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A&A 619, A61 (2018) Astronomy https://doi.org/10.1051/0004-6361/201833747 & c ESO 2018 Astrophysics Dramatic change in the boundary layer in the symbiotic recurrent nova T Coronae Borealis G. J. M. Luna1,2,3 , K. Mukai4,5, J. L. Sokoloski6, T. Nelson7, P. Kuin8, A. Segreto9, G. Cusumano9, M. Jaque Arancibia10,11, and N. E. Nuñez11 1 CONICET-Universidad de Buenos Aires, Instituto de Astronomía y Física del Espacio (IAFE), Av. Inte. Güiraldes 2620, C1428ZAA Buenos Aires, Argentina e-mail: [email protected] 2 Universidad de Buenos Aires, Facultad de Ciencias Exactas y Naturales, Buenos Aires, Argentina 3 Universidad Nacional Arturo Jauretche, Av. Calchaquí 6200, F. Varela, Buenos Aires, Argentina 4 CRESST and X-ray Astrophysics Laboratory, NASA Goddard Space Flight Center, Greenbelt, MD 20771, USA 5 Department of Physics, University of Maryland, Baltimore County, 1000 Hilltop Circle, Baltimore, MD 21250, USA 6 Columbia Astrophysics Lab 550 W 120th St., 1027 Pupin Hall, MC 5247 Columbia University, New York, NY 10027, USA 7 Department of Physics and Astronomy, University of Pittsburgh, Pittsburgh, PA 15260, USA 8 University College London, Mullard Space Science Laboratory, Holmbury St. Mary, Dorking RH5 6NT, UK 9 INAF – Istituto di Astrofisica Spaziale e Fisica Cosmica, Via U. La Malfa 153, 90146 Palermo, Italy 10 Departamento de Física y Astronomía, Universidad de La Serena, Av. Cisternas 1200, La Serena, Chile 11 Instituto de Ciencias Astronómicas, de la Tierra y del Espacio (ICATE-CONICET), Av. España Sur 1512, J5402DSP San Juan, Argentina Received 29 June 2018 / Accepted 23 August 2018 ABSTRACT A sudden increase in the rate at which material reaches the most internal part of an accretion disk, i.e., the boundary layer, can change its structure dramatically. -
136, June 2008
British Astronomical Association VARIABLE STAR SECTION CIRCULAR No 136, June 2008 Contents Group Photograph, AAVSO/BAAVSS meeting ........................ inside front cover From the Director ............................................................................................... 1 Eclipsing Binary News ....................................................................................... 4 Experiments in the use of a DSLR camera for V photometry ............................ 5 Joint Meeting of the AAVSO and the BAAVSS ................................................. 8 Coordinated HST and Ground Campaigns on CVs ............................... 8 Eclipsing Binaries - Observational Challenges .................................................. 9 Peer to Peer Astronomy Education .................................................................. 10 AAVSO Acronyms De-mystified in Fifteen Minutes ...................................... 11 New Results on SW Sextantis Stars and Proposed Observing Campaign ........ 12 A Week in the Life of a Remote Observer ........................................................ 13 Finding Eclipsing Binaries in NSVS Data ......................................................... 13 British Variable Star Associations 1848-1908 .................................................. 14 “Chasing Rainbows” (The European Amateur Spectroscopy Scene) .............. 15 Long Term Monitoring and the Carbon Miras ................................................. 18 Cataclysmic Variables from Large Surveys: A Silent Revolution -
Stellar Populations in a Standard ISOGAL Field in the Galactic Disc
A&A 493, 785–807 (2009) Astronomy DOI: 10.1051/0004-6361:200809668 & c ESO 2009 Astrophysics Stellar populations in a standard ISOGAL field in the Galactic disc, S. Ganesh1,2,A.Omont1,U.C.Joshi2,K.S.Baliyan2, M. Schultheis3,1,F.Schuller4,1,andG.Simon5 1 Institut d’Astrophysique de Paris, CNRS and Université Paris 6, 98bis boulevard Arago, 75014 Paris, France e-mail: [email protected] 2 Physical Research Laboratory, Navrangpura, Ahmedabad-380 009, India e-mail: [email protected] 3 Observatoire de Besançon, Besançon, France 4 Max-Planck-Institut fur Radioastronomie, Auf dem Hugel 69, 53121 Bonn, Germany 5 GEPI, UMS-CNRS 2201, Observatoire de Paris, France Received 28 February 2008 / Accepted 3 September 2008 ABSTRACT Aims. We identify the stellar populations (mostly red giants and young stars) detected in the ISOGAL survey at 7 and 15 μmtowards a field (LN45) in the direction = −45, b = 0.0. Methods. The sources detected in the survey of the Galactic plane by the Infrared Space Observatory were characterised based on colour−colour and colour−magnitude diagrams. We combine the ISOGAL catalogue with the data from surveys such as 2MASS and GLIMPSE. Interstellar extinction and distance were estimated using the red clump stars detected by 2MASS in combination with the isochrones for the AGB/RGB branch. Absolute magnitudes were thus derived and the stellar populations identified from their absolute magnitudes and their infrared excess. Results. A standard approach to analysing the ISOGAL disc observations has been established. We identify several hundred RGB/AGB stars and 22 candidate young stellar objects in the direction of this field in an area of 0.16 deg2. -
First Science with the Keck Interferometer Nuller R
The Astrophysical Journal, 677:1253Y1267, 2008 April 20 # 2008. The American Astronomical Society. All rights reserved. Printed in U.S.A. MILLIARCSECOND N-BAND OBSERVATIONS OF THE NOVA RS OPHIUCHI: FIRST SCIENCE WITH THE KECK INTERFEROMETER NULLER R. K. Barry,1,2 W. C. Danchi,1 W. A. Traub,3 J. L. Sokoloski,4 J. P. Wisniewski,1 E. Serabyn,3 M. J. Kuchner,1 R. Akeson,5 E. Appleby,6 J. Bell,6 A. Booth,3 H. Brandenburg,5 M. Colavita,3 S. Crawford,3 M. Creech-Eakman,3 W. Dahl,6 C. Felizardo,5 J. Garcia,3 J. Gathright,6 M. A. Greenhouse,1 J. Herstein,5 E. Hovland,3 M. Hrynevych,6 C. Koresko,3 R. Ligon,3 B. Mennesson,3 R. Millan-Gabet,5 D. Morrison,6 D. Palmer,3 T. Panteleeva,6 S. Ragland,6 M. Shao,3 R. Smythe,3 K. Summers,6 M. Swain,3 K. Tsubota,6 C. Tyau,6 E. Wetherell,6 P. Wizinowich,6 J. Woillez,6 and G. Vasisht3 Received 2007 August 9; accepted 2008 January 9 ABSTRACT We report observations of the nova RS Ophiuchi (RS Oph) using the Keck Interferometer Nuller (KIN), approxi- mately 3.8 days following the most recent outburst that occurred on 2006 February 12. These observations represent the first scientific results from the KIN, which operates in N band from 8 to 12.5 m in a nulling mode. The nulling technique is the sparse aperture equivalent of the conventional coronagraphic technique used in filled aperture tele- scopes. In this mode the stellar light itself is suppressed by a destructive fringe, effectively enhancing the contrast of the circumstellar material located near the star. -
A Secondary Clump of Red Giant Stars: Why and Where
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server A secondary clump of red giant stars: why and where L´eo Girardi Max-Planck-Institut f¨ur Astrophysik, Karl-Schwarzschild-Str. 1, D-85740 Garching bei M¨unchen, Germany E-mail: [email protected] submitted to Monthly Notices of the Royal Astronomical Society Abstract. Based on the results of detailed population synthesis models, Girardi et al. (1998) recently claimed that the clump of red giants in the colour–magnitude diagram (CMD) of composite stellar populations should present an extension to lower luminosities, which goes down to about 0.4 mag below the main clump. This feature is made of stars just massive enough for having ignited helium in non- degenerate conditions, and therefore corresponds to a limited interval of stellar masses and ages. In the present models, which include moderate convective over- shooting, it corresponds to 1 Gyr old populations. In this paper, we go into∼ more details about the origin and properties of this feature. We first compare the clump theoretical models with data for clusters of different ages and metallicities, basically confirming the predicted behaviours. We then refine the previous models in order to show that: (i) The faint extension is expected to be clearly separated from the main clump in the CMD of metal-rich populations, defining a ‘secondary clump’ by itself. (ii) It should be present in all galactic fields containing 1 Gyr old stars and with mean metallicities higher than about Z =0:004. -
Variable Star Classification and Light Curves Manual
Variable Star Classification and Light Curves An AAVSO course for the Carolyn Hurless Online Institute for Continuing Education in Astronomy (CHOICE) This is copyrighted material meant only for official enrollees in this online course. Do not share this document with others. Please do not quote from it without prior permission from the AAVSO. Table of Contents Course Description and Requirements for Completion Chapter One- 1. Introduction . What are variable stars? . The first known variable stars 2. Variable Star Names . Constellation names . Greek letters (Bayer letters) . GCVS naming scheme . Other naming conventions . Naming variable star types 3. The Main Types of variability Extrinsic . Eclipsing . Rotating . Microlensing Intrinsic . Pulsating . Eruptive . Cataclysmic . X-Ray 4. The Variability Tree Chapter Two- 1. Rotating Variables . The Sun . BY Dra stars . RS CVn stars . Rotating ellipsoidal variables 2. Eclipsing Variables . EA . EB . EW . EP . Roche Lobes 1 Chapter Three- 1. Pulsating Variables . Classical Cepheids . Type II Cepheids . RV Tau stars . Delta Sct stars . RR Lyr stars . Miras . Semi-regular stars 2. Eruptive Variables . Young Stellar Objects . T Tau stars . FUOrs . EXOrs . UXOrs . UV Cet stars . Gamma Cas stars . S Dor stars . R CrB stars Chapter Four- 1. Cataclysmic Variables . Dwarf Novae . Novae . Recurrent Novae . Magnetic CVs . Symbiotic Variables . Supernovae 2. Other Variables . Gamma-Ray Bursters . Active Galactic Nuclei 2 Course Description and Requirements for Completion This course is an overview of the types of variable stars most commonly observed by AAVSO observers. We discuss the physical processes behind what makes each type variable and how this is demonstrated in their light curves. Variable star names and nomenclature are placed in a historical context to aid in understanding today’s classification scheme. -
Arxiv:1712.02405V2 [Astro-Ph.SR] 11 Dec 2017
Draft version October 19, 2018 Typeset using LATEX twocolumn style in AASTeX61 PHOTOSPHERIC DIAGNOSTICS OF CORE HELIUM BURNING IN GIANT STARS Keith Hawkins,1 Yuan-Sen Ting,2, 3, 4, 5 and Hans-Walter Rix6 1Department of Astronomy, Columbia University, 550 W 120th St, New York, NY 10027, USA 2Research School of Astronomy and Astrophysics, Mount Stromlo Observatory, The Australian National University, ACT 2611, Australia 3Institute for Advanced Study, Princeton, NJ 08540, USA 4Department of Astrophysical Sciences, Princeton University, Princeton, NJ 08544, USA 5Observatories of the Carnegie Institution of Washington, Pasadena, CA 91101, USA 6Max-Planck-Institut f¨urAstronomie, K¨onigstuhl17, D-69117 Heidelberg, Germany ABSTRACT Core helium burning primary red clump (RC) stars are evolved red giant stars which are excellent standard candles. As such, these stars are routinely used to map the Milky Way or determine the distance to other galaxies among other things. However distinguishing RC stars from their less evolved precursors, namely red giant branch (RGB) stars, is still a difficult challenge and has been deemed the domain of asteroseismology. In this letter, we use a sample of 1,676 RGB and RC stars which have both single epoch infrared spectra from the APOGEE survey and asteroseismic parameters and classification to show that the spectra alone can be used to (1) predict asteroseismic parameters with precision high enough to (2) distinguish core helium burning RC from other giant stars with less than 2% contamination. This will not only allow for a clean selection of a large number of standard candles across our own and other galaxies from spectroscopic surveys, but also will remove one of the primary roadblocks for stellar evolution studies of mixing and mass loss in red giant stars. -
Exoplanet Community Report
JPL Publication 09‐3 Exoplanet Community Report Edited by: P. R. Lawson, W. A. Traub and S. C. Unwin National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California March 2009 The work described in this publication was performed at a number of organizations, including the Jet Propulsion Laboratory, California Institute of Technology, under a contract with the National Aeronautics and Space Administration (NASA). Publication was provided by the Jet Propulsion Laboratory. Compiling and publication support was provided by the Jet Propulsion Laboratory, California Institute of Technology under a contract with NASA. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does not constitute or imply its endorsement by the United States Government, or the Jet Propulsion Laboratory, California Institute of Technology. © 2009. All rights reserved. The exoplanet community’s top priority is that a line of probeclass missions for exoplanets be established, leading to a flagship mission at the earliest opportunity. iii Contents 1 EXECUTIVE SUMMARY.................................................................................................................. 1 1.1 INTRODUCTION...............................................................................................................................................1 1.2 EXOPLANET FORUM 2008: THE PROCESS OF CONSENSUS BEGINS.....................................................2 -
Stellar Evolution
Stellar Astrophysics: Stellar Evolution 1 Stellar Evolution Update date: December 14, 2010 With the understanding of the basic physical processes in stars, we now proceed to study their evolution. In particular, we will focus on discussing how such processes are related to key characteristics seen in the HRD. 1 Star Formation From the virial theorem, 2E = −Ω, we have Z M 3kT M GMr = dMr (1) µmA 0 r for the hydrostatic equilibrium of a gas sphere with a total mass M. Assuming that the density is constant, the right side of the equation is 3=5(GM 2=R). If the left side is smaller than the right side, the cloud would collapse. For the given chemical composition, ρ and T , this criterion gives the minimum mass (called Jeans mass) of the cloud to undergo a gravitational collapse: 3 1=2 5kT 3=2 M > MJ ≡ : (2) 4πρ GµmA 5 For typical temperatures and densities of large molecular clouds, MJ ∼ 10 M with −1=2 a collapse time scale of tff ≈ (Gρ) . Such mass clouds may be formed in spiral density waves and other density perturbations (e.g., caused by the expansion of a supernova remnant or superbubble). What exactly happens during the collapse depends very much on the temperature evolution of the cloud. Initially, the cooling processes (due to molecular and dust radiation) are very efficient. If the cooling time scale tcool is much shorter than tff , −1=2 the collapse is approximately isothermal. As MJ / ρ decreases, inhomogeneities with mass larger than the actual MJ will collapse by themselves with their local tff , different from the initial tff of the whole cloud. -
High-Resolution N-Band Observations of the Nova RS Ophiuchi with the Keck Interferometer Nuller
High-Resolution N-Band Observations of the Nova RS Ophiuchi with the Keck Interferometer Nuller ABSTRACT We report new observations of the nova RS Ophiuchi (RS Oph) using the Keck Interferometer Nulling Instrument, approximately 3.8 days following the most recent outburst that occurred on 2006 February 12. The Keck Interferome- ter Nuller (KIN) operates in K-band from 8 to 12.5 pm in a nulling mode, which means that the central broad-band interference fringe is a dark fringe - with an angular width of 25 mas at mid band - rather than the bright fringe used ill a con- ventional optical interferometer. In this mode the stellar light itself is suppressed by the destructive fringe, effectively enhancing the contrast of the circumstellar material located near the star. By subsequently shifting the neighboring bright fringe onto the center of the source brightness distribution and integrating, a second spatial regime dominated by light from the central portion of the source is almost simultaneously sampled. The nulling technique is the sparse aperture equivalent of the conventional corongraphic technique used in filled aperture tele- scopes. By fitting the unique KIK inner and outer spatial regime data, we have obtained an angular size of the mid-infrared continuum of 6.2, 4.0. or 5.4 mas for a disk profile, gaussian profile (fwhm), and shell profile respectively. The data show evidence of enhanced neutral atomic hydrogen emission located in the inner spatial regime relative to the outer regime. There is also evidence of a 9.7 micron silicate feature seen outside of this region. -
Stars and Their Spectra: an Introduction to the Spectral Sequence Second Edition James B
Cambridge University Press 978-0-521-89954-3 - Stars and Their Spectra: An Introduction to the Spectral Sequence Second Edition James B. Kaler Index More information Star index Stars are arranged by the Latin genitive of their constellation of residence, with other star names interspersed alphabetically. Within a constellation, Bayer Greek letters are given first, followed by Roman letters, Flamsteed numbers, variable stars arranged in traditional order (see Section 1.11), and then other names that take on genitive form. Stellar spectra are indicated by an asterisk. The best-known proper names have priority over their Greek-letter names. Spectra of the Sun and of nebulae are included as well. Abell 21 nucleus, see a Aurigae, see Capella Abell 78 nucleus, 327* ε Aurigae, 178, 186 Achernar, 9, 243, 264, 274 z Aurigae, 177, 186 Acrux, see Alpha Crucis Z Aurigae, 186, 269* Adhara, see Epsilon Canis Majoris AB Aurigae, 255 Albireo, 26 Alcor, 26, 177, 241, 243, 272* Barnard’s Star, 129–130, 131 Aldebaran, 9, 27, 80*, 163, 165 Betelgeuse, 2, 9, 16, 18, 20, 73, 74*, 79, Algol, 20, 26, 176–177, 271*, 333, 366 80*, 88, 104–105, 106*, 110*, 113, Altair, 9, 236, 241, 250 115, 118, 122, 187, 216, 264 a Andromedae, 273, 273* image of, 114 b Andromedae, 164 BDþ284211, 285* g Andromedae, 26 Bl 253* u Andromedae A, 218* a Boo¨tis, see Arcturus u Andromedae B, 109* g Boo¨tis, 243 Z Andromedae, 337 Z Boo¨tis, 185 Antares, 10, 73, 104–105, 113, 115, 118, l Boo¨tis, 254, 280, 314 122, 174* s Boo¨tis, 218* 53 Aquarii A, 195 53 Aquarii B, 195 T Camelopardalis, -
Arxiv:1803.04461V1 [Astro-Ph.SR] 12 Mar 2018 (Received; Revised March 14, 2018) Submitted to Apj
Draft version March 14, 2018 Typeset using LATEX preprint style in AASTeX61 CHEMICAL ABUNDANCES OF MAIN-SEQUENCE, TURN-OFF, SUBGIANT AND RED GIANT STARS FROM APOGEE SPECTRA I: SIGNATURES OF DIFFUSION IN THE OPEN CLUSTER M67 Diogo Souto,1 Katia Cunha,2, 1 Verne V. Smith,3 C. Allende Prieto,4, 5 D. A. Garc´ıa-Hernandez,´ 4, 5 Marc Pinsonneault,6 Parker Holzer,7 Peter Frinchaboy,8 Jon Holtzman,9 J. A. Johnson,6 Henrik Jonsson¨ ,10 Steven R. Majewski,11 Matthew Shetrone,12 Jennifer Sobeck,11 Guy Stringfellow,13 Johanna Teske,14 Olga Zamora,4, 5 Gail Zasowski,7 Ricardo Carrera,15 Keivan Stassun,16 J. G. Fernandez-Trincado,17, 18 Sandro Villanova,17 Dante Minniti,19 and Felipe Santana20 1Observat´orioNacional, Rua General Jos´eCristino, 77, 20921-400 S~aoCrist´ov~ao,Rio de Janeiro, RJ, Brazil 2Steward Observatory, University of Arizona, 933 North Cherry Avenue, Tucson, AZ 85721-0065, USA 3National Optical Astronomy Observatory, 950 North Cherry Avenue, Tucson, AZ 85719, USA 4Instituto de Astrof´ısica de Canarias, E-38205 La Laguna, Tenerife, Spain 5Departamento de Astrof´ısica, Universidad de La Laguna, E-38206 La Laguna, Tenerife, Spain 6Department of Astronomy, The Ohio State University, Columbus, OH 43210, USA 7Department of Physics and Astronomy, The University of Utah, Salt Lake City, UT 84112, USA 8Department of Physics & Astronomy, Texas Christian University, Fort Worth, TX, 76129, USA 9New Mexico State University, Las Cruces, NM 88003, USA 10Lund Observatory, Department of Astronomy and Theoretical Physics, Lund University, Box 43,