Gaia Data Release 2 Special Issue
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The Agb Newsletter
THE AGB NEWSLETTER An electronic publication dedicated to Asymptotic Giant Branch stars and related phenomena Official publication of the IAU Working Group on Red Giants and Supergiants No. 276 — 1 July 2020 https://www.astro.keele.ac.uk/AGBnews Editors: Jacco van Loon, Ambra Nanni and Albert Zijlstra Editorial Board (Working Group Organising Committee): Marcelo Miguel Miller Bertolami, Carolyn Doherty, JJ Eldridge, Anibal Garc´ıa-Hern´andez, Josef Hron, Biwei Jiang, Tomasz Kami´nski, John Lattanzio, Emily Levesque, Maria Lugaro, Keiichi Ohnaka, Gioia Rau, Jacco van Loon (Chair) Figure 1: The Cat’s Eye Planetary Nebula imaged by Mark Hanson at Stan Watson Observatory with a 24′′ f6.7 teelescope. It includes 23 hours worth of [O iii]. The best known part, the “eye” is just the small object in the middle, while the messy halo extends much further. Notice also the bowshock on the right. (Suggestion by Sakib Rasool.) 1 Editorial Dear Colleagues, It is a pleasure to present you the 276th issue of the AGB Newsletter. Note that IAU Symposium 366 (”The Origin of Outflows in Evolved Stars”) has been postponed until November next year, while in June 2021 there will be a 4-week programme of workshops on stellar astrophysics in the Gaia era, in Munich (Germany). See the announcements for both meetings at the end of the newsletter. Unfortunately our proposal for a Focus Meeting at next year’s IAU General Assembly was not successful. One of the reasons given was: ”Some evaluators commented that Most of the topics in this proposal could have been made 10 or 20 years ago. -
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. -
Detecting Reflected Light from Close-In Extrasolar Giant Planets with the Kepler Photometer
Accepted for publication by the Astrophysical Journal 05/2003 Detecting Reflected Light from Close-In Extrasolar Giant Planets with the Kepler Photometer Jon M. Jenkins SETI Institute/NASA Ames Research Center, MS 244-30, Moffett Field, CA 94035 [email protected] and Laurance R. Doyle SETI Institute, 2035 Landings Drive, Mountain View, CA 94043 [email protected] ABSTRACT NASA’s Kepler Mission promises to detect transiting Earth-sized planets in the habitable zones of solar-like stars. In addition, it will be poised to detect the reflected light component from close-in extrasolar giant planets (CEGPs) similar to 51 Peg b. Here we use the DIARAD/SOHO time series along with models for the reflected light signatures of CEGPs to evaluate Kepler’s ability to detect arXiv:astro-ph/0305473v1 24 May 2003 such planets. We examine the detectability as a function of stellar brightness, stellar rotation period, planetary orbital inclination angle, and planetary orbital period, and then estimate the total number of CEGPs that Kepler will detect over its four year mission. The analysis shows that intrinsic stellar variability of solar-like stars is a major obstacle to detecting the reflected light from CEGPs. Monte Carlo trials are used to estimate the detection threshold required to limit the total number of expected false alarms to no more than one for a survey of 100,000 stellar light curves. Kepler will likely detect 100-760 51 Peg b-like planets by reflected light with orbital periods up to 7 days. Subject headings: planetary systems — techniques: photometry — methods: data analysis –2– 1. -
THE VALLEY SKYWATCHER Volume 47 Number 3 Summer 2010
THE VALLEY SKYWATCHER Volume 47 Number 3 Summer 2010 The Valley Skywatcher is the official publication of the Chagrin Valley Astronomical Society, founded 1963. Our mailing address is PO Box 11, Chagrin Falls, OH 44022 More information can be found on our web site: www.chagrinvalleyastronomy.org Editor: Dan Rothstein Table of Contents: A Few Summer Double Stars George Gliba Constellation Quiz Dan Rothstein Discovery History and Recent Light Curves for 1700 Zvezdara Ron Baker Astronomical Alignments in Ireland Dan Rothstein A Few Summer Double Stars - by G.W. Gliba There are many fine double stars available in the Summer sky that can be split in a small refractor or medium size reflector this time of the year. One of my favorite is Xi Bootids, because it was originally thought to be the radiant to a solo minor meteorite shower, which is now known to be a complex of several radiants, now recognized by the IAU as the Bootid-Corona Borealis Complex. It can be split with a good 2.4-inch refractor. The components consists of a 4.8 magnitude primary star that is a G8V with a 7th magnitude companion of K5V spec. type, which appears yellow and orange respectively to an observer. This star system is 22 light years distant. The G8V component is also a variable star of low amplitude know as a BY Draconis type star, which varies from 4.52 to 4.67 over 10.137 days. However, this variability can't be noticed visually. Much easier and more colorful is the nice pair Epsilon Bootis nearby, also known as Izar. -
Flares on Active M-Type Stars Observed with XMM-Newton and Chandra
Flares on active M-type stars observed with XMM-Newton and Chandra Urmila Mitra Kraev Mullard Space Science Laboratory Department of Space and Climate Physics University College London A thesis submitted to the University of London for the degree of Doctor of Philosophy I, Urmila Mitra Kraev, confirm that the work presented in this thesis is my own. Where information has been derived from other sources, I confirm that this has been indicated in the thesis. Abstract M-type red dwarfs are among the most active stars. Their light curves display random variability of rapid increase and gradual decrease in emission. It is believed that these large energy events, or flares, are the manifestation of the permanently reforming magnetic field of the stellar atmosphere. Stellar coronal flares are observed in the radio, optical, ultraviolet and X-rays. With the new generation of X-ray telescopes, XMM-Newton and Chandra , it has become possible to study these flares in much greater detail than ever before. This thesis focuses on three core issues about flares: (i) how their X-ray emission is correlated with the ultraviolet, (ii) using an oscillation to determine the loop length and the magnetic field strength of a particular flare, and (iii) investigating the change of density sensitive lines during flares using high-resolution X-ray spectra. (i) It is known that flare emission in different wavebands often correlate in time. However, here is the first time where data is presented which shows a correlation between emission from two different wavebands (soft X-rays and ultraviolet) over various sized flares and from five stars, which supports that the flare process is governed by common physical parameters scaling over a large range. -
5. Cosmic Distance Ladder Ii: Standard Candles
5. COSMIC DISTANCE LADDER II: STANDARD CANDLES EQUIPMENT Computer with internet connection GOALS In this lab, you will learn: 1. How to use RR Lyrae variable stars to measures distances to objects within the Milky Way galaxy. 2. How to use Cepheid variable stars to measure distances to nearby galaxies. 3. How to use Type Ia supernovae to measure distances to faraway galaxies. 1 BACKGROUND A. MAGNITUDES Astronomers use apparent magnitudes , which are often referred to simply as magnitudes, to measure brightness: The more negative the magnitude, the brighter the object. The more positive the magnitude, the fainter the object. In the following tutorial, you will learn how to measure, or photometer , uncalibrated magnitudes: http://skynet.unc.edu/ASTR101L/videos/photometry/ 2 In Afterglow, go to “File”, “Open Image(s)”, “Sample Images”, “Astro 101 Lab”, “Lab 5 – Standard Candles”, “CD-47” and open the image “CD-47 8676”. Measure the uncalibrated magnitude of star A: uncalibrated magnitude of star A: ____________________ Uncalibrated magnitudes are always off by a constant and this constant varies from image to image, depending on observing conditions among other things. To calibrate an uncalibrated magnitude, one must first measure this constant, which we do by photometering a reference star of known magnitude: uncalibrated magnitude of reference star: ____________________ 3 The known, true magnitude of the reference star is 12.01. Calculate the correction constant: correction constant = true magnitude of reference star – uncalibrated magnitude of reference star correction constant: ____________________ Finally, calibrate the uncalibrated magnitude of star A by adding the correction constant to it: calibrated magnitude = uncalibrated magnitude + correction constant calibrated magnitude of star A: ____________________ The true magnitude of star A is 13.74. -
Exoplanet Community Report
JPL Publication 09‐3 Exoplanet Community Report Edited by: P. R. Lawson, W. A. Traub and S. C. Unwin National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California March 2009 The work described in this publication was performed at a number of organizations, including the Jet Propulsion Laboratory, California Institute of Technology, under a contract with the National Aeronautics and Space Administration (NASA). Publication was provided by the Jet Propulsion Laboratory. Compiling and publication support was provided by the Jet Propulsion Laboratory, California Institute of Technology under a contract with NASA. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does not constitute or imply its endorsement by the United States Government, or the Jet Propulsion Laboratory, California Institute of Technology. © 2009. All rights reserved. The exoplanet community’s top priority is that a line of probeclass missions for exoplanets be established, leading to a flagship mission at the earliest opportunity. iii Contents 1 EXECUTIVE SUMMARY.................................................................................................................. 1 1.1 INTRODUCTION...............................................................................................................................................1 1.2 EXOPLANET FORUM 2008: THE PROCESS OF CONSENSUS BEGINS.....................................................2 -
Determining Pulsation Period for an RR Lyrae Star
Leah Fabrizio Dr. Mitchell 06/10/2010 Determining Pulsation Period for an RR Lyrae Star As children we used to sing in wonderment of the twinkling stars above and many of us asked, “Why do stars twinkle?” All stars twinkle because their emitted light travels through the Earth’s atmosphere of turbulent gas and clouds that move and shift causing the traversing light to fluctuate. This means that the actual light output of the star is not changing. However there are a number of stars called Variable Stars that actually produce light of varying brightness before it hits the Earth’s atmosphere. There are two categories of variable stars: the intrinsic, where light fluctuation is due from the star physically changing and producing different luminosities, and extrinsic, where the amount of starlight varies due to another star eclipsing or blocking the star’s light from reaching earth (AAVSO 2010). Within the category of intrinsic variable stars are the pulsating variables that have a periodic change in brightness due to the actual size and light production of the star changing; within this group are the RR Lyrae stars (“variable star” 2010). For my research project, I will observe an RR Lyrae and find the period of its luminosity pulsation. The first RR Lyrae star was named after its namesake star (Strobel 2004). It was first found while astronomers were studying the longer period variable stars Cepheids and stood out because of its short period. In comparison to Cepheids, RR Lyraes are smaller and therefore fainter with a shorter period as well as being much older. -
Searching for RR Lyrae Stars in M15
Searching for RR Lyrae Stars in M15 ARCC Scholar thesis in partial fulfillment of the requirements of the ARCC Scholar program Khalid Kayal February 1, 2013 Abstract The expansion and contraction of an RR Lyrae star provides a high level of interest to research in astronomy because of the several intrinsic properties that can be studied. We did a systematic search for RR Lyrae stars in the globular cluster M15 using the Catalina Real-time Transient Survey (CRTS). The CRTS searches for rapidly moving Near Earth Objects and stationary optical transients. We created an algorithm to create a hexagonal tiling grid to search the area around a given sky coordinate. We recover light curve plots that are produced by the CRTS and, using the Lafler-Kinman search algorithm, we determine the period, which allows us to identify RR Lyrae stars. We report the results of this search. i Glossary of Abbreviations and Symbols CRTS Catalina Real-time Transient Survey RR A type of variable star M15 Messier 15 RA Right Ascension DEC Declination RF Radio frequency GC Globular cluster H-R Hertzsprung-Russell SDSS Sloan Digital Sky Survey CCD Couple-Charged Device Photcat DB Photometry Catalog Database FAP False Alarm Probability ii Contents 1 Introduction 1 2 Background on RR Lyrae Stars 5 2.1 What are RR Lyraes? . 5 2.2 Types of RR Lyrae Stars . 6 2.3 Stellar Evolution . 8 2.4 Pulsating Mechanism . 9 3 Useful Tools and Surveys 10 3.1 Choosing M15 . 10 3.2 Catalina Real-time Transient Survey . 11 3.3 The Sloan Digital Sky Survey . -
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. -
The Coronal X-Ray – Age Relation and Its Implications for the Evaporation of Exoplanets
Mon. Not. R. Astron. Soc. 000, 1–20 (2011) Printed 24 October 2018 (MN LATEX style file v2.2) The coronal X-ray – age relation and its implications for the evaporation of exoplanets Alan P. Jackson1,2⋆, Timothy A. Davis1,3⋆ and Peter J. Wheatley4 1Sub-Department of Astrophysics, University of Oxford, Denys Wilkinson Building, Keble Road, Oxford, UK, OX1 3RH 2Institute of Astronomy, University of Cambridge, Madingley Road, Cambridge, UK, CB3 0HA 3European Southern Observatory, Karl-Schwarzschild-Str. 2, 85748, Garching bei Muenchen, Germany 4Department of Physics, University of Warwick, Gibbet Hill Road, Coventry, UK, CV4 7AL Submitted 2011 ABSTRACT We study the relationship between coronal X-ray emission and stellar age for late-type stars, and the variation of this relationship with spectral type. We select 717 stars from 13 open clusters and find that the ratio of X-ray to bolometric luminosity during the saturated phase of coronal emission decreases from 10−3.1 for late K-dwarfs to 10−4.3 for early F-type stars (across the range 0.29 6 (B − V )0 < 1.41). Our determined saturation timescales vary between 107.8 and 108.3 years, though with no clear trend across the whole FGK range. We apply our X-ray emission – age relations to the investigation of the evaporation history of 121 known transiting exoplanets using a simple energy-limited model of evaporation and taking into consideration Roche lobe effects and different heating/evaporation efficiencies. We confirm that a linear cut-off of the planet distribution in the M 2/R3 versus a−2 plane is an expected result of population modification by evaporation and show that the known transiting exoplanets display such a cut-off. -
Cepheid Variable Stars Cepheid Variable Stars As Distance Indicators
Cepheid Variable Stars Cepheid variable stars as distance indicators. Certain stars that have used up their main supply of hydrogen fuel are unstable and pulsate. RR Lyrae variables have periods of about a day. Their brightness doubles from dimest to brightest. Typical light curve for a Cepheid variable star. Cepheid variables have longer periods, from one day up to about 50 days. Their brightness also doubles from dimest to brightest. From the shape of the ``light curve'' of a Cepheid variable star, one can tell that it is a Cepheid variable. The period is simple to measure, as is the apparent brightness at maximum brightness. Cepheids as distance indicators Cepheids are important beyond their intrinsic interest as pulsating stars. Astronomomers have found that their is a relation between the period of a Cepheid and its luminosity. http://zebu.uoregon.edu/~soper/MilkyWay/cepheid.html (1 of 3) [5/25/1999 10:34:08 AM] Cepheid Variable Stars This enables astronomers to determine distances: ● Find the period. ● This gives the luminosity. ● Measure the apparent brightness. ● Determine the distance from the luminosity and brightness. The same applies to RR Lyrae variable stars. Once you know that a star is an RR Lyrae variable (eg. from the shape of its light curve), then you know its luminosity. Where did this period-luminosity relation come from? ● American astronomer Henrietta Leavitt looked at many Cepheid variables in the Small Magellanic Cloud (a satellite galaxy to ours.) ● She found the period luminosity relation (reported in 1912). ● One needs a distance measurement from some other method for at least one Cepheid.