Radial Velocity Variations in Red Giant Stars: Pulsations, Spots and Planets
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Precise Radial Velocities of Giant Stars. III. Spectroscopic Stellar Parameters
Astronomy & Astrophysics manuscript no. finalversionlcor6nov1 c ESO 2018 October 28, 2018 Precise radial velocities of giant stars. III.⋆ Spectroscopic stellar parameters S. Hekker1 and J. Mel´endez2 1 Leiden Observatory, Leiden University, P.O. Box 9513, 2300 RA Leiden, The Netherlands 2 Research School of Astronomy & Astrophysics, Mount Stromlo Observatory, Cotter Road, Weston Creek, ACT 2611, Australia Received ¡date¿; accepted ¡date¿ ABSTRACT Context. A radial velocity survey of about 380 G and K giant stars is ongoing at Lick observatory. For each star we have a high signal to noise ratio template spectrum, which we use to determine spectroscopic stellar parameters. Aims. The aim of this paper is to present spectroscopic stellar parameters, i.e. effective temperature, surface gravity, metallicity and rotational velocity for our sample of G and K giant stars. Methods. Effective temperatures, surface gravities and metallicities are determined from the equivalent width of iron lines, by imposing exci- tation and ionisation equilibrium through stellar atmosphere models. Rotational velocities are determined from the full width at half maximum (FWHM) of moderate spectral lines. A calibration between the FWHM and total broadening (rotational velocity and macro turbulence) is ob- tained from stars in common between our sample and the sample from Gray (1989). Macro turbulence is determined from the macro turbulence vs. spectral type relations from Gray (2005). Results. The metallicity we derive is essentially equal to the literature values, while the effective temperature and surface gravity are slightly higher by 56 K and 0.15 dex, respectively. A method comparison is performed with 72 giants in common with Luck and Heiter (2007), which shows that both methods give similar results. -
Basics of Astrophysics Revisited. I. Mass- Luminosity Relation for K, M and G Class Stars
Basics of astrophysics revisited. I. Mass- luminosity relation for K, M and G class stars Edgars Alksnis [email protected] Small volume statistics show, that luminosity of slow rotating stars is proportional to their angular momentums of rotation. Cause should be outside of standard solar model. Slow rotating giants and dim dwarfs are not out of „main sequence” in this concept. Predictive power of stellar mass-radius- equatorial rotation speed-luminosity relation has been offered to test in numerous examples. Keywords: mass-luminosity relation, stellar rotation, stellar mass prediction, stellar rotation prediction ...Such vibrations would proceed from deep inside the sun. They are a fast way of transporting large amounts of energy from the interior to the surface that is not envisioned in present theory.... They could stir up the material inside the sun, which current theory tends to see as well layered, and that could affect the fusion dynamics. If they come to be generally accepted, they will require a reworking of solar theory, and that carries in its train a reworking of stellar theory generally. These vibrations could reverberate throughout astronomy. (Science News, Vol. 115, April 21, 1979, p. 270). Actual expression for stellar mass-luminosity relation (fig.1) Fig.1 Stellar mass- luminosity relation. Credit: Ay20. L- luminosity, relative to the Sun, M- mass, relative to the Sun. remain empiric and in fact contain unresolvable contradiction: stellar luminosity basically is connected with their surface area (radius squared) but mass (radius in cube) appears as a factor which generate luminosity. That purely geometric difference had pressed astrophysicists to place several classes of stars outside of „main sequence” in the frame of their strange theoretic constructions. -
Exploring Milky Way Halo Substructures with Large-Area Sky Surveys
EXPLORING MILKY WAY HALO SUBSTRUCTURES WITH LARGE-AREA SKY SURVEYS A Dissertation by TING LI Submitted to the Office of Graduate and Professional Studies of Texas A&M University in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY Chair of Committee, Darren L. DePoy Co-Chair of Committee, Jennifer L. Marshall Committee Members, Nicholas B. Suntzeff Casey J. Papovich Sherry J. Yennello Head of Department, George R. Welch August 2016 Major Subject: Physics Copyright 2016 Ting Li ABSTRACT Over the last two decades, our understanding of the Milky Way has been improved thanks to large data sets arising from large-area digital sky surveys. The stellar halo is now known to be inhabited by a variety of spatial and kinematic stellar substructures, including stellar streams and stellar clouds, all of which are predicted by hierarchical Lambda Cold Dark Matter models of galaxy formation. In this dissertation, we first present the analysis of spectroscopic observations of individual stars from the two candidate structures discovered using an M-giant catalog from the Two Micron All-Sky Survey. The follow-up observations show that one of the candidates is a genuine structure which might be associated with the Galactic Anticenter Stellar Structure, while the other one is a false detection due to the systematic photometric errors in the survey or dust extinction in low Galactic latitudes. We then presented the discovery of an excess of main sequence turn-off stars in the direction of the constellations of Eridanus and Phoenix from the first-year data of the Dark Energy Survey (DES) { a five-year, 5,000 deg2 optical imaging survey in the Southern Hemisphere. -
Observed Stellar Spectra As Templates for Gaia
Universit`adegli Studi di Padova DIPARTIMENTO DI ASTRONOMIA Dottorato di Ricerca in Astronomia XXIII ciclo Observed Stellar Spectra As Templates For Gaia Coordinatore: Prof. Giampaolo Piotto Supervisori: Prof. Antonella Vallenari Prof. Ulisse Munari Dottoranda: Tenay Saguner 2 31 Gennaio 2011 To My Family & To Prof. I. Ethem Derman Contents Index i Figures List x Tables List x 1 Introduction 1 2 The Gaia Mission 3 2.1 OverviewOfTheGaiaMission . 5 2.1.1 MeasurementPrinciples . 5 2.1.2 ObservationPrinciple . 7 2.1.3 Instruments And Performances . 7 2.1.4 TheAccuracyOfGaiaMeasurements . 10 2.2 The Classification of Gaia objects . ..... 15 2.3 TheFinalCatalogue ............................... 16 2.4 TheImportanceoftrainingdata . 16 3 The Red Clump Stars 19 3.1 The Structure And The Evolution Of the Red Clump . 19 3.2 RedClumpStarsInTheLiterature. 21 4 Target Selection and The Input Catalog 23 4.1 TargetSelectionCriteria. 23 i ii 5 Observations And Data Reduction 27 5.1 The B&C Spectrograph At The 1.22 meter TelescopeInAsiago ............................... 27 5.2 Softwares To Use The 1.22 meter Telescope . ..... 29 5.3 DataAcquisitionAtTheTelescope . 29 5.4 Selecting The Wavelength Interval To Observe . ....... 31 5.5 DataReduction.................................. 35 5.5.1 WavelengthCalibration . 38 5.5.2 ContinuumNormalization . 38 5.5.3 HeliocentricCorrection . 41 6 Measuring Radial Velocities 45 6.1 Cross-CorrelationTechnique. 45 6.2 Accuracy Tests With IAU Radial Velocity Standards . ........ 48 6.3 ExtendedTestsOnRadialVelocities . ..... 52 7 Atmospheric Parameter Determonation 55 7.1 χ2 Technique ................................... 55 7.1.1 TheSyntheticspectralLibrary . 56 7.1.2 The χ2 Methods ............................. 58 7.2 Accuracy Tests With Red Clump Stars In the Literature . -
Nexstar 8 & 11 GPS Star List
Double SAO # RA (hr) RA (min) Dec Deg Dec Amin Mag Const Sep HD 225020 2 0 2.8 80 16.9 7.7,9.9 Cep Sep AB:16 HD 5679 U Cep 168 1 2.3 81 52.5 6.9,11.2,12.9 Cep Sep AB:14, Sep AC:21 HD 7471 218 1 19.1 80 51.7 7.2,8 Cep Sep AB:130 HD 8890 Alpha UMi; 1 UMi; Polaris 308 2 31.6 89 15.9 2,9,13,12 UMi Sep AB:18, Sep AC:45, Sep AD:83 HD 105943 OS 117 1991 12 11.0 81 42.6 6,8.3 Cam Sep AB:67 HD 106798 2009 12 16.2 80 7.5 7.2,7.8 Cam Sep AB:14 HD 112028 2102 12 49.2 83 24.8 5.4,5.9 Cam Sep AB:22 HD 112651 2112 12 54.2 82 31.1 7.1,10.5 Cam Sep AB:10 HD 131616 2433 14 33.3 85 56.3 7.1,10.1 UMi Sep AB:3 HD 139777 Pi 1 Umi 2556 15 29.3 80 26.8 6.6,7.3,11 UMi Sep AB:31, Sep AC:154 HD 153751 Epsilon UMi 2770 16 46.0 82 2.2 4.2,11.2 UMi Sep AB:77 HD 166926 24 Umi 2940 17 30.7 86 58.1 8.5,9 UMi Sep AB:31 HD 184146 3209 19 15.1 83 27.8 6.5,10.6 Dra Sep AB:6 HD 196787 3408 20 28.2 81 25.4 5.6,11.1,6.9 Dra Sep AB:110, Sep AC:198 HD 196925 3413 20 29.4 81 5.3 6.1,9.3 Dra Sep AB:214 HD 209942 3673 21 58.3 82 52.2 6.9,7.5 Cep Sep AB:14 HD 919 4062 0 14.0 76 1.6 7.2,7.7 Cep Sep AB:76 HD 3366 4165 0 37.8 72 53.7 7,12.7 Cas Sep AB:32 HD 3553 4176 0 40.0 76 52.3 6.7,8.6 Cas Sep AB:116 HD 4161 H N 122; YZ Cas 4216 0 45.6 74 59.3 5.7,9.4 Cas Sep AB:36 HD 7406 4360 1 16.6 74 1.6 7.1,7.9 Cas Sep AB:61 HD 9774 40 Cas 4453 1 38.5 73 2.4 5.3,11.3 Cas Sep AB:53 HD 11316 4512 1 55.4 76 13.5 7.4,8.4 Cas Sep AB:3 HD 12013 4550 2 2.1 75 30.1 6.3,8.2,8.8 Cas Sep AB:1.3, Sep AC:117 HD 12111 48 Cas 4554 2 2.0 70 54.4 4.6,12.6 Cas Sep AB:51 HD 12173 4559 2 3.2 73 51.0 6.1,8.6 Cas -