned sources of energy, there is a continued energy input from an active central pulsar. We argue that in those rare cases when the energy loss rate of the pulsar is comparable to the luminosity of the supernova near light maximum, the light curve will be characterized by an extended plateau phase. The essential reason for this is that the pulsar luminosity is expected to decline over timescales which are much longer than the timescale of, say, radioactive decay. The light curve of the recent supernova in the Large Magellanic Cloud is suggestive of continued energy input from an active pulsar. A detection of strong W,X -ray and 1-ray plerion after the ejecta becomes optically thin will be a clear evidence of the pulsar having powered the light curve. CONTENTS CHAPTER 8 INFLUENCE OF PULSARS ON SUPERNOVAE 8.1 INTRODUCTION ................... 8-1 8.2 EARLIER WORK .................. -
Annual Report 2016–2017 AAVSO
AAVSO The American Association of Variable Star Observers Annual Report 2016–2017 AAVSO Annual Report 2012 –2013 The American Association of Variable Star Observers AAVSO Annual Report 2016–2017 The American Association of Variable Star Observers 49 Bay State Road Cambridge, MA 02138-1203 USA Telephone: 617-354-0484 Fax: 617-354-0665 email: [email protected] website: https://www.aavso.org Annual Report Website: https://www.aavso.org/annual-report On the cover... At the 2017 AAVSO Annual Meeting.(clockwise from upper left) Knicole Colon, Koji Mukai, Dennis Conti, Kristine Larsen, Joey Rodriguez; Rachid El Hamri, Andy Block, Jane Glanzer, Erin Aadland, Jamin Welch, Stella Kafka; and (clockwise from upper left) Joey Rodriguez, Knicole Colon, Koji Mukai, Frans-Josef “Josch” Hambsch, Chandler Barnes. Picture credits In additon to images from the AAVSO and its archives, the editors gratefully acknowledge the following for their image contributions: Glenn Chaple, Shawn Dvorak, Mary Glennon, Bill Goff, Barbara Harris, Mario Motta, NASA, Gary Poyner, Msgr. Ronald Royer, the Mary Lea Shane Archives of the Lick Observatory, Chris Stephan, and Wheatley, et al. 2003, MNRAS, 345, 49. Table of Contents 1. About the AAVSO Vision and Mission Statement 1 About the AAVSO 1 What We Do 2 What Are Variable Stars? 3 Why Observe Variable Stars? 3 The AAVSO International Database 4 Observing Variable Stars 6 Services to Astronomy 7 Education and Outreach 9 2. The Year in Review Introduction 11 The 106th AAVSO Spring Membership Meeting, Ontario, California 11 The -
Formation of the Active Star Forming Region LHA 120-N 44 Triggered By
Draft version December 24, 2018 Typeset using LATEX twocolumn style in AASTeX61 FORMATION OF THE ACTIVE STAR FORMING REGION LHA 120-N 44 TRIGGERED BY TIDALLY-DRIVEN COLLIDING HI FLOWS Kisetsu Tsuge,1 Hidetoshi Sano,1,2 Kengo Tachihara,1 Cameron Yozin,3 Kenji Bekki,3 Tsuyoshi Inoue,1 Norikazu Mizuno,4 Akiko Kawamura,4 Toshikazu Onishi,5 and Yasuo Fukui1,2 1Department of Physics, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8601, Japan; [email protected] 2Institute for Advanced Research, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8601, Japan 3ICRAR, M468, The University of Western Australia, 35 Stirling Highway, Crawley Western Australia 6009, Australia 4National Astronomical Observatory of Japan, Mitaka, Tokyo 181-8588, Japan 5Department of Physical Science, Graduate School of Science, Osaka Prefecture University, 1-1 Gakuen-cho, Naka-ku, Sakai, Osaka 599-8531, Japan (Accepted November 30, 2018) ABSTRACT N44 is the second active site of high mass star formation next to R136 in the Large Magellanic Cloud (LMC). We carried out a detailed analysis of Hi at 60 arcsec resolution by using the ATCA & Parkes data. We presented decomposition of the Hi emission into two velocity components (the L- and D-components) with the velocity separation of ∼60 km s−1. In addition, we newly defined the I-component whose velocity is intermediate between the L- and D-components. The D-component was used to derive the rotation curve of the LMC disk, which is consistent with the stellar rotation curve (Alves & Nelson 2000). Toward the active cluster forming region of LHA 120-N 44, the three velocity components of Hi gas show signatures of dynamical interaction including bridges and complementary spatial distributions. -
UC Irvine UC Irvine Previously Published Works
UC Irvine UC Irvine Previously Published Works Title Astrophysics in 2006 Permalink https://escholarship.org/uc/item/5760h9v8 Journal Space Science Reviews, 132(1) ISSN 0038-6308 Authors Trimble, V Aschwanden, MJ Hansen, CJ Publication Date 2007-09-01 DOI 10.1007/s11214-007-9224-0 License https://creativecommons.org/licenses/by/4.0/ 4.0 Peer reviewed eScholarship.org Powered by the California Digital Library University of California Space Sci Rev (2007) 132: 1–182 DOI 10.1007/s11214-007-9224-0 Astrophysics in 2006 Virginia Trimble · Markus J. Aschwanden · Carl J. Hansen Received: 11 May 2007 / Accepted: 24 May 2007 / Published online: 23 October 2007 © Springer Science+Business Media B.V. 2007 Abstract The fastest pulsar and the slowest nova; the oldest galaxies and the youngest stars; the weirdest life forms and the commonest dwarfs; the highest energy particles and the lowest energy photons. These were some of the extremes of Astrophysics 2006. We attempt also to bring you updates on things of which there is currently only one (habitable planets, the Sun, and the Universe) and others of which there are always many, like meteors and molecules, black holes and binaries. Keywords Cosmology: general · Galaxies: general · ISM: general · Stars: general · Sun: general · Planets and satellites: general · Astrobiology · Star clusters · Binary stars · Clusters of galaxies · Gamma-ray bursts · Milky Way · Earth · Active galaxies · Supernovae 1 Introduction Astrophysics in 2006 modifies a long tradition by moving to a new journal, which you hold in your (real or virtual) hands. The fifteen previous articles in the series are referenced oc- casionally as Ap91 to Ap05 below and appeared in volumes 104–118 of Publications of V. -
Fundamental Parameters of Wolf-Rayet Stars VI
Astron. Astrophys. 320, 500–524 (1997) ASTRONOMY AND ASTROPHYSICS Fundamental parameters of Wolf-Rayet stars VI. Large Magellanic Cloud WNL stars? P.A.Crowther and L.J. Smith Department of Physics and Astronomy, University College London, Gower Street, London, WC1E 6BT, UK Received 5 February 1996 / Accepted 26 June 1996 Abstract. We present a detailed, quantitative study of late WN Key words: stars: Wolf-Rayet;mass-loss; evolution; fundamen- (WNL) stars in the LMC, based on new optical spectroscopy tal parameters – galaxies: Magellanic Clouds (AAT, MSO) and the Hillier (1990) atmospheric model. In a pre- vious paper (Crowther et al. 1995a), we showed that 4 out of the 10 known LMC Ofpe/WN9 stars should be re-classified WN9– 10. We now present observations of the remaining stars (except the LBV R127), and show that they are also WNL (WN9–11) 1. Introduction stars, with the exception of R99. Our total sample consists of 17 stars, and represents all but one of the single LMC WN6– Quantitative studies of hot luminous stars in galaxies are im- 11 population and allows a direct comparison with the stellar portant for a number of reasons. First, and probably foremost, parameters and chemical abundances of Galactic WNL stars is the information they provide on the effect of the environment (Crowther et al. 1995b; Hamann et al. 1995a). Previously un- on such fundamental properties as the mass-loss rate and stellar published ultraviolet (HST-FOS, IUE-HIRES) spectroscopy are evolution. In the standard picture (e.g. Maeder & Meynet 1987) presented for a subset of our programme stars. -
The Distance to the Large Magellanic Cloud
Proceedings Astronomy from 4 perspectives 1. Cosmology The distance to the large magellanic cloud Stefan V¨olker (Jena) In the era of modern cosmology it is necessary to determine the Hubble constant as precise as possible. Therefore it is important to know the distance to the Large Mag- ellanic Cloud (LMC), because this distance forms the fundament of the cosmological distance ladder. The determination of the LMC's distance is an suitable project for highschool students and will be presented in what follows. Calculating the distance to the LMC using the supernova SN 1987 A [1, 2] By combining the angular size α of an object with its absolute size R, one can calculate the distance d (at least for our cosmological neighborhood) using the equation R R d = ≈ (1) tan α α and the approximation d R. In the case of the SN 1987 A students can measure the angular size of the circumstellar ring on the Hubble Space Telescope (HST) image (Figure 1). The absolute size of the ring can be derived from the delay time due to light-travel effects seen in the emission light curve (also Figure 1). Once the supernova exploded, the UV-flash started 1,00 0,75 0,50 intensity (normalized) 0,25 0 0 500 1000 time t/d ESA/Hubble tP1' tP2' Figure 1: left: HST picture of the SN 1987 A; right: emission light curve of the circumstellar [2, 3] propagating and reached the whole ring at the same time, which started emitting immediately. The additional distance x is linked to the delay time by the equation x = c · ∆t = c · (t 0 − t 0 ). -
In IAU Symp. 193, Wolf-Rayet Phenomena in Stars and Starburst
Synthesis Models for Starburst Populations with Wolf-Rayet Stars Claus Leitherer Space Telescope Science Institute1, 3700 San Martin Drive, Baltimore, MD 21218 Abstract. The prospects of utilizing Wolf-Rayet populations in star- burst galaxies to infer the stellar content are reviewed. I discuss which Wolf-Rayet star features can be detected in an integrated stellar pop- ulation. Specific examples are given where the presence of Wolf-Rayet stars can help understand galaxy properties independent of the O-star population. I demonstrate how populations with small age spread, such as super star clusters, permit observational tests to distinguish between single-star and binary models to produce Wolf-Rayet stars. Different synthesis models for Wolf-Rayet populations are compared. Predictions for Wolf-Rayet properties vary dramatically between individual models. The current state of the models is such that a comparison with starburst populations is more useful for improving Wolf-Rayet atmosphere and evo- lution models than for deriving the star-formation history and the initial mass function. 1. Wolf-Rayet Signatures in Young Populations The central 30 Doradus region has the highest concentration of Wolf-Rayet (WR) stars in the LMC. Parker et al. (1995) classify 15 stars within 2000 (or 5 pc) of R136 as WR stars, including objects which may appear WR-like due to very dense winds (de Koter et al. 1997). This suggests that about 1 out of 10 ionizing stars around R136 is of WR type. The WR stars can be seen in an ultraviolet (UV) drift-scan spectrum of the integrated 30 Dor population obtained by Vacca et al.