Testing Stellar Structure and Evolution with Gaia *
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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. -
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. -
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. -
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. -
Hertzsprung-Russell Diagram and Mass Distribution of Barium Stars ? A
Astronomy & Astrophysics manuscript no. HRD_Ba c ESO 2019 May 14, 2019 Hertzsprung-Russell diagram and mass distribution of barium stars ? A. Escorza1; 2, H.M.J. Boffin3, A.Jorissen2, S. Van Eck2, L. Siess2, H. Van Winckel1, D. Karinkuzhi2, S. Shetye2; 1, and D. Pourbaix2 1 Institute of Astronomy, KU Leuven, Celestijnenlaan 200D, 3001 Leuven, Belgium 2 Institut d’Astronomie et d’Astrophysique, Université Libre de Bruxelles, ULB, Campus Plaine C.P. 226, Boulevard du Triomphe, B-1050 Bruxelles, Belgium 3 ESO, Karl Schwarzschild Straße 2, D-85748 Garching bei München, Germany Received; Accepted ABSTRACT With the availability of parallaxes provided by the Tycho-Gaia Astrometric Solution, it is possible to construct the Hertzsprung-Russell diagram (HRD) of barium and related stars with unprecedented accuracy. A direct result from the derived HRD is that subgiant CH stars occupy the same region as barium dwarfs, contrary to what their designations imply. By comparing the position of barium stars in the HRD with STAREVOL evolutionary tracks, it is possible to evaluate their masses, provided the metallicity is known. We used an average metallicity [Fe/H] = −0.25 and derived the mass distribution of barium giants. The distribution peaks around 2.5 M with a tail at higher masses up to 4.5 M . This peak is also seen in the mass distribution of a sample of normal K and M giants used for comparison and is associated with stars located in the red clump. When we compare these mass distributions, we see a deficit of low-mass (1 – 2 M ) barium giants. -
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, -
Abundance–Age Relations with Red Clump Stars in Open Clusters?,?? L
A&A 652, A25 (2021) Astronomy https://doi.org/10.1051/0004-6361/202039951 & c L. Casamiquela et al. 2021 Astrophysics Abundance–age relations with red clump stars in open clusters?,?? L. Casamiquela1, C. Soubiran1 , P. Jofré2 , C. Chiappini3, N. Lagarde4 , Y. Tarricq1 , R. Carrera5 , C. Jordi6 , L. Balaguer-Núñez6 , J. Carbajo-Hijarrubia6, and S. Blanco-Cuaresma7 1 Laboratoire d’Astrophysique de Bordeaux, Univ. Bordeaux, CNRS, B18N, allée Geoffroy Saint-Hilaire, 33615 Pessac, France e-mail: [email protected] 2 Núcleo de Astronomía, Facultad de Ingeniería y Ciencias, Universidad Diego Portales, Av. Ejército 441, Santiago, Chile 3 Leibniz-Institut für Astrophysik Potsdam (AIP), An der Sternwarte 16, 14482 Potsdam, Germany 4 Institut UTINAM, CNRS UMR6213, Univ. Bourgogne Franche-Comté, OSU-THETA Franche-Comté-Bourgogne, Observatoire de Besançon, BP 1615, 25010 Besançon Cedex, France 5 INAF-Osservatorio Astronomico di Padova, vicolo dell’Osservatorio 5, 35122 Padova, Italy 6 Dept. FQA, Institut de Ciéncies del Cosmos (ICCUB), Universitat de Barcelona (IEEC-UB), Martí Franqués 1, 08028 Barcelona, Spain 7 Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138, USA Received 19 November 2020 / Accepted 14 May 2021 ABSTRACT Context. Precise chemical abundances coupled with reliable ages are key ingredients to understanding the chemical history of our Galaxy. Open clusters (OCs) are useful for this purpose because they provide ages with good precision. Aims. The aim of this work is to investigate the relation between different chemical abundance ratios and age traced by red clump (RC) stars in OCs. Methods. We analyzed a large sample of 209 reliable members in 47 OCs with available high-resolution spectroscopy. -
Module 14 H. R. Diagram TABLE of CONTENTS 1. Learning Outcomes
Module 14 H. R. Diagram TABLE OF CONTENTS 1. Learning Outcomes 2. Introduction 3. H. R. Diagram 3.1. Coordinates of H. R. Diagram 3.2. Stellar Families 3.3. Hertzsprung Gap 3.4. H. R. Diagram and Stellar Radii 4. Summary 1. Learning Outcomes After studying this module, you should be able to recognize an H. R. Diagram explain the coordinates of an H. R. Diagram appreciate the shape of an H. R. Diagram understand that in this diagram stars appear in distinct families recount the characteristics of these families recognize that there is a real gap in the horizontal branch of the diagram, called the Hertzsprung gap explain that during their evolution stars pass very rapidly through this region and therefore there is a real paucity of stars here derive the shape of the 퐥퐨퐠 푻 − 퐥퐨퐠 푳 plot at a given stellar radius explain that the stellar radius (and mass) increases upwards in the H. R. Diagram 2. Introduction In the last few modules we have discussed the stellar spectra and spectral classification based on stellar spectra. The Harvard system of spectral classification categorized stellar spectra in 7 major classes, from simple spectra containing only a few lines to spectra containing a huge number of lines and molecular bands. The major classes were named O, B, A, F, G, K and M. Each major class was further subdivided into 10 subclasses, running from 0 to 9. Considering the bewildering variety of stellar spectra, classes Q, P and Wolf-Rayet had to be introduced at the top of the classification and classes R and N were introduced at the bottom of the classification scheme. -
A Spectroscopic Study of Detached Binary Systems Using Precise Radial
A spectroscopic study of detached binary systems using precise radial velocities ———————————————————— A thesis submitted in partial fulfilment of the requirements for the Degree of Doctor of Philosophy in Astronomy in the University of Canterbury by David J. Ramm —————————– University of Canterbury 2004 Abstract Spectroscopic orbital elements and/or related parameters have been determined for eight bi- nary systems, using radial-velocity measurements that have a typical precision of about 15 m s−1. The orbital periods of these systems range from about 10 days to 26 years, with a median of about 6 years. Orbital solutions were determined for the seven systems with shorter periods. The measurement of the mass ratio of the longest-period system, HD 217166, demonstrates that this important astrophysical quantity can be estimated in a model-free manner with less than 10% of the orbital cycle observed spectroscopically. Single-lined orbital solutions have been derived for five of the binaries. Two of these systems are astrometric binaries: β Ret and ν Oct. The other SB1 systems were 94 Aqr A, θ Ant, and the 10-day system, HD 159656. The preliminary spectroscopic solution for θ Ant (P 18 years), is ∼ the first one derived for this system. The improvement to the precision achieved for the elements of the other four systems was typically between 1–2 orders of magnitude. The very high pre- cision with which the spectroscopic solution for HD 159656 has been measured should allow an investigation into possible apsidal motion in the near future. In addition to the variable radial velocity owing to its orbital motion, the K-giant, ν Oct, has been found to have an additional long-term irregular periodicity, attributed, for the time being, to the rotation of a large surface feature. -
The Hertzsprung-Russell Diagram
PHY111 1 The HR Diagram THE HERTZSPRUNG -RUSSELL DIAGRAM THE AXES The Hertzsprung-Russell (HR) diagram is a plot of luminosity (total power output) against surface temperature , both on log scales. Since neither luminosity nor surface temperature is a directly observed quantity, real plots tend to use observable quantities that are related to luminosity and temperature. The table below gives common axis scales you may see in the lectures or in textbooks. Note that the x-axis runs from hot to cold, not from cold to hot! Axis Theoretical Observational x Teff (on log scale) Spectral class OBAFGKM or Colour index B – V, V – I or log 10 Teff y L/L⊙ (on log scale) Absolute visual magnitude MV (or other wavelengths) 1 or log 10 (L/L⊙) Apparent visual magnitude V (or other wavelengths) The symbol ⊙ means the Sun—i.e., the luminosity is measured in terms of the Sun’s luminosity, rather than in watts. Teff is effective temperature (the temperature of a blackbody of the same surface area and total power output). BRANCHES OF THE HR DIAGRAM This is a real HR diagram, of the globular cluster NGC1261, constructed using data from the HST. The horizontal line is a fit to the diagram assuming [Fe/H] = −1.35 branch (the heavy element content of the cluster is 4.5% of the Sun’s heavy element content), a distance red giant modulus of 16.15 (the absolute magnitude is found branch by subtracting 16.15 from the apparent magnitude) and an age of 12.0 Gyr. subgiant Reference: NEQ Paust et al, AJ 139 (2010) 476. -
Structure and Evolution of FK Comae Corona
A&A 383, 919–932 (2002) Astronomy DOI: 10.1051/0004-6361:20011810 & c ESO 2002 Astrophysics Structure and evolution of FK Comae corona P. Gondoin, C. Erd, and D. Lumb Space Science Department, European Space Agency – Postbus 299, 2200 AG Noordwijk, The Netherlands Received 16 October 2001 / Accepted 17 December 2001 Abstract. FK Comae (HD 117555) is a rapidly rotating single G giant whose distinctive characteristics include a quasisinusoidal optical light curve and high X-ray luminosity. FK Comae was observed twice at two weeks interval in January 2001 by the XMM-Newton space observatory. Analysis results suggest a scenario where the corona of FK Comae is dominated by large magnetic structures similar in size to interconnecting loops between solar active regions but significantly hotter. The interaction of these structures themselves could explain the permanent flaring activity on large scales that is responsible for heating FK Comae plasma to high temperatures. During our observations, these flares were not randomly distributed on the star surface but were partly grouped within a large compact region of about 30 degree extent in longitude reminiscent of a large photospheric spot. We argue that the α − Ω dynamo driven activity on FK Comae will disappear in the future with the effect of suppressing large scale magnetic structures in its corona. Key words. stars: individual: FK Comae – stars: activity – stars: coronae – stars: evolution – stars: late-type – X-ray: stars 1. Introduction ments and their temporal behaviour during the observa- tions. Sections 5 and 6 describe the spectral analysis of the FK Comae (HD 117555) is the prototype of a small group EPIC and RGS datasets. -
PDF Hosted at the Radboud Repository of the Radboud University Nijmegen
PDF hosted at the Radboud Repository of the Radboud University Nijmegen The following full text is a publisher's version. For additional information about this publication click this link. http://hdl.handle.net/2066/92441 Please be advised that this information was generated on 2021-09-26 and may be subject to change. The Astrophysical Journal Letters, 729:L21 (5pp), 2011 March 10 doi:10.1088/2041-8205/729/2/L21 C 2011. The American Astronomical Society. All rights reserved. Printed in the U.S.A. THE X-RAY QUIESCENCE OF SWIFT J195509.6+261406 (GRB 070610): AN OPTICAL BURSTING X-RAY BINARY? N. Rea1, P. G. Jonker2,3,4, G. Nelemans4,J.A.Pons5,M.M.Kasliwal6, S. R. Kulkarni6, and R. Wijnands7 1 Institut de Ciencies de l’Espai (CSIC–IEEC), Campus UAB, Facultat de Ciencies, Torre C5-parell, 2a planta, 08193, Bellaterra (Barcelona), Spain; [email protected] 2 SRON-Netherlands Institute for Space Research, Sorbonnelaan 2, 3584 CA Utrecht, The Netherlands 3 Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138, USA 4 Department of Astrophysics, Radboud University Nijmegen, IMAPP, P.O. Box 9010, 6500 GL, Nijmegen, The Netherlands 5 Departament de Fisica Aplicada, Universitat d’Alacant, Ap. Correus 99, 03080 Alacant, Spain 6 Department of Astronomy, California Institute of Technology, Mail Stop 105-24, Pasadena, CA 91125, USA 7 University of Amsterdam, Astronomical Institute “Anton Pannekoek,” Postbus 94249, 1090 GE, Amsterdam, The Netherlands Received 2010 November 11; accepted 2011 January 18; published 2011 February 15 ABSTRACT We report on an ∼63 ks Chandra observation of the X-ray transient Swift J195509.6+261406 discovered as the afterglow of what was first believed to be a long-duration gamma-ray burst (GRB 070610).