Exploring the Final Stages of Stars in Our Milky Way Using Large Sky

Total Page:16

File Type:pdf, Size:1020Kb

Exploring the Final Stages of Stars in Our Milky Way Using Large Sky Exploring the final stages of stars in our Milky Way using large sky surveys by Sandra Magdy Kamel Greiss Thesis Submitted to the University of Warwick for the degree of Doctor of Philosophy Department of Physics July 2014 Contents List of Tables iv List of Figures vi Acknowledgments xiv Declarations xvi Abstract xvii Chapter 1 Motivation 1 Chapter 2 Compact stars 5 2.1 TheHertzsprung-Russelldiagram . 5 2.2 Stellar evolution in a nutshell . 5 2.2.1 Nuclearprocesses......................... 5 2.2.2 Shell-hydrogen burning and red-giant phase . 7 2.2.3 Death of stars like the Sun . 9 2.2.4 Death of massive stars . 10 2.3 WhiteDwarfs............................... 11 2.3.1 Spectraltypes .......................... 12 2.3.2 Massdistribution. .. .. .. .. .. .. .. 12 2.3.3 Whyaretheyuseful? ...................... 12 2.3.4 Pulsatingwhitedwarfs. 16 2.3.4.1 Theoretical context . 17 2.4 NeutronStars............................... 23 2.5 Blackholes ................................ 25 2.6 Compactbinarysystems. 25 2.6.1 Cataclysmic variables . 26 2.6.2 Low-massX-raybinaries. 28 Chapter 3 Astronomical tools and methods 30 3.1 Charge-coupleddevices . 30 3.2 Photometry ................................ 30 3.2.1 Colour-colour and colour-magnitude diagrams . 34 3.2.2 Time-series photometry . 34 i 3.3 Spectroscopy ............................... 36 3.3.1 Biasremoval ........................... 36 3.3.2 FlatFielding ........................... 37 3.3.3 Spectrum extraction . 37 3.3.4 Wavelength calibration . 37 3.3.5 Flux calibration . 37 3.4 Summary ................................. 38 Chapter 4 Large Sky Surveys 39 4.1 X-raysurvey ............................... 39 4.1.1 Galactic Bulge Survey (GBS) . 39 4.2 Thenear-infraredsurveys . 41 4.2.1 The Two Micron All Sky Survey (2MASS) . 41 4.2.2 UKIDSS Galactic Plane Survey (GPS) . 42 4.2.3 VISTA Variables in the Via Lactea (VVV) . 43 4.3 Optical survey: The Kepler-INTSurvey ................ 45 4.3.1 Kepler mission .......................... 45 4.3.2 Survey imaging with the Isaac Newton Telescope . 48 4.3.3 INT observations and data . 49 4.3.3.1 Observations . .. .. .. .. .. .. 49 4.3.3.2 Data .......................... 49 4.3.3.3 Quality control flags . 50 4.3.3.4 Photometric calibration . 50 4.3.3.5 Catalogue description . 56 4.4 Summary ................................. 60 Chapter 5 Near-infrared and optical study of the GBS sources 63 5.1 Near-infrared coverage of the Bulge . 63 5.1.1 Coverage ............................. 63 5.1.2 VVVvs2MASS ......................... 64 5.1.3 VVVvsUKIDSSGPS...................... 66 5.2 Extinction................................. 68 5.3 Results................................... 69 5.3.1 Quantifying the false alarm rate . 71 5.3.2 Randommatching ........................ 72 5.3.3 Positional uncertainties . 74 5.3.4 TotalFAP............................. 74 5.3.5 Multiplematches. .. .. .. .. .. .. .. 74 5.3.6 Finaltable ............................ 78 5.3.7 Influence of the hardness of the X-ray sources . 81 5.4 Near-infrared photometry discussion . 81 5.4.1 NIR colours of Hα emission line objects . 81 5.4.2 Towards the identification of key GBS source classes . 83 5.5 VVVVariability ............................. 84 5.6 Mosaicopticaldata............................ 88 ii 5.7 OpticalVariability ............................ 94 5.8 Summary ................................. 96 Chapter 6 White dwarfs in the Kepler field 99 6.1 Searching for white dwarfs in the Kepler field ............. 99 6.2 Spectroscopy ............................... 99 6.3 Ground-based confirmation of pulsators . 107 6.4 Kepler dataoffourZZCetistars . 108 6.4.1 KIC11911480........................... 108 6.4.1.1 Significance threshold . 113 6.4.1.2 Pulsation modes of KIC 11911480 . 113 6.4.1.3 Rotation rate of KIC 11911480 . 116 6.4.2 KIC10132702........................... 118 6.4.2.1 Pulsation modes of KIC 10132702 . 118 6.4.2.2 Rotation rate of KIC 10132702 . 118 6.4.3 KIC04357037........................... 120 6.4.3.1 Pulsation modes of KIC 04357037 . 121 6.4.3.2 Rotation rate of KIC 04357037 . 121 6.4.4 KIC07594781........................... 123 6.4.4.1 Pulsation modes of KIC 07594781 . 123 6.4.4.2 Rotation rate of KIC 07594781 . 124 6.4.5 Summary ............................. 125 6.5 Asteroseismic model of KIC 11911480 . 126 6.5.1 Method .............................. 127 6.5.2 Optimalmodel .......................... 128 6.5.3 Stellar rotation . 128 6.5.4 Nonadiabatic approach . 132 6.5.5 Asteroseismic properties of KIC 11911480 . 133 Chapter 7 Conclusion and future work 135 Abbreviations 139 iii List of Tables 2.1 Stellar evolution end-states as a function of initial masse (Tauris & van den Heuvel, 2006) .......................... 11 2.2 White dwarf spectral types (Koester, 2013). .............. 13 2.3 Observational properties of LMXBs (Tauris & van den Heuvel, 2006) 29 4.1 Exposure times and 5σ limiting magnitudes in all three NIR surveys used in this paper. The GPS integration times are longer than those applied in VVV, allowing for deeper observations of the Bulge than VVV. The magnitude limits given here are for fields that are moder- ately crowded similar to the GBS areas. ................ 45 4.2 Filter parameters of INT observations (Gonz´alez-Solares et al., 2008; Groot et al., 2009) ............................ 48 4.3 Morphological flags ........................... 50 4.4 ∆ filter is the median offset between the KIC and KIS magnitudes { } (see Section 4.3.3.4). The standard deviations of the distributions in each filter are also given here (σ filter ). The distributions are shown in Figure 4.8. ...............................{ } 54 4.5 Description of columns in KIS catalogue ............... 61 4.6 Example of light version of the KIS catalogue ............. 62 5.1 Percentage of total number of GBS X-ray sources with possible coun- terparts found within a 5 arcseconds (upper section) radius and 2.8 arcseconds (lower section) of the X-ray positions, in 2MASS, UKIDSS GPS (DR8) and VVV .......................... 65 5.2 Positions of the 4 closest matches of CX0013 found within R95 in VVV. The red cross indicates the X-ray position and the large dashed green circle indicates the R95 boundary of 2.84 arcseconds in this case. The table below provides information on their magnitudes and false alarm probabilities. ........................... 78 5.3 Four closest VVV matches to CX0013. ................ 78 5.4 Table containing all NIR data and FAP of matches within R95 . 80 6.1 Summary of photometric data of our WD candidates selected for spec- troscopic follow-up. ........................... 102 iv 6.2 Summary of spectroscopic observations and results from model atmo- sphere fits to the spectra. ........................ 106 6.3 Summary of ground-based time-series data of six ZZ Ceti stars con- firmed from our survey. The dominant periods and frequencies found in the amplitude power spectra of each source are given here. 108 6.4 Pulsation frequencies of KIC 11911480 from the Q12 and Q16 data. The uncertainties are given in parentheses. ∆f corresponds to the frequency spacing between two consecutive frequencies in the table . 112 6.5 Pulsation frequencies of KIC 10132702 from the Q15 data. ∆f cor- responds to the frequency spacing between two consecutive frequencies in the table ................................ 119 6.6 Pulsation frequencies of KIC 04357037 from one month of Q16 obser- vations. ∆f corresponds to the frequency spacing between two con- secutive frequencies in the table ..................... 122 6.7 Pulsation frequencies of KIC 07594781 from one month of Q16 obser- vations. ∆f corresponds to the frequency spacing between two con- secutive frequencies in the table ..................... 123 6.8 Identified modes and their periods of optimal model of KIC 11911480. 129 6.9 Pulsation frequencies of KIC 11911480 from the combined Q12 and Q16 data (see Table 6.4). The uncertainties are given in between brackets. ∆f corresponds to the frequency spacing between two con- secutive frequencies in the table. ..................... 131 6.10 Non adiabatic properties of the optimal model of KIC 11911480. 133 v List of Figures 2.1 The Hertzsprung-Russell diagram, showing the locii of the main-sequence where most stars actually lie, as well as other phases. The positions of some specific stars are also included in this sketch. ......... 6 2.2 The H-R diagram with evolutionary tracks of stars with different main-sequence masses. .......................... 8 2.3 Sketch of the stellar composition during different stages of its stellar evolution. ................................. 9 2.4 SDSS DA, DB, DAO and DZ spectra of white dwarf stars (top to bottom). The legend for the lines is the following: cyan H, pink ≡ dashed HeI, blue dotted HeII, yellow CaII. .......... 14 ≡ ≡ ≡ 2.5 Surface gravity and mass distribution of DA WD stars with Teff >13 000 K from the Palomar Green survey (Liebert et al., 2005). The mean values and standard deviations of both distributions are given at the top of each panel. ............................ 15 2.6 A pulsation H-R diagram showing different classes of pulsating stars, taken from Aerts et al. (2010). ..................... 16 2.7 Chemical composition of ZZ Ceti model (taken from Fontaine & Bras- sard 2008). The x-axis corresponds to the logarithm of the fractional mass depth, a scale chosen to emphasize the outer layers of the star, where most of the ‘action’ takes place. ................. 18 2.8 Profiles of the Lamb (dotted) and Brunt-V¨ais¨al¨a(solid) frequencies in a typical ZZ Ceti model (taken from Fontaine & Brassard 2008). 20 2.9 Typical ZZ Ceti model with excited mode l=1, k=1 (taken from Fontaine & Brassard 2008). For the explanation of curves, see Section 2.3.4.1. 22 2.10 Mass-radius diagram for neutron stars, taken from Lattimer & Prakash 2004. The black and green curves are for different equations of state of neutron stars. Regions excluded by general relativity (GR), causal- ity, and rotation constraints are also indicated. ............ 24 2.11 Equipotential lines in a binary system, also indicating the five Lagrangian points of potential equilibrium (Tauris & van den Heuvel, 2006). ..... 27 3.1 Illustration of the concept of a CCD where the ‘raindrops’ are actually the photons.
Recommended publications
  • Toward an Empirical Determination of the Zz Ceti Instability Strip A
    The Astrophysical Journal, 631:1100–1112, 2005 October 1 # 2005. The American Astronomical Society. All rights reserved. Printed in U.S.A. TOWARD AN EMPIRICAL DETERMINATION OF THE ZZ CETI INSTABILITY STRIP A. Gianninas, P. Bergeron, and G. Fontaine De´partement de Physique, Universite´ de Montre´al, C.P. 6128, Succursale Centreville, Montreal, PQ H3C 3J7, Canada; [email protected], [email protected], [email protected] Received 2005 April 22; accepted 2005 June 17 ABSTRACT We present atmospheric parameters for a large sample of DA white dwarfs that are known to be photometrically constant. For each star, we determine the effective temperature and surface gravity by comparing high signal-to-noise ratio optical spectra to the predictions of detailed model atmosphere calculations. We also report the successful prediction and detection of photometric variability in G232À38 based on similar Teff and log g determinations. The atmospheric parameters derived for this sample of constant stars, as well as those for the known sample of bright ZZ Ceti stars (now boosted to a total of 39), have been obtained in a highly homogeneous way. We combine them to study the empirical red and blue edges, as well as the purity of the ZZ Ceti instability strip. We find that the red edge is rather well constrained, whereas there exists a rather large range of possibilities for the slope of the blue edge. Furthermore, the ZZ Ceti instability strip that results from our analysis contains no nonvariable white dwarfs. Our sample of constant stars is part of a much broader spectroscopic survey of bright (V < 17) DAwhite dwarfs, which we have recently undertaken.
    [Show full text]
  • Arxiv:1706.07020V1 [Astro-Ph.SR] 21 Jun 2017
    Pulsating White Dwarfs S. O. Kepler1;? and Alejandra D. Romero1;?? 1Departamento de Astronomia, Instituto de Física, Universidade Federal do Rio Grande do Sul, 91501-970 Porto Alegre, RS - Brasil Abstract. The Sloan Digital Sky Survey has allowed us to increase the number of known white dwarfs by a factor of five and consequently the number of known pulsating white dwarfs also by a factor of five. It has also led to the discovery of new types of variable white dwarfs, as the variable hot DQs, and the pulsating Extremely Low Mass white dwarfs. With the Kepler Mission, it has been possible to discover new phenomena, the outbursts present in a few pulsating white dwarfs. 1 Introduction White dwarf stars are the final evolutionary state of stars with initial masses up to 8.5–10.6 M [1], corresponding to 95 – 97 % of all stars. The fraction depends on the stellar metallicity, which affects both the Initial-Mass-Function and the Initial-to-Final-Mass Relation. For single stars, the minimum mass of a present day white dwarf is around 0.30–0.45 M [2], because progenitors that would become lower mass white dwarfs have main sequence evolution time larger than the age of the Universe. Such masses correspond, considering the mass-radius relation of white dwarfs, to a minimal log g ' 6:5. Evolutionary models e.g. by Ref. [3] indicate that the maximum surface gravity for main sequence A stars, which have similar optical spectra to DA white dwarfs, corresponds to log g ≤ 4:75, including very low metallicity.
    [Show full text]
  • TESS First Look at Evolved Compact Pulsators: Known ZZ Ceti Stars Of
    Astronomy & Astrophysics manuscript no. 18DAVs c ESO 2020 March 26, 2020 TESS first look at evolved compact pulsators: Known ZZ Ceti stars of the southern ecliptic hemisphere as seen by TESS Zs. Bognár1, 2, 3,⋆, S. D. Kawaler4, K. J. Bell5, 6, C. Schrandt4, A. S. Baran7, P. A. Bradley8, J. J. Hermes9, S. Charpinet10, G. Handler11, S. E. Mullally12, S. J. Murphy13, R. Raddi14, 15, Á. Sódor1, 2, P.-E. Tremblay16 M. Uzundag17, and W. Zong18 1 Konkoly Observatory, Research Centre for Astronomy and Earth Sciences, Konkoly Thege Miklós út 15-17, H–1121, Budapest, Hungary 2 MTA CSFK Lendület Near-Field Cosmology Research Group 3 ELTE Eötvös Loránd University, Institute of Phyiscs, Pázmány Péter sétány 1/A, H-1171, Budapest, Hungary 4 Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA 5 DIRAC Institute, Department of Astronomy, University of Washington, Seattle, WA 98195-1580, USA 6 NSF Astronomy and Astrophysics Fellow and DIRAC Fellow 7 ARDASTELLA Research Group, Institute of Physics, Pedagogical University of Cracow, ul. Podchora¸˙zych 2, 30-084 Kraków, Poland 8 XCP-6, MS F-699 Los Alamos National Laboratory, Los Alamos, NM 87545, USA 9 Department of Astronomy, Boston University, 725 Commonwealth Ave., Boston, MA 02215 - USA 10 Institut de Recherche en Astrophysique et Planétologie, CNRS, Université de Toulouse, CNES, 14 avenue Edouard Belin, F-31400 Toulouse, France 11 Nicolaus Copernicus Astronomical Center, Bartycka 18, 00-716 Warsaw, Poland 12 Space Telescope Science Institute, 3700 San Martin Dr., Baltimore MD 21212 13 Sydney Institute for Astronomy (SIfA), School of Physics, The University of Sydney, NSW 2006, Australia 14 Dr.
    [Show full text]
  • Survival of Exomoons Around Exoplanets 2
    Survival of exomoons around exoplanets V. Dobos1,2,3, S. Charnoz4,A.Pal´ 2, A. Roque-Bernard4 and Gy. M. Szabo´ 3,5 1 Kapteyn Astronomical Institute, University of Groningen, 9747 AD, Landleven 12, Groningen, The Netherlands 2 Konkoly Thege Mikl´os Astronomical Institute, Research Centre for Astronomy and Earth Sciences, E¨otv¨os Lor´and Research Network (ELKH), 1121, Konkoly Thege Mikl´os ´ut 15-17, Budapest, Hungary 3 MTA-ELTE Exoplanet Research Group, 9700, Szent Imre h. u. 112, Szombathely, Hungary 4 Universit´ede Paris, Institut de Physique du Globe de Paris, CNRS, F-75005 Paris, France 5 ELTE E¨otv¨os Lor´and University, Gothard Astrophysical Observatory, Szombathely, Szent Imre h. u. 112, Hungary E-mail: [email protected] January 2020 Abstract. Despite numerous attempts, no exomoon has firmly been confirmed to date. New missions like CHEOPS aim to characterize previously detected exoplanets, and potentially to discover exomoons. In order to optimize search strategies, we need to determine those planets which are the most likely to host moons. We investigate the tidal evolution of hypothetical moon orbits in systems consisting of a star, one planet and one test moon. We study a few specific cases with ten billion years integration time where the evolution of moon orbits follows one of these three scenarios: (1) “locking”, in which the moon has a stable orbit on a long time scale (& 109 years); (2) “escape scenario” where the moon leaves the planet’s gravitational domain; and (3) “disruption scenario”, in which the moon migrates inwards until it reaches the Roche lobe and becomes disrupted by strong tidal forces.
    [Show full text]
  • Measuring the Evolutionary Rate of Cooling of ZZ Ceti
    Publications 7-1-2013 Measuring the Evolutionary Rate of Cooling of ZZ Ceti Anjum S. Mukadam University of Washington - Seattle Campus Ted von Hippel Embry-Riddle Aeronautical University, [email protected] et al. Follow this and additional works at: https://commons.erau.edu/publication Part of the Stars, Interstellar Medium and the Galaxy Commons Scholarly Commons Citation Mukadam, A. S., von Hippel, T., & al., e. (2013). Measuring the Evolutionary Rate of Cooling of ZZ Ceti. The Astrophysical Journal, 771(1). https://doi.org/10.1088/0004-637X/771/1/17 This Article is brought to you for free and open access by Scholarly Commons. It has been accepted for inclusion in Publications by an authorized administrator of Scholarly Commons. For more information, please contact [email protected]. The Astrophysical Journal, 771:17 (11pp), 2013 July 1 doi:10.1088/0004-637X/771/1/17 C 2013. The American Astronomical Society. All rights reserved. Printed in the U.S.A. MEASURING THE EVOLUTIONARY RATE OF COOLING OF ZZ Ceti Anjum S. Mukadam1,2, Agnes Bischoff-Kim3, Oliver Fraser1,2,A.H.Corsico´ 4,5, M. H. Montgomery6,7,8, S. O. Kepler9, A. D. Romero9,D.E.Winget6,8, J. J. Hermes6,8, T. S. Riecken1,2, M. E. Kronberg1,2,K.I.Winget6,8, Ross E. Falcon6,8, D. W. Chandler10, J. W. Kuehne8, D. J. Sullivan11, D. Reaves6,8, T. von Hippel12, F. Mullally13, H. Shipman7,14, S. E. Thompson13, N. M. Silvestri1,2, and R. I. Hynes15 1 Department of Astronomy, University of Washington, Seattle, WA 98195, USA 2 Apache Point Observatory, 2001 Apache Point Road, Sunspot, NM 88349, USA 3 Georgia College & State University, Milledgeville, GA 31061, USA 4 Facultad de Ciencias Astronomicas´ y Geof´ısicas, Universidad Nacional de La Plata, Argentina 5 Consejo Nacional de Investigaciones Cient´ıficas y Tecnicas´ (CONICET), Argentina 6 Department of Astronomy, University of Texas at Austin, Austin, TX 78759, USA 7 Delaware Asteroseismic Research Center, Mt.
    [Show full text]
  • Amplitude and Frequency Modulations of Oscillation Modes in Hot B Subdwarf and White Dwarf Stars from Kepler Photometry Weikai Zong
    Amplitude and frequency modulations of oscillation modes in hot B subdwarf and white dwarf stars from Kepler photometry Weikai Zong To cite this version: Weikai Zong. Amplitude and frequency modulations of oscillation modes in hot B subdwarf and white dwarf stars from Kepler photometry. Astrophysics [astro-ph]. Université Toulouse 3 Paul Sabatier, 2016. English. tel-01434986 HAL Id: tel-01434986 https://tel.archives-ouvertes.fr/tel-01434986 Submitted on 13 Jan 2017 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. THÈSETHÈSE En vue de l’obtention du DOCTORAT DE L’UNIVERSITÉ DE TOULOUSE Délivré par : l’Université Toulouse 3 Paul Sabatier (UT3 Paul Sabatier) Présentée et soutenue le 17/10/2016 par : Weikai ZONG Amplitude and frequency modulations of oscillation modes in hot B subdwarf and white dwarf stars from Kepler photometry JURY Dr. Marie-Jo Goupil Astronome Rapporteur Dr. Roberto Silvotti Chercheur Rapporteur Prof. Jianning FU Professeur Examinateur Prof. Sylvie VAUCLAIR Professeur d’Université Président Dr. Gérard VAUCLAIR Directeur de Recherche Co-Directeur de thèse Dr. Stéphane Chargé de Recherche Directeur de thèse CHARPINET École doctorale et spécialité : SDU2E : Astrophysique, Sciences de l’Espace, Planétologie Unité de Recherche : Institut de Recherche en Astrophysique et Planétologie (UMR 5277) Directeur de Thèse : Dr.
    [Show full text]
  • Pulsating White Dwarfs: New Insights
    The Astronomy and Astrophysics Review (2019) 27:7 https://doi.org/10.1007/s00159-019-0118-4 REVIEW ARTICLE Pulsating white dwarfs: new insights Alejandro H. Córsico1,2 · Leandro G. Althaus1,2 · Marcelo M. Miller Bertolami1,2 · S. O. Kepler3 Received: 11 March 2019 © Springer-Verlag GmbH Germany, part of Springer Nature 2019 Abstract Stars are extremely important astronomical objects that constitute the pillars on which the Universe is built, and as such, their study has gained increasing interest over the years. White dwarf stars are not the exception. Indeed, these stars constitute the final evolutionary stage for more than 95% of all stars. The Galactic population of white dwarfs conveys a wealth of information about several fundamental issues and are of vital importance to study the structure, evolution and chemical enrichment of our Galaxy and its components—including the star formation history of the Milky Way. Several important studies have emphasized the advantage of using white dwarfs as reliable clocks to date a variety of stellar populations in the solar neighborhood and in the nearest stellar clusters, including the thin and thick disks, the Galactic spheroid and the system of globular and open clusters. In addition, white dwarfs are tracers of the evolution of planetary systems along several phases of stellar evolution. Not less relevant than these applications, the study of matter at high densities has benefited from our detailed knowledge about evolutionary and observational properties of white dwarfs. In this sense, white dwarfs are used as laboratories for astro-particle physics, being their interest focused on physics beyond the standard model, that is, neutrino physics, axion physics and also radiation from “extra dimensions”, and even B Alejandro H.
    [Show full text]
  • Arxiv:1907.00115V1 [Astro-Ph.SR] 28 Jun 2019
    Noname manuscript No. (will be inserted by the editor) Pulsating white dwarfs: new insights Alejandro H. C´orsico, Leandro G. Althaus, Marcelo M. Miller Bertolami, S. O. Kepler Received: July 2, 2019/ Accepted: July 2, 2019 Abstract Stars are extremely important astronomical objects that constitute the pillars on which the Universe is built, and as such, their study has gained increasing interest over the years. White dwarf stars are not the exception. Indeed, these stars constitute the final evolutionary stage for more than 95 per cent of all stars. The Galactic population of white dwarfs conveys a wealth of information about several fundamental issues and are of vital importance to study the structure, evolution and chemical enrichment of our Galaxy and its components — including the star formation history of the Milky Way. Several important studies have emphasized the advantage of using white dwarfs as reliable clocks to date a variety of stellar populations in the solar neighborhood and in the nearest stellar clusters, including the thin and thick disks, the Galactic spheroid and the system of globular and open clusters. In addition, white dwarfs are tracers of the evolution of planetary systems along several phases of stellar evolution. Not less relevant than these applications, the study of matter at high densities has benefited from our detailed knowledge about evolutionary and observational properties of white dwarfs. In this sense, white dwarfs are used as laboratories for astro-particle physics, being their interest focused on physics beyond the standard model, that is, neutrino physics, axion physics and also radiation from “extra dimensions”, and even crystallization.
    [Show full text]
  • White Dwarf Stars from the 4.5 Million SDSS Spectra Through Their Colors, Automated Spectra fitting by the SDSS Pipeline, and Targeted Search of Template Spectra
    February 7, 2017 1:27 WSPC/INSTRUCTION FILE kepler International Journal of Modern Physics: Conference Series c The Authors White Dwarf Stars S. O. Kepler, Alejandra Daniela Romero, Ingrid Pelisoli & Gustavo Ourique Departamento de Astronomia, Instituto de F´ısica, Universidade Federal do Rio Grande do Sul, 91501-970 Porto Alegre, RS, Brazil [email protected] Received 3 Feb 2017 White dwarf stars are the final stage of most stars, born single or in multiple systems. We discuss the identification, magnetic fields, and mass distribution for white dwarfs detected from spectra obtained by the Sloan Digital Sky Survey up to Data Release 13 in 2016, which lead to the increase in the number of spectroscopically identified white dwarf stars from 5 000 to 39 000. This number includes only white dwarf stars with log g ≥ 6.5 stars, i.e., excluding the Extremely Low Mass white dwarfs, which are necessarily the byproduct of stellar interaction. Keywords: white dwarf; magnetic field; pulsar. PACS numbers: 1. Introduction White dwarf stars are the final evolutionary state of stars with initial masses up 1 to 8.5–10.6 M⊙ , corresponding to 95 – 97 % of all stars. The fraction depends on the stellar metallicity, which affects both the Initial-Mass-Function and the Initial- to-Final-Mass Relation. For single stars, the minimum mass of a present day white 2 arXiv:1702.01134v1 [astro-ph.SR] 3 Feb 2017 dwarf is around 0.30–0.45 M⊙ , because progenitors that would become lower mass white dwarfs have main sequence evolution time larger than the age of the Universe.
    [Show full text]
  • Frequency Analysis of DAV Pulsators Using TESS Data
    Iowa State University Capstones, Theses and Graduate Theses and Dissertations Dissertations 2019 Frequency analysis of DAV pulsators using TESS data Cory Daniel Schrandt Iowa State University Follow this and additional works at: https://lib.dr.iastate.edu/etd Part of the Astrophysics and Astronomy Commons Recommended Citation Schrandt, Cory Daniel, "Frequency analysis of DAV pulsators using TESS data" (2019). Graduate Theses and Dissertations. 17558. https://lib.dr.iastate.edu/etd/17558 This Thesis is brought to you for free and open access by the Iowa State University Capstones, Theses and Dissertations at Iowa State University Digital Repository. It has been accepted for inclusion in Graduate Theses and Dissertations by an authorized administrator of Iowa State University Digital Repository. For more information, please contact [email protected]. Frequency analysis of DAV pulsators using TESS data by Cory Daniel Schrandt A thesis submitted to the graduate faculty in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE Major: Astrophysics Program of Study Committee: Steven Kawaler, Major Professor Massimo Marengo Soeren Prell Dae-Young Lee The student author, whose presentation of the scholarship herein was approved by the program of study committee, is solely responsible for the content of this thesis. The Graduate College will ensure this thesis is globally accessible and will not permit alterations after a degree is conferred. Iowa State University Ames, Iowa 2019 Copyright c Cory Daniel Schrandt, 2019. All rights reserved. ii DEDICATION I would like to dedicate this thesis to my soon-to-be wife, Amanda, without whose support I would not have been able to complete this work.
    [Show full text]
  • Pulsating White Dwarfs
    EPJ Web of Conferences 152, 01011 (2017) DOI: 10.1051/ epjconf/201715201011 Wide-Field Variability Surveys: A 21st Century Perspective Pulsating white dwarfs S. O. Kepler1, and Alejandra D. Romero1, 1Departamento de Astronomia, Instituto de Física, Universidade Federal do Rio Grande do Sul, 91501-970 Porto Alegre, RS, Brazil Abstract. The Sloan Digital Sky Survey has allowed us to increase the number of known white dwarfs by a factor of five and consequently the number of known pulsating white dwarfs also by a factor of five. It has also led to the discovery of new types of variable white dwarfs, as the variable hot DQs, and the pulsating Extremely Low Mass white dwarfs. With the Kepler Mission, it has been possible to discover new phenomena, the outbursts present in a few pulsating white dwarfs. 1 Introduction White dwarf stars are the final evolutionary state of stars with initial masses up to 8.5 − 10.6 M ([1]), corresponding to 95–97 % of all stars. The fraction depends on the stellar metallicity, which affects both the Initial-Mass-Function and the Initial-to-Final-Mass Relation. For single stars, the minimum mass of a present day white dwarf is around 0.30 − 0.45 M ([2]), because progenitors that would become lower mass white dwarfs have main sequence evolution time larger than the age of the Universe. Such masses correspond, considering the mass-radius relation of white dwarfs, to a minimal log g 6.5. Evolutionary models e.g. by [3] indicate that the maximum surface gravity for main sequence A stars, which have similar optical spectra to DA white dwarfs, corresponds to log g ≤ 4.75, including very low metallicity.
    [Show full text]
  • White Dwarf Rotation As a Function of Mass and a Dichotomy of Mode Line Widths: Keplerobservations of 27 Pulsating DA White Dwarfs Through K2 Campaign 8
    Manuscript version: Published Version The version presented in WRAP is the published version (Version of Record). Persistent WRAP URL: http://wrap.warwick.ac.uk/112839 How to cite: The repository item page linked to above, will contain details on accessing citation guidance from the publisher. Copyright and reuse: The Warwick Research Archive Portal (WRAP) makes this work by researchers of the University of Warwick available open access under the following conditions. Copyright © and all moral rights to the version of the paper presented here belong to the individual author(s) and/or other copyright owners. To the extent reasonable and practicable the material made available in WRAP has been checked for eligibility before being made available. Copies of full items can be used for personal research or study, educational, or not-for-profit purposes without prior permission or charge. Provided that the authors, title and full bibliographic details are credited, a hyperlink and/or URL is given for the original metadata page and the content is not changed in any way. Publisher’s statement: Please refer to the repository item page, publisher’s statement section, for further information. For more information, please contact the WRAP Team at: [email protected] warwick.ac.uk/lib-publications The Astrophysical Journal Supplement Series, 232:23 (28pp), 2017 October https://doi.org/10.3847/1538-4365/aa8bb5 © 2017. The American Astronomical Society. All rights reserved. White Dwarf Rotation as a Function of Mass and a Dichotomy of Mode Line Widths: KeplerObservations of 27 Pulsating DA White Dwarfs through K2 Campaign 8 J. J.
    [Show full text]