PREFACE Symposium 177 of the International Astronomical Union
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Spectroscopic Analysis of Accretion/Ejection Signatures in the Herbig Ae/Be Stars HD 261941 and V590 Mon T Moura, S
Spectroscopic analysis of accretion/ejection signatures in the Herbig Ae/Be stars HD 261941 and V590 Mon T Moura, S. Alencar, A. Sousa, E. Alecian, Y. Lebreton To cite this version: T Moura, S. Alencar, A. Sousa, E. Alecian, Y. Lebreton. Spectroscopic analysis of accretion/ejection signatures in the Herbig Ae/Be stars HD 261941 and V590 Mon. Monthly Notices of the Royal Astronomical Society, Oxford University Press (OUP): Policy P - Oxford Open Option A, 2020, 494 (3), pp.3512-3535. 10.1093/mnras/staa695. hal-02523038 HAL Id: hal-02523038 https://hal.archives-ouvertes.fr/hal-02523038 Submitted on 16 May 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. MNRAS 000,1–24 (2019) Preprint 27 February 2020 Compiled using MNRAS LATEX style file v3.0 Spectroscopic analysis of accretion/ejection signatures in the Herbig Ae/Be stars HD 261941 and V590 Mon T. Moura1?, S. H. P. Alencar1, A. P. Sousa1;2, E. Alecian2, Y. Lebreton3;4 1Universidade Federal de Minas Gerais, Departamento de Física, Av. Antônio Carlos 6627, 31270-901, Brazil 2Univ. Grenoble Alpes, IPAG, F-38000 Grenoble, France 3LESIA, Observatoire de Paris, PSL Research University, CNRS, Sorbonne Universités, UPMC Univ. -
Ira Sprague Bowen Papers, 1940-1973
http://oac.cdlib.org/findaid/ark:/13030/tf2p300278 No online items Inventory of the Ira Sprague Bowen Papers, 1940-1973 Processed by Ronald S. Brashear; machine-readable finding aid created by Gabriela A. Montoya Manuscripts Department The Huntington Library 1151 Oxford Road San Marino, California 91108 Phone: (626) 405-2203 Fax: (626) 449-5720 Email: [email protected] URL: http://www.huntington.org/huntingtonlibrary.aspx?id=554 © 1998 The Huntington Library. All rights reserved. Observatories of the Carnegie Institution of Washington Collection Inventory of the Ira Sprague 1 Bowen Papers, 1940-1973 Observatories of the Carnegie Institution of Washington Collection Inventory of the Ira Sprague Bowen Paper, 1940-1973 The Huntington Library San Marino, California Contact Information Manuscripts Department The Huntington Library 1151 Oxford Road San Marino, California 91108 Phone: (626) 405-2203 Fax: (626) 449-5720 Email: [email protected] URL: http://www.huntington.org/huntingtonlibrary.aspx?id=554 Processed by: Ronald S. Brashear Encoded by: Gabriela A. Montoya © 1998 The Huntington Library. All rights reserved. Descriptive Summary Title: Ira Sprague Bowen Papers, Date (inclusive): 1940-1973 Creator: Bowen, Ira Sprague Extent: Approximately 29,000 pieces in 88 boxes Repository: The Huntington Library San Marino, California 91108 Language: English. Provenance Placed on permanent deposit in the Huntington Library by the Observatories of the Carnegie Institution of Washington Collection. This was done in 1989 as part of a letter of agreement (dated November 5, 1987) between the Huntington and the Carnegie Observatories. The papers have yet to be officially accessioned. Cataloging of the papers was completed in 1989 prior to their transfer to the Huntington. -
Plotting Variable Stars on the H-R Diagram Activity
Pulsating 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. -
The Evolution of Helium White Dwarfs: Applications to Millisecond
Pulsar Astronomy — 2000 and Beyond ASP Conference Series, Vol. 3 × 108, 1999 M. Kramer, N. Wex, and R. Wielebinski, eds. The evolution of helium white dwarfs: Applications for millisecond pulsars T. Driebe and T. Bl¨ocker Max-Planck-Institut f¨ur Radioastronomie, Bonn, Germany D. Sch¨onberner Astrophysikalisches Institut Potsdam, Potsdam, Germany 1. White Dwarf Evolution Low-mass white dwarfs with helium cores (He-WDs) are known to result from mass loss and/or exchange events in binary systems where the donor is a low mass star evolving along the red giant branch (RGB). Therefore, He-WDs are common components in binary systems with either two white dwarfs or with a white dwarf and a millisecond pulsar (MSP). If the cooling behaviour of He- WDs is known from theoretical studies (see Driebe et al. 1998, and references therein) the ages of MSP systems can be calculated independently of the pulsar properties provided the He-WD mass is known from spectroscopy. Driebe et al. (1998, 1999) investigated the evolution of He-WDs in the mass range 0.18 < MWD/M⊙ < 0.45 using the code of Bl¨ocker (1995). The evolution of a 1 M⊙-model was calculated up to the tip of the RGB. High mass loss termi- nated the RGB evolution at appropriate positions depending on the desired final white dwarf mass. When the model started to leave the RGB, mass loss was virtually switched off and the models evolved towards the white dwarf cooling branch. The applied procedure mimicks the mass transfer in binary systems. Contrary to the more massive C/O-WDs (MWD ∼> 0.5 M⊙, carbon/oxygen core), whose progenitors have also evolved through the asymptotic giant branch phase, He-WDs can continue to burn hydrogen via the pp cycle along the cooling branch arXiv:astro-ph/9910230v1 13 Oct 1999 down to very low effective temperatures, resulting in cooling ages of the order of Gyr, i. -
College of San Mateo Observatory Stellar Spectra Catalog ______
College of San Mateo Observatory Stellar Spectra Catalog SGS Spectrograph Spectra taken from CSM observatory using SBIG Self Guiding Spectrograph (SGS) ___________________________________________________ A work in progress compiled by faculty, staff, and students. Stellar Spectroscopy Stars are divided into different spectral types, which result from varying atomic-level activity on the star, due to its surface temperature. In spectroscopy, we measure this activity via a spectrograph/CCD combination, attached to a moderately sized telescope. The resultant data are converted to graphical format for further analysis. The main spectral types are characterized by the letters O,B,A,F,G,K, & M. Stars of O type are the hottest, as well as the rarest. Stars of M type are the coolest, and by far, the most abundant. Each spectral type is also divided into ten subtypes, ranging from 0 to 9, further delineating temperature differences. Type Temperature Color O 30,000 - 60,000 K Blue B 10,000 - 30,000 K Blue-white A 7,500 - 10,000 K White F 6,000 - 7,500 K Yellow-white G 5,000 - 6,000 K Yellow K 3,500 - 5,000 K Yellow-orange M >3,500 K Red Class Spectral Lines O -Weak neutral and ionized Helium, weak Hydrogen, a relatively smooth continuum with very few absorption lines B -Weak neutral Helium, stronger Hydrogen, an otherwise relatively smooth continuum A -No Helium, very strong Hydrogen, weak CaII, the continuum is less smooth because of weak ionized metal lines F -Strong Hydrogen, strong CaII, weak NaI, G-band, the continuum is rougher because of many ionized metal lines G -Weaker Hydrogen, strong CaII, stronger NaI, many ionized and neutral metals, G-band is present K -Very weak Hydrogen, strong CaII, strong NaI and many metals G- band is present M -Strong TiO molecular bands, strongest NaI, weak CaII very weak Hydrogen absorption. -
• Classifying Stars: HR Diagram • Luminosity, Radius, and Temperature • “Vogt-Russell” Theorem • Main Sequence • Evolution on the HR Diagram
Stars • Classifying stars: HR diagram • Luminosity, radius, and temperature • “Vogt-Russell” theorem • Main sequence • Evolution on the HR diagram Classifying stars • We now have two properties of stars that we can measure: – Luminosity – Color/surface temperature • Using these two characteristics has proved extraordinarily effective in understanding the properties of stars – the Hertzsprung- Russell (HR) diagram If we plot lots of stars on the HR diagram, they fall into groups These groups indicate types of stars, or stages in the evolution of stars Luminosity classes • Class Ia,b : Supergiant • Class II: Bright giant • Class III: Giant • Class IV: Sub-giant • Class V: Dwarf The Sun is a G2 V star Luminosity versus radius and temperature A B R = R R = 2 RSun Sun T = T T = TSun Sun Which star is more luminous? Luminosity versus radius and temperature A B R = R R = 2 RSun Sun T = T T = TSun Sun • Each cm2 of each surface emits the same amount of radiation. • The larger stars emits more radiation because it has a larger surface. It emits 4 times as much radiation. Luminosity versus radius and temperature A1 B R = RSun R = RSun T = TSun T = 2TSun Which star is more luminous? The hotter star is more luminous. Luminosity varies as T4 (Stefan-Boltzmann Law) Luminosity Law 2 4 LA = RATA 2 4 LB RBTB 1 2 If star A is 2 times as hot as star B, and the same radius, then it will be 24 = 16 times as luminous. From a star's luminosity and temperature, we can calculate the radius. -
69-22,173 MARKOWITZ, Allan Henry, 1941- a STUDY of STARS
This dissertation has been microfilmed exactly u received 6 9 -2 2 ,1 7 3 MARKOWITZ, Allan Henry, 1941- A STUDY OF STARS EXHIBITING COM POSITE SPECTRA. The Ohio State University, Ph.D., 1969 A stron om y University Microfilms, Inc., Ann Arbor, Michigan A STUDY OF STARS EXHIBITING COMPOSITE SPECTRA DISSERTATION Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Allan Henry Markowitz, A.B., M.Sc. ******** The Ohio S ta te U n iv e rsity 1969 Approved by UjiIjl- A dviser Department of Astronomy ACKNOWLEDGMENTS It is a sincere pleasure to thank my adviser, Professor Arne Slettebak, who originally suggested this problem and whose advice and encouragement were indispensable throughout the course of the research. I am also greatly indebted to Professor Philip Keenan for help in classifying certain late-type spectra and to Professor Terry Roark for instructing me in the operation of the Perkins Observatory telescope, I owe a special debt of gratitude to Dr. Carlos Jaschek of the La Plata Observatory for his inspiration, advice, and encourage ment. The Lowell Observatory was generous in providing extra telescope time when the need arose. I wish to particularly thank Dr. John Hall for this and for his interest. I also gratefully acknowledge the assistance of the Perkins Observatory staff. To my wife, Joan, I owe my profound thanks for her devotion and support during the seemingly unending tenure as a student. I am deeply grateful to my mother for her eternal confidence and to my in-laws for their encouragement. -
The Hr Diagram for Late-Type Nearby Stars
379 THE H-R DIAGRAM FOR LATE-TYPE NEARBY STARS AS A FUNCTION OF HELIUM CONTENT AND METALLICITY 1 2 3 2 1 1 Y. Lebreton , M.-N. Perrin ,J.Fernandes ,R.Cayrel ,G.Cayrel de Strob el , A. Baglin 1 Observatoire de Paris, Place J. Janssen - 92195 Meudon Cedex, France 2 Observatoire de Paris, 61 Avenue de l'Observatoire - 75014 Paris, France 3 Observat orio Astron omico da Universidade de Coimbra, 3040 Coimbra, Portugal Key words: Galaxy: solar neighb ourho o d; stars: ABSTRACT abundances; stars: low-mass; stars: HR diagram; Galaxy: abundances. Recent theoretical stellar mo dels are used to discuss the helium abundance of a numberoflow-mass stars for which the p osition in the Hertzsprung-Russell di- 1. INTRODUCTION agram and the metallicity are known with high accu- racy. The knowledge of the initial helium abundance of Hipparcos has provided very high quality parallaxes stars b orn in di erent sites with di erent metallicities of a sample of a hundred disk stars, of typeFtoK,lo- is of great imp ortance for many astrophysical stud- cated in the solar neighb ourho o d. Among these stars ies. The lifetime of a star and its internal structure we have carefully selected those for which detailed very much dep end on its initial helium content and sp ectroscopic analysis has provided e ective temp er- this has imp ortant consequences not only for stellar ature and [Fe/H] ratio with a high accuracy. astrophysics but also in cosmology or in studies of the chemical evolution of galaxies. Wehave calculated evolved stellar mo dels and their Direct measurement of the helium abundance in the asso ciated iso chrones in a large range of mass, for photosphere of a low mass star cannot b e made since several values of the metallicity and of the helium there are no helium lines in the sp ectra. -
Evolution, Mass Loss and Variability of Low and Intermediate-Mass Stars What Are Low and Intermediate Mass Stars?
Evolution, Mass Loss and Variability of Low and Intermediate-Mass Stars What are low and intermediate mass stars? Defined by properties of late stellar evolutionary stages Intermediate mass stars: ~1.9 < M/Msun < ~7 Develop electron-degenerate cores after core helium burning and ascending the red giant branch for the second time i.e. on the Asymptotic Giant Branch (AGB). AGB Low mass stars: M/Msun < ~1.9 Develop electron-degenerate cores on leaving RGB the main-sequence and ascending the red giant branch for the first time i.e. on the Red Giant Branch (RGB). Maeder & Meynet 1989 Stages in the evolution of low and intermediate-mass stars These spikes are real The AGB Surface enrichment Pulsation Mass loss The RGB Surface enrichment RGB Pulsation Mass loss About 108 years spent here Most time spent on the main-sequence burning H in the core (~1010 years) Low mass stars: M < ~1.9 Msun Intermediate mass stars: Wood, P. R.,2007, ASP Conference Series, 374, 47 ~1.9 < M/Msun < ~7 Stellar evolution and surface enrichment The Red giant Branch (RGB) zHydrogen burns in a shell around an electron-degenerate He core, star evolves to higher luminosity. zFirst dredge-up occurs: The convection in the envelope moves in when the stars is near the bottom of the RGB and "dredges up" material that has been through partial hydrogen burning by the CNO cycle and pp chains. From John Lattanzio But there's more: extra-mixing What's the evidence? Various abundances and isotopic ratios vary continuously up the RGB. This is not predicted by a single first dredge-up alone. -
DADOS User Manual
Jan 2014 – English Revision v1.4 The collaborators on the DADOS spectrograph project are: • Max-Planck Institut für Extraterrestrische Physik www.mpe.mpg.de • CAOS www.eso.org/projects/caos/ • Baader Planetarium GmbH Zur Sternwarte D - 82291 Mammendorf Tel.: +49 (0) 8145 - 80 89-0 Fax: +49 (0) 8145 - 80 89-105 www.baader-planetarium.de 2 DADOS Spectrograph User’s Guide Thank you for purchasing this Baader Planetarium product. To get the most out of your DADOS Spectrograph, please read this instruction manual thoroughly before starting to work with the spectrograph. Keep this User’s Guide available for future reference and visit the Baader Planetarium website: http://www.baader-planetarium.de for up-to-date information about the product. 3 Unpacking As you unpack the spectrograph, check the list below and make sure that all items shown above are included. If anything is missing contact your original retailer. Standard accessories: • DADOS spectrograph • Allen Wrench 1.5 mm • Eyepiece 20mm • Allen Wrench 1.3 mm • Eyepiece 10mm • 1 ¼" Stop ring 1905131 • Slit Viewer Assy. (Guiding lens with M28.8-thread) • T2 Quick Changer #2456313 (mounted at the Dados) • T2 Quick Change Ring #2456320 mounted at the eyepiece barrel with Focusing eyepiece holder (#2458125) • Gloves for changing the grating • Manual 4 Part description 1. 2” Nosepiece 2. Slit illuminator 3. 1 ¼” Slit viewer port 4. Slit-viewer port locking screws 5. Micrometer 6. Rotation stage counter spring (pre-adjusted, do not touch) 7. Focuser 8. Focuser locking screw 9. Grating angle locking screw For a full list of accessories see Appendix D 5 Table of Contents 1. -
Binary Star Modeling: a Computational Approach
TCNJ JOURNAL OF STUDENT SCHOLARSHIP VOLUME XIV APRIL 2012 BINARY STAR MODELING: A COMPUTATIONAL APPROACH Author: Daniel Silano Faculty Sponsor: R. J. Pfeiffer, Department of Physics ABSTRACT This paper illustrates the equations and computational logic involved in writing BinaryFactory, a program I developed in Spring 2011 in collaboration with Dr. R. J. Pfeiffer, professor of physics at The College of New Jersey. This paper outlines computational methods required to design a computer model which can show an animation and generate an accurate light curve of an eclipsing binary star system. The final result is a light curve fit to any star system using BinaryFactory. An example is given for the eclipsing binary star system TU Muscae. Good agreement with observational data was obtained using parameters obtained from literature published by others. INTRODUCTION This project started as a proposal for a simple animation of two stars orbiting one another in C++. I found that although there was software that generated simple animations of binary star orbits and generated light curves, the commercial software was prohibitively expensive or not very user friendly. As I progressed from solving the orbits to generating the Roche surface to generating a light curve, I learned much about computational physics. There were many trials along the way; this paper aims to explain to the reader how a computational model of binary stars is made, as well as how to avoid pitfalls I encountered while writing BinaryFactory. Binary Factory was written in C++ using the free C++ libraries, OpenGL, GLUT, and GLUI. A basis for writing a model similar to BinaryFactory in any language will be presented, with a light curve fit for the eclipsing binary star system TU Muscae in the final secion. -
The Deaths of Stars
The Deaths of Stars 1 Guiding Questions 1. What kinds of nuclear reactions occur within a star like the Sun as it ages? 2. Where did the carbon atoms in our bodies come from? 3. What is a planetary nebula, and what does it have to do with planets? 4. What is a white dwarf star? 5. Why do high-mass stars go through more evolutionary stages than low-mass stars? 6. What happens within a high-mass star to turn it into a supernova? 7. Why was SN 1987A an unusual supernova? 8. What was learned by detecting neutrinos from SN 1987A? 9. How can a white dwarf star give rise to a type of supernova? 10.What remains after a supernova explosion? 2 Pathways of Stellar Evolution GOOD TO KNOW 3 Low-mass stars go through two distinct red-giant stages • A low-mass star becomes – a red giant when shell hydrogen fusion begins – a horizontal-branch star when core helium fusion begins – an asymptotic giant branch (AGB) star when the helium in the core is exhausted and shell helium fusion begins 4 5 6 7 Bringing the products of nuclear fusion to a giant star’s surface • As a low-mass star ages, convection occurs over a larger portion of its volume • This takes heavy elements formed in the star’s interior and distributes them throughout the star 8 9 Low-mass stars die by gently ejecting their outer layers, creating planetary nebulae • Helium shell flashes in an old, low-mass star produce thermal pulses during which more than half the star’s mass may be ejected into space • This exposes the hot carbon-oxygen core of the star • Ultraviolet radiation from the exposed