Communications in Asteroseismology
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Asteroseismology with ET
Asteroseismology with ET Erich Gaertig & Kostas D. Kokkotas Theoretical Astrophysics - University of Tübingen nice, et-wp4 meeting,september 1st-2nd, 2010 Asteroseismology with gravitational waves as a tool to probe the inner structure of NS • neutron stars build from single-fluid, normal matter Andersson, Kokkotas (1996, 1998) Benhar, Berti, Ferrari(1999) Benhar, Ferrari, Gualtieri(2004) Asteroseismology with gravitational waves as a tool to probe the inner structure of NS • neutron stars build from single-fluid, normal matter • strange stars composed of deconfined quarks NONRADIAL OSCILLATIONS OF QUARK STARS PHYSICAL REVIEW D 68, 024019 ͑2003͒ NONRADIAL OSCILLATIONS OF QUARK STARS PHYSICAL REVIEW D 68, 024019 ͑2003͒ H. SOTANI AND T. HARADA PHYSICAL REVIEW D 68, 024019 ͑2003͒ FIG. 5. The horizontal axis is the bag constant B (MeV/fmϪ3) Sotani, Harada (2004) FIG. 4. Complex frequencies of the lowest wII mode for each and the vertical axis is the f mode frequency Re(). The squares, stellar model except for the plot for Bϭ471.3 MeV fmϪ3, for circles, and triangles correspond to stellar models whose radiation which the second wII mode is plotted. The labels in this figure radii are fixed at 3.8, 6.0, and 8.2 km, respectively. The dotted line Benhar, Ferrari, Gualtieri, Marassicorrespond (2007) to those of the stellar models in Table I. denotes the new empirical relationship ͑4.3͒ obtained in Sec. IV between Re() of the f mode and B. simple extrapolation to quark stars is not very successful. We want to construct an alternative formula for quark star mod- fixed at Rϱϭ3.8, 6.0, and 8.2 km, and the adopted bag con- els by using our numerical results for f mode QNMs, but we stants are Bϭ42.0 and 75.0 MeV fmϪ3. -
Asteroseismic Fingerprints of Stellar Mergers
MNRAS 000,1–13 (2021) Preprint 7 September 2021 Compiled using MNRAS LATEX style file v3.0 Asteroseismic Fingerprints of Stellar Mergers Nicholas Z. Rui,1¢ Jim Fuller1 1TAPIR, California Institute of Technology, Pasadena, CA 91125, USA Accepted XXX. Received YYY; in original form ZZZ ABSTRACT Stellar mergers are important processes in stellar evolution, dynamics, and transient science. However, it is difficult to identify merger remnant stars because they cannot easily be distinguished from single stars based on their surface properties. We demonstrate that merger remnants can potentially be identified through asteroseismology of red giant stars using measurements of the gravity mode period spacing together with the asteroseismic mass. For mergers that occur after the formation of a degenerate core, remnant stars have over-massive envelopes relative to their cores, which is manifested asteroseismically by a g mode period spacing smaller than expected for the star’s mass. Remnants of mergers which occur when the primary is still on the main sequence or whose total mass is less than ≈2 " are much harder to distinguish from single stars. Using the red giant asteroseismic catalogs of Vrard et al.(2016) and Yu et al.(2018), we identify 24 promising candidates for merger remnant stars. In some cases, merger remnants could also be detectable using only their temperature, luminosity, and asteroseismic mass, a technique that could be applied to a larger population of red giants without a reliable period spacing measurement. Key words: asteroseismology—stars: evolution—stars: interiors—stars: oscillations 1 INTRODUCTION for the determination of evolutionary states (Bedding et al. 2011; Bildsten et al. -
Gaia Data Release 2 Special Issue
A&A 623, A110 (2019) Astronomy https://doi.org/10.1051/0004-6361/201833304 & © ESO 2019 Astrophysics Gaia Data Release 2 Special issue Gaia Data Release 2 Variable stars in the colour-absolute magnitude diagram?,?? Gaia Collaboration, L. Eyer1, L. Rimoldini2, M. Audard1, R. I. Anderson3,1, K. Nienartowicz2, F. Glass1, O. Marchal4, M. Grenon1, N. Mowlavi1, B. Holl1, G. Clementini5, C. Aerts6,7, T. Mazeh8, D. W. Evans9, L. Szabados10, A. G. A. Brown11, A. Vallenari12, T. Prusti13, J. H. J. de Bruijne13, C. Babusiaux4,14, C. A. L. Bailer-Jones15, M. Biermann16, F. Jansen17, C. Jordi18, S. A. Klioner19, U. Lammers20, L. Lindegren21, X. Luri18, F. Mignard22, C. Panem23, D. Pourbaix24,25, S. Randich26, P. Sartoretti4, H. I. Siddiqui27, C. Soubiran28, F. van Leeuwen9, N. A. Walton9, F. Arenou4, U. Bastian16, M. Cropper29, R. Drimmel30, D. Katz4, M. G. Lattanzi30, J. Bakker20, C. Cacciari5, J. Castañeda18, L. Chaoul23, N. Cheek31, F. De Angeli9, C. Fabricius18, R. Guerra20, E. Masana18, R. Messineo32, P. Panuzzo4, J. Portell18, M. Riello9, G. M. Seabroke29, P. Tanga22, F. Thévenin22, G. Gracia-Abril33,16, G. Comoretto27, M. Garcia-Reinaldos20, D. Teyssier27, M. Altmann16,34, R. Andrae15, I. Bellas-Velidis35, K. Benson29, J. Berthier36, R. Blomme37, P. Burgess9, G. Busso9, B. Carry22,36, A. Cellino30, M. Clotet18, O. Creevey22, M. Davidson38, J. De Ridder6, L. Delchambre39, A. Dell’Oro26, C. Ducourant28, J. Fernández-Hernández40, M. Fouesneau15, Y. Frémat37, L. Galluccio22, M. García-Torres41, J. González-Núñez31,42, J. J. González-Vidal18, E. Gosset39,25, L. P. Guy2,43, J.-L. Halbwachs44, N. C. Hambly38, D. -
ESO Annual Report 2004 ESO Annual Report 2004 Presented to the Council by the Director General Dr
ESO Annual Report 2004 ESO Annual Report 2004 presented to the Council by the Director General Dr. Catherine Cesarsky View of La Silla from the 3.6-m telescope. ESO is the foremost intergovernmental European Science and Technology organi- sation in the field of ground-based as- trophysics. It is supported by eleven coun- tries: Belgium, Denmark, France, Finland, Germany, Italy, the Netherlands, Portugal, Sweden, Switzerland and the United Kingdom. Created in 1962, ESO provides state-of- the-art research facilities to European astronomers and astrophysicists. In pur- suit of this task, ESO’s activities cover a wide spectrum including the design and construction of world-class ground-based observational facilities for the member- state scientists, large telescope projects, design of innovative scientific instruments, developing new and advanced techno- logies, furthering European co-operation and carrying out European educational programmes. ESO operates at three sites in the Ataca- ma desert region of Chile. The first site The VLT is a most unusual telescope, is at La Silla, a mountain 600 km north of based on the latest technology. It is not Santiago de Chile, at 2 400 m altitude. just one, but an array of 4 telescopes, It is equipped with several optical tele- each with a main mirror of 8.2-m diame- scopes with mirror diameters of up to ter. With one such telescope, images 3.6-metres. The 3.5-m New Technology of celestial objects as faint as magnitude Telescope (NTT) was the first in the 30 have been obtained in a one-hour ex- world to have a computer-controlled main posure. -
Magnetar Asteroseismology with Long-Term Gravitational Waves
Magnetar Asteroseismology with Long-Term Gravitational Waves Kazumi Kashiyama1 and Kunihito Ioka2 1Department of Physics, Kyoto University, Kyoto 606-8502, Japan 2Theory Center, KEK(High Energy Accelerator Research Organization), Tsukuba 305-0801, Japan Magnetic flares and induced oscillations of magnetars (supermagnetized neutron stars) are promis- ing sources of gravitational waves (GWs). We suggest that the GW emission, if any, would last longer than the observed x-ray quasiperiodic oscillations (X-QPOs), calling for the longer-term GW anal- yses lasting a day to months, compared to than current searches lasting. Like the pulsar timing, the oscillation frequency would also evolve with time because of the decay or reconfiguration of the magnetic field, which is crucial for the GW detection. With the observed GW frequency and its time-derivatives, we can probe the interior magnetic field strength of ∼ 1016 G and its evolution to open a new GW asteroseismology with the next generation interferometers like advanced LIGO, advanced VIRGO, LCGT and ET. PACS numbers: 95.85.Sz,97.60.Jd In the upcoming years, the gravitational wave (GW) In this Letter, we suggest that the GWs from magne- astronomy will be started by the 2nd generation GW de- tar GFs would last much longer than the X-QPOs if the tectors [1–3], such as advanced LIGO, advanced VIRGO GW frequencies are close to the X-QPO frequencies [see and LCGT, and the 3rd generation ones like ET [4] in the Eq.(6)]. We show that the long-term GW analyses from 10 Hz-kHz band. These GW interferometers will bring a day to months are necessary to detect the GW, even about a greater synergy among multimessenger (electro- if the GW energy is comparable to the electromagnetic magnetic, neutrino, cosmic ray and GW) signals. -
Variable Star
Variable star A variable star is a star whose brightness as seen from Earth (its apparent magnitude) fluctuates. This variation may be caused by a change in emitted light or by something partly blocking the light, so variable stars are classified as either: Intrinsic variables, whose luminosity actually changes; for example, because the star periodically swells and shrinks. Extrinsic variables, whose apparent changes in brightness are due to changes in the amount of their light that can reach Earth; for example, because the star has an orbiting companion that sometimes Trifid Nebula contains Cepheid variable stars eclipses it. Many, possibly most, stars have at least some variation in luminosity: the energy output of our Sun, for example, varies by about 0.1% over an 11-year solar cycle.[1] Contents Discovery Detecting variability Variable star observations Interpretation of observations Nomenclature Classification Intrinsic variable stars Pulsating variable stars Eruptive variable stars Cataclysmic or explosive variable stars Extrinsic variable stars Rotating variable stars Eclipsing binaries Planetary transits See also References External links Discovery An ancient Egyptian calendar of lucky and unlucky days composed some 3,200 years ago may be the oldest preserved historical document of the discovery of a variable star, the eclipsing binary Algol.[2][3][4] Of the modern astronomers, the first variable star was identified in 1638 when Johannes Holwarda noticed that Omicron Ceti (later named Mira) pulsated in a cycle taking 11 months; the star had previously been described as a nova by David Fabricius in 1596. This discovery, combined with supernovae observed in 1572 and 1604, proved that the starry sky was not eternally invariable as Aristotle and other ancient philosophers had taught. -
Astrophysics
A&A 424, 935–950 (2004) Astronomy DOI: 10.1051/0004-6361:20040517 & c ESO 2004 Astrophysics Multi-element abundance Doppler imaging of the rapidly oscillating Ap star HR 3831 O. Kochukhov1,N.A.Drake2,3, N. Piskunov4, and R. de la Reza2 1 Institut für Astronomie, Universität Wien, Türkenschanzstraße 17, 1180 Wien, Austria e-mail: [email protected] 2 Observatório Nacional/MCT, Rua General Jose Cristino 77, 20921-400, Rio de Janeiro, Brazil 3 Sobolev Astronomical Institute, St. Petersburg State University, Universitetsky pr. 28, Petrodvorets, 198504, St. Petersburg, Russia 4 Department of Astronomy and Space Physics, Uppsala University, Box 515, 751 20 Uppsala, Sweden Received 25 March 2004 / Accepted 24 May 2004 Abstract. We investigate magnetic field geometry and surface distribution of chemical elements in the rapidly oscillating Ap star HR 3831. Results of the model atmosphere analysis of the spectra of this star are combined with the Hipparcos parallax and evolutionary models to obtain new accurate estimates of the fundamental stellar parameters: Teff = 7650 K, log L/L = ◦ 1.09, M/M = 1.77 and an inclination angle i = 68 of the stellar axis of rotation. We find that the variation of the longitudinal magnetic field of HR 3831 and the results of our analysis of the magnetic intensification of Fe lines in the spectrum of this ◦ star are consistent with a dipolar magnetic topology with a magnetic obliquity β = 87 and a polar strength Bp = 2.5kG. We apply a multi-element abundance Doppler imaging inversion code for the analysis of the spectrum variability of HR 3831, and recover surface distributions of 17 chemical elements, including Li, C, O, Na, Mg, Si, Ca, Ti, Cr, Mn, Fe, Co, Ba, Y, Pr, Nd, Eu. -
Asteroseismology
Asteroseismology Gerald Handler Copernicus Astronomical Center, Bartycka 18, 00-716 Warsaw, Poland Email: [email protected] Abstract Asteroseismology is the determination of the interior structures of stars by using their oscillations as seismic waves. Simple explanations of the astrophysical background and some basic theoretical considerations needed in this rapidly evolving field are followed by introductions to the most important concepts and methods on the basis of example. Previous and potential applications of asteroseismology are reviewed and future trends are attempted to be foreseen. Introduction: variable and pulsating stars Nearly all the physical processes that determine the structure and evolution of stars occur in their (deep) interiors. The production of nuclear energy that powers stars takes place in their cores for most of their lifetime. The effects of the physical processes that modify the simplest models of stellar evolution, such as mixing and diffusion, also predominantly take place in the inside of stars. The light that we receive from the stars is the main information that astronomers can use to study the universe. However, the light of the stars is radiated away from their surfaces, carrying no memory of its origin in the deep interior. Therefore it would seem that there is no way that the analysis of starlight tells us about the physics going on in the unobservable stellar interiors. However, there are stars that reveal more about themselves than others. Variable stars are objects for which one can observe time-dependent light output, on a time scale shorter arXiv:1205.6407v1 [astro-ph.SR] 29 May 2012 than that of evolutionary changes. -
Diagnostics of the Unstable Envelopes of Wolf-Rayet Stars L
Astronomy & Astrophysics manuscript no. 27873_am c ESO 2021 September 13, 2021 Diagnostics of the unstable envelopes of Wolf-Rayet stars L. Grassitelli1,? , A.-N. Chené2 , D. Sanyal1 , N. Langer1 , N. St.Louis3 , J.M. Bestenlehner4; 1, and L. Fossati5; 1 1 Argelander-Institut für Astronomie, Universität Bonn, Auf dem Hügel 71, 53121 Bonn, Germany 2 Gemini Observatory, Northern Operations Center, 670 North A’ohoku Place, Hilo, HI 96720, USA 3 Département de Physique, Pavillon Roger Gaudry, Université Montréal, CP 6128, Succ. Centre-Ville, Montréal, H3C 3J7 Quebec, Canada 4 Max-Planck-Institute for Astronomy, Königstuhl 17, 69117 Heidelberg, Germany 5 Space Research Institute, Austrian Academy of Sciences, Schmiedlstrasse 6, A-8042 Graz, Austria Received //, 2015 ABSTRACT Context. The envelopes of stars near the Eddington limit are prone to various instabilities. A high Eddington factor in connection with the iron opacity peak leads to convective instability, and a corresponding envelope inflation may induce pulsational instability. Here, we investigate the occurrence and consequences of both instabilities in models of Wolf-Rayet stars. Aims. We determine the convective velocities in the sub-surface convective zones to estimate the amplitude of the turbulent velocity at the base of the wind that potentially leads to the formation of small-scale wind structures, as observed in several Wolf-Rayet stars. We also investigate the effect of stellar wind mass loss on the pulsations of our stellar models. Methods. We approximated solar metallicity Wolf-Rayet stars in the range 2−17 M by models of mass-losing helium stars, computed with the Bonn stellar evolution code. We characterized the properties of convection in the envelope of these stars adopting the standard mixing length theory. -
On the Eddington Limit and Wolf-Rayet Stars
A&A 539, A110 (2012) Astronomy DOI: 10.1051/0004-6361/201118328 & c ESO 2012 Astrophysics On the Eddington limit and Wolf-Rayet stars A. Maeder1,C.Georgy2,G.Meynet1, and S. Ekström1 1 Geneva Observatory, Geneva University, 1290 Sauverny, Switzerland e-mail: [andre.maeder;georges.meynet;sylvia.ekstrom]@unige.ch 2 Centre de Recherche Astrophysique, École Normale Supérieure de Lyon, 46 allée d’Italie, 69384 Lyon Cedex 07, France e-mail: [email protected] Received 25 October 2011 / Accepted 13 January 2012 ABSTRACT Aims. We examine some properties of stars evolving close to the classical Eddington limit for electron-scattering opacity, when these stars maintain a chemically homogeneous structure as a result of mixing and/or mass loss. Methods. We consider analytical relations and models computed with the Geneva code. Results. Homologous, chemically homogeneous stars evolving with a constant Eddington factor obey a relation of the form μ2 M = const. This applies, for example, to Wolf-Rayet (WR) stars in stages without hydrogen. The value of the constant may depend on the metallicity, initial mass, evolutionary stage, and physical processes included in the considered homologous evolutionary sequence. An average value of the constant between 20 and 40 in solar units is consistent with the masses of Galactic WR stars. Key words. stars: evolution – circumstellar matter – stars: mass-loss – stars: massive – stars: Wolf-Rayet 1. Introduction An additional motivation for this study is that the homoge- neous evolution of massive hot stars has been proposed as the Stars must have a luminosity inferior to the Eddington limit, oth- scenario leading to long-soft gamma ray bursts (Yoon & Langer erwise “.. -
A Study of the Variability of Yellow Supergiant Stars
Searching for frequency multiplets in the pulsating subdwarf B star PG 1219+534 John Crooke, Ryan Roessler Advisor: Mike Reed Physics, Astronomy, and Materials Science 0 | 4/22/2017 | Physics, Astronomy, and Materials Science Asteroseismology • Study of pulsations to g-modes infer internal structure • Only way to “observe” the inside of a star • Two oscillation modes • p: pressure mode, high frequency • g: gravity mode, low frequency p-modes 1 | 4/22/2017 | Physics, Astronomy, and Materials Science Asteroseismology m= 0 1 2 3 4 • Using frequency multiplets (rotation period), it is 0 possible to remove azimuthal degeneracy and associate pulsations with 1 spherical harmonics • Angular degree: l l= 2 • # of nodal lines • Azimuthal order: m 3 • # of nodal lines crossing equator • Radial order: n 4 • # of nodal lines along radius 2 | 4/22/2017 | Physics, Astronomy, and Materials Science Subdwarf B (sdB) stars • 0.5 Msun, 0.2 Rsun • 20,000 – 30,000 K • Horizontal Branch • post helium-flash • Thin, inert envelopes1 • Helium fusing cores 3 | 4/22/2017 | Physics, Astronomy, and Materials Science Previous Work on PG1219+534 • Four dominant • Frequency multiplets pulsation frequencies2 indicating rotation 3 • 6721 μHZ, 148.8 seconds period of ~35 days No evidence or data • 6961 μHZ, 143.7 seconds • published • 7590 μHZ, 131.8 seconds • 7807 μHZ, 128.1 seconds • Goal of project is to find evidence of this rotation 4 | 4/22/2017 | Physics, Astronomy, and Materials Science Observations • January-August 2015, Baker Observatory • Baker Observatory Robotic -
Asteroseismology and Transport Processes in Stellar Interiors
AAsstteerroosseeiissmmoollooggyy aanndd ttrraannssppoorrtt pprroocceesssseess iinn sstteellllaarr iinntteerriioorrss Patrick Eggenberger Département d’Astronomie de l’Université de Genève In collaboration with: Gaël Buldgen, Sébastien Deheuvels, Jacqueline den Hartogh, Georges Meynet, Camilla Pezzotti, Sébastien Salmon Asteroseismology of MS stars • The solar rotation profile – Helioseismic measurements Garcia et al. 2007, Science, 316, 1591 — Inefficient transport by hydrodynamic processes Pinsonneault et al. 1989; Chaboyer et al. 1995; Talon et al. 1997; Eggenberger et al. 2005; Turck-Chièze et al. 2010 Asteroseismology of MS stars • The solar rotation profile: magnetic fields – Steady internal field in radiative zones ? – issue: mechanical coupling to the convective zone – Small-scale dynamos in radiative zones ? – Tayler-Spruit: Braithwaite (2006); Zahn et al. (2007) – MRI (strong shears): Arlt et al. (2003); Rüdiger et al. (2014, 2015); Jouve et al. (2015) Eggenberger et al. 2019a, A&A, 626, L1 Asteroseismology of MS stars • Solar-like oscillations in MS stars mean internal rotation from rotational splittings + independent measurements of surface rotation rates Benomar et al. 2015, MNRAS, 452, 2654 Nielsen et al. 2015, A&A, 582, A10 Asteroseismology of MS stars • Impact of an efficient AM transport on rotating MS models Eggenberger et al. 2010, A&A, 519, A116 Asteroseismology of red giants Mixed modes in the 1.5 M red giant KIC 8366239 (Beck et al. 2012) - Inefficient AM transport by hydrodynamic processes - Efficiency of the needed additional mechanism can be precisely determined thanks to seismic constraints (Eggenberger et al. 2012) 4 2 -1 νadd = 3⋅10 cm s Eggenberger et al. 2012, A&A, 544, L4 Asteroseismology of red giants KIC 7341231: a low-mass (0.84 M) red giant (Deheuvels et al.