The Science of Exoplanets and Their Systems
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Ann Merchant Boesgaard Publications Merchant, A. E., Bodenheimer, P., and Wallerstein, G
Ann Merchant Boesgaard Publications Merchant, A. E., Bodenheimer, P., and Wallerstein, G. (1965). “The Lithium Isotope Ratio in Two Hyades F Stars.” Ap. J., 142, 790. Merchant, A. E. (1966). “Beryllium in F- and G-Type Dwarfs.” Ap. J., 143, 336. Hodge, P. W., and Merchant, A. E. (1966). “Photometry of SO Galaxies II. The Peculiar Galaxy NGC 128.” Ap. J., 144, 875. Merchant, A. E. (1967). “The Abundance of Lithium in Early M-Type Stars.” Ap. J., 147, 587. Merchant, A. E. (1967). “Measured Equivalent Widths in Early M-Type Stars.” Lick Obs. Bull. No. 595 (Univ. of California Press). Boesgaard, A. M. (1968). “Isotopes of Magnesium in Stellar Atmosphere.” Ap. J., 154, 185. Boesgaard, A. M. (1968). “Observations of Beryllium in Stars.” Highlights of Astron- omy, ed. L. Perek (Dordrecht: D. Reidel), p. 237. Boesgaard, A. M. (1969). “Intensity Variation in Ca Emission in an MS Star.” Pub. A. S. P., 81, 283. Boesgaard, A. M. (1969). “Observational Clues to the Evolution of M Giant Stars.” Pub. A. S. P., 81, 365. Boesgaard, A. M. (1970). “The Lithium Isotope Ratio in δ Sagittae.” Ap. J., 159, 727. Boesgaard, A. M. (1970). “The Ratio of Titanium to Zirconium in Late-Type Stars.” Ap. J., 161, 163. Boesgaard, A. M. (1970). “On the Lithium Content in Late-Type Giants.” Ap. Letters, 5, 145. Boesgaard, A. M. (1970). “Lithium in Heavy-Metal Red Giants.” Ap. J., 161, 1003. Boesgaard, A. M. (1971). “The Lithium Content of Capella.” Ap. J., 167, 511. Boesgaard, A. M. (1973). “Iron Emission Lines in a Orionis.” In Stellar Chromospheres, eds. -
Urania Nr 3/2005
> /2005 (717) urania 3/tom LXXVI maj—czerwiec mhćirn iVlich jp f f l owiek, który świat nauczył rnier> życe(?) wokóf planetoid Fotome anzytów za pomocą rnaiych Europejskie Obserwatorium Południowe leskopami pomocniczymi (AT) o średnicy a dalej ogromne budynki mieszczące wiel (ESO) zbudowało w latach 1988-2002, na 1,8 m, które mogą zajmować 30 różnych kie teleskopy i 2 kopuły teleskopów pomoc ściętym wierzchołku góry Cerro Paranal pozycji, będą stanowiły ciągle rozbudowy niczych (obecnie są 2 AT, będzie ich 8). (2635 m n.p.m.) na pustyni Atacama w Chi wany instrument interferometryczny (VLTI) Na górnym zdjęciu widzimy teleskop „z gó le, Bardzo Duży Teleskop (VLT). Składa o bazie sięgającej przeszło 200 m, które ry" wraz z okolicznym krajobrazem, toro się on z czterech teleskopów o średnicy go rozdzielczość (0,001 sekundy łuku) bę wiskami teleskopów AT i drogami kanałów 8,2 m, mogących kierować zebrane świa dzie tak wielka, że można by widzieć nim optycznych prowadzących zebrane świa tło do wspólnego ogniska. Razem zbierają astronautę na Księżycu. Dolne zdjęcie tło do wspólnego ogniska interferometru one tyle światła, ile zbierałby teleskop przedstawia ogólny, obecny (2005 r.) wi oznaczonego gwiazdką. Idea i zasady o średnicy 16 m, a pracując w systemie dok tego obserwatorium. Na pierwszym działania tego instrumentu wywodzą się interferometrycznym, stanowią teleskop planie widzimy torowisko i stanowiska ob z odkryć i prac Alberta Michelsona. o średnicy prawie 130 m. Wspomagane te serwacyjne dla teleskopów pomocniczych, Zdjęcia ESO U R A N IA - POSTtPY ASTRONOMII 3/2005 Szanowni i Drodzy Czytelnicy, Interferometria, jako technika badawcza, zdobywa coraz szersze pola zastosowań w astronomii. -
The Tierras Observatory: an Ultra-Precise Photometer to Characterize Nearby Terrestrial Exoplanets
The Tierras Observatory: An ultra-precise photometer to characterize nearby terrestrial exoplanets Juliana Garc´ıa-Mej´ıaa, David Charbonneaua, Daniel Fabricanta, Jonathan M. Irwina, Robert Fataa, Joseph M. Zajaca, and Peter E. Dohertya aCenter for Astrophysics Harvard and Smithsonian, 60 Garden Street, Cambridge MA j ABSTRACT We report on the status of the Tierras Observatory, a refurbished 1.3-m ultra-precise fully-automated photometer located at the F. L. Whipple Observatory atop Mt. Hopkins, Arizona. Tierras is designed to limit systematic errors, notably precipitable water vapor (PWV), to 250 ppm, enabling the characterization of terrestrial planet transits orbiting < 0:3 R stars, as well as the potential discovery of exo-moons and exo-rings. The design choices that will enable our science goals include: a four-lens focal reducer and field-flattener to increase the field-of-view of the telescope from a 11:940 to a 0:48◦ side; a custom narrow bandpass (40:2 nm FWHM) filter centered around 863:5 nm to minimize PWV errors known to limit ground-based photometry of red dwarfs; and a deep-depletion 4K 4K CCD with a 300ke- full well and QE> 85% in our bandpass, operating in frame transfer mode. We are also× pursuing the design of a set of baffles to minimize the significant amount of scattered light reaching the image plane. Tierras will begin science operations in early 2021. Keywords: ultra-precise photometry, terrestrial planet detection, exoplanet instrumentation, transit method 1. INTRODUCTION The construction of observatories tailor-built to routinely achieve precise photometry from the ground is mo- tivated by the multitude of exoplanetary and stellar phenomena whose exploration will be enabled with high- cadence, ultra-precise time series of diverse stellar targets. -
The Ubvri and Infrared Colour Indices of the Sun and Sun-Like Stars
The 19th Cambridge Workshop on Cool Stars, Stellar Systems, and the Sun Edited by G. A. Feiden THE UBVRI AND INFRARED COLOUR INDICES OF THE SUN AND SUN-LIKE STARS Mehmet TANRIVER1, Ferhat Fikri ÖZEREN1 1 Erciyes University, Astronomy and Space Sciences Department, 38039, Kayseri, Turkey Abstract The Sun is not a point source, the photometric observational techniques that are utilised for observing other stars cannot be utilised for the Sun, meaning that it is dicult to derive its colours accurately for astronomical work from direct measurements in dierent passbands. The solar twins are the best choices because they are the stars that are ideally the same as the Sun in all parameters, and also, their colours are highly similar to those of the Sun. From the 60 articles on the Sun and Sun-like stars in the literature from 1964 until today, the solar colour indices in the optic and infrared regions have been estimated. 1 INTRODUCTION Table 1: The obtained average colour indices values of the The Sun is an average-low-mass star in the main sequence Sun with standart deviation (±σ)( Tanrıver (2012), Tanrıver of the Hertzsprung-Russell diagram. Moreover, the Sun is (2014a), Tanrıver (2014b) ). not a point source, the photometric observational techniques that are utilised for observing other stars cannot be utilised B-V 0.6457 ± 0.0421 V-J 1.1413 ± 0.1063 for the Sun. Therefore, the colours and colour indices of the H-K 0.0572 ± 0.0351 U-B 0.1463 ± 0.0596 sun-like stars are used in order to determine the sun’s colour V-H 1.4613 ± 0.1183 J-K 0.3777 ± 0.0494 indices. -
Naming the Extrasolar Planets
Naming the extrasolar planets W. Lyra Max Planck Institute for Astronomy, K¨onigstuhl 17, 69177, Heidelberg, Germany [email protected] Abstract and OGLE-TR-182 b, which does not help educators convey the message that these planets are quite similar to Jupiter. Extrasolar planets are not named and are referred to only In stark contrast, the sentence“planet Apollo is a gas giant by their assigned scientific designation. The reason given like Jupiter” is heavily - yet invisibly - coated with Coper- by the IAU to not name the planets is that it is consid- nicanism. ered impractical as planets are expected to be common. I One reason given by the IAU for not considering naming advance some reasons as to why this logic is flawed, and sug- the extrasolar planets is that it is a task deemed impractical. gest names for the 403 extrasolar planet candidates known One source is quoted as having said “if planets are found to as of Oct 2009. The names follow a scheme of association occur very frequently in the Universe, a system of individual with the constellation that the host star pertains to, and names for planets might well rapidly be found equally im- therefore are mostly drawn from Roman-Greek mythology. practicable as it is for stars, as planet discoveries progress.” Other mythologies may also be used given that a suitable 1. This leads to a second argument. It is indeed impractical association is established. to name all stars. But some stars are named nonetheless. In fact, all other classes of astronomical bodies are named. -
Magnetism, Dynamo Action and the Solar-Stellar Connection
Living Rev. Sol. Phys. (2017) 14:4 DOI 10.1007/s41116-017-0007-8 REVIEW ARTICLE Magnetism, dynamo action and the solar-stellar connection Allan Sacha Brun1 · Matthew K. Browning2 Received: 23 August 2016 / Accepted: 28 July 2017 © The Author(s) 2017. This article is an open access publication Abstract The Sun and other stars are magnetic: magnetism pervades their interiors and affects their evolution in a variety of ways. In the Sun, both the fields themselves and their influence on other phenomena can be uncovered in exquisite detail, but these observations sample only a moment in a single star’s life. By turning to observa- tions of other stars, and to theory and simulation, we may infer other aspects of the magnetism—e.g., its dependence on stellar age, mass, or rotation rate—that would be invisible from close study of the Sun alone. Here, we review observations and theory of magnetism in the Sun and other stars, with a partial focus on the “Solar-stellar connec- tion”: i.e., ways in which studies of other stars have influenced our understanding of the Sun and vice versa. We briefly review techniques by which magnetic fields can be measured (or their presence otherwise inferred) in stars, and then highlight some key observational findings uncovered by such measurements, focusing (in many cases) on those that offer particularly direct constraints on theories of how the fields are built and maintained. We turn then to a discussion of how the fields arise in different objects: first, we summarize some essential elements of convection and dynamo theory, includ- ing a very brief discussion of mean-field theory and related concepts. -
Habitability on Local, Galactic and Cosmological Scales
Habitability on local, Galactic and cosmological scales Luigi Secco1 • Marco Fecchio1 • Francesco Marzari1 Abstract The aim of this paper is to underline con- detectable studying our site. The Climatic Astronom- ditions necessary for the emergence and development ical Theory is introduced in sect.5 in order to define of life. They are placed at local planetary scale, at the circumsolar habitable zone (HZ) (sect.6) while the Galactic scale and within the cosmological evolution, translation from Solar to extra-Solar systems leads to a as pointed out by the Anthropic Cosmological Princi- generalized circumstellar habitable zone (CHZ) defined ple. We will consider the circumstellar habitable zone in sect.7 with some exemplifications to the Gliese-667C (CHZ) for planetary systems and a Galactic Habitable and the TRAPPIST-1 systems; some general remarks Zone (GHZ) including also a set of strong cosmologi- follow (sect.8). A first conclusion related to CHZ is cal constraints to allow life (cosmological habitability done moving toward GHZ and COSH (sect.9). The (COSH)). Some requirements are specific of a single conditions for the development of life are indeed only scale and its related physical phenomena, while others partially connected to the local scale in which a planet are due to the conspired effects occurring at more than is located. A strong interplay between different scales one scale. The scenario emerging from this analysis is exists and each single contribution to life from individ- that all the habitability conditions here detailed must ual scales is difficult to be isolated. However we will at least be met. -
HOW to CONSTRAIN YOUR M DWARF: MEASURING EFFECTIVE TEMPERATURE, BOLOMETRIC LUMINOSITY, MASS, and RADIUS Andrew W
The Astrophysical Journal, 804:64 (38pp), 2015 May 1 doi:10.1088/0004-637X/804/1/64 © 2015. The American Astronomical Society. All rights reserved. HOW TO CONSTRAIN YOUR M DWARF: MEASURING EFFECTIVE TEMPERATURE, BOLOMETRIC LUMINOSITY, MASS, AND RADIUS Andrew W. Mann1,2,8,9, Gregory A. Feiden3, Eric Gaidos4,5,10, Tabetha Boyajian6, and Kaspar von Braun7 1 University of Texas at Austin, USA; [email protected] 2 Institute for Astrophysical Research, Boston University, USA 3 Department of Physics and Astronomy, Uppsala University, Box 516, SE-751 20, Uppsala, Sweden 4 Department of Geology and Geophysics, University of Hawaii at Manoa, Honolulu, HI 96822, USA 5 Max Planck Institut für Astronomie, Heidelberg, Germany 6 Department of Astronomy, Yale University, New Haven, CT 06511, USA 7 Lowell Observatory, 1400 W. Mars Hill Rd., Flagstaff, AZ, USA Received 2015 January 6; accepted 2015 February 26; published 2015 May 4 ABSTRACT Precise and accurate parameters for late-type (late K and M) dwarf stars are important for characterization of any orbiting planets, but such determinations have been hampered by these stars’ complex spectra and dissimilarity to the Sun. We exploit an empirically calibrated method to estimate spectroscopic effective temperature (Teff) and the Stefan–Boltzmann law to determine radii of 183 nearby K7–M7 single stars with a precision of 2%–5%. Our improved stellar parameters enable us to develop model-independent relations between Teff or absolute magnitude and radius, as well as between color and Teff. The derived Teff–radius relation depends strongly on [Fe/H],as predicted by theory. -
A Detailed Analysis of the Hd 73526 2:1 Resonant Planetary System∗
The Astrophysical Journal, 780:140 (9pp), 2014 January 10 doi:10.1088/0004-637X/780/2/140 C 2014. The American Astronomical Society. All rights reserved. Printed in the U.S.A. A DETAILED ANALYSIS OF THE HD 73526 2:1 RESONANT PLANETARY SYSTEM∗ Robert A. Wittenmyer1,2,XianyuTan3,4, Man Hoi Lee3,5, Jonathan Horner1,2,C.G.Tinney1,2, R. P. Butler6, G. S. Salter1,2, B. D. Carter7,H.R.A.Jones8, S. J. O’Toole9, J. Bailey1,2, D. Wright1,2,J.D.Crane10, S. A. Schectman10, P. Arriagada6, I. Thompson10, D. Minniti11,12,andM.Diaz11 1 School of Physics, University of New South Wales, Sydney 2052, Australia; [email protected] 2 Australian Centre for Astrobiology, University of New South Wales, Sydney 2052, Australia 3 Department of Earth Sciences, The University of Hong Kong, Pokfulam Road, Hong Kong 4 Department of Planetary Sciences and Lunar and Planetary Laboratory, The University of Arizona, 1629 University Boulevard, Tucson, AZ 85721, USA 5 Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong 6 Department of Terrestrial Magnetism, Carnegie Institution of Washington, 5241 Broad Branch Road, NW, Washington, DC 20015-1305, USA 7 Faculty of Sciences, University of Southern Queensland, Toowoomba, Queensland 4350, Australia 8 University of Hertfordshire, Centre for Astrophysics Research, Science and Technology Research Institute, College Lane, AL10 9AB, Hatfield, UK 9 Australian Astronomical Observatory, PO Box 915, North Ryde, NSW 1670, Australia 10 The Observatories of the Carnegie Institution of Washington, 813 Santa Barbara Street, Pasadena, CA 91101, USA 11 Institute of Astrophysics, Pontificia Universidad Catolica de Chile, Casilla 306, Santiago 22, Chile 12 Vatican Observatory, V00120 Vatican City State, Italy Received 2013 August 14; accepted 2013 November 26; published 2013 December 18 ABSTRACT We present six years of new radial velocity data from the Anglo-Australian and Magellan Telescopes on the HD 73526 2:1 resonant planetary system. -
A Basic Requirement for Studying the Heavens Is Determining Where In
Abasic requirement for studying the heavens is determining where in the sky things are. To specify sky positions, astronomers have developed several coordinate systems. Each uses a coordinate grid projected on to the celestial sphere, in analogy to the geographic coordinate system used on the surface of the Earth. The coordinate systems differ only in their choice of the fundamental plane, which divides the sky into two equal hemispheres along a great circle (the fundamental plane of the geographic system is the Earth's equator) . Each coordinate system is named for its choice of fundamental plane. The equatorial coordinate system is probably the most widely used celestial coordinate system. It is also the one most closely related to the geographic coordinate system, because they use the same fun damental plane and the same poles. The projection of the Earth's equator onto the celestial sphere is called the celestial equator. Similarly, projecting the geographic poles on to the celest ial sphere defines the north and south celestial poles. However, there is an important difference between the equatorial and geographic coordinate systems: the geographic system is fixed to the Earth; it rotates as the Earth does . The equatorial system is fixed to the stars, so it appears to rotate across the sky with the stars, but of course it's really the Earth rotating under the fixed sky. The latitudinal (latitude-like) angle of the equatorial system is called declination (Dec for short) . It measures the angle of an object above or below the celestial equator. The longitud inal angle is called the right ascension (RA for short). -
Publications Ofthe Astronomical Society Ofthe Pacific 99:490-496, June 1987
Publications ofthe Astronomical Society ofthe Pacific 99:490-496, June 1987 RADIAL VELOCITIES OF M DWARF STARS GEOFFREY W. MARCY,* VICTORIA LINDSAY,* AND KAREN WILSON Department of Physics and Astronomy, San Francisco State University, San Francisco, California 94132 Received 1987 February 26, revised 1987 March 28 ABSTRACT Radial velocities for 72 M dwarfs have been obtained having internal errors of about 0.1 km s1 and external errors of about 0.4 km s_1. Multiple velocity measurements of ten dMe stars have yielded a set of six which have no stellar companions, providing confirmation that the dMe phenomenon can occur in single stars. These single dMe stars have low space motions indicative of relative youth. Four stars from the entire survey were found to have double-line spectra and two were found to be single-line spectroscopic binaries of low amplitude. The zero point of the velocity scale is found to agree well with that of O. C. Wilson (1967) and differences are noted among other radial-velocity studies. Most of the stars in this study have velocities sufficiently well determined to constitute potential radial-velocity standards. Key words: K-M dwarfs-radial velocities I. Introduction atic difference between their velocities and O. C. 1 Accurate measurements of radial velocities for M Wilson's of —1.7 km s , a discrepancy not explainable by dwarfs are used to address a number of astrophysical the random errors of the two studies. problems such as the age dependence of the kinematics of Thus, it is not known at present which zero point is to the Galaxy (cf. -
Stars and Telescopes : a Resource Book for Teachers of Lower School Science
Edith Cowan University Research Online ECU Publications Pre. 2011 1981 Stars and telescopes : a resource book for teachers of lower school science Clifton L. Smith Follow this and additional works at: https://ro.ecu.edu.au/ecuworks Part of the Science and Mathematics Education Commons Smith, C. (1981). Stars and telescopes : a resource book for teachers of lower school science. Nedlands, Australia: Nedlands College of Advanced Education. This Book is posted at Research Online. https://ro.ecu.edu.au/ecuworks/7034 Edith Cowan University Copyright Warning You may print or download ONE copy of this document for the purpose of your own research or study. The University does not authorize you to copy, communicate or otherwise make available electronically to any other person any copyright material contained on this site. You are reminded of the following: Copyright owners are entitled to take legal action against persons who infringe their copyright. A reproduction of material that is protected by copyright may be a copyright infringement. Where the reproduction of such material is done without attribution of authorship, with false attribution of authorship or the authorship is treated in a derogatory manner, this may be a breach of the author’s moral rights contained in Part IX of the Copyright Act 1968 (Cth). Courts have the power to impose a wide range of civil and criminal sanctions for infringement of copyright, infringement of moral rights and other offences under the Copyright Act 1968 (Cth). Higher penalties may apply, and higher damages may be awarded, for offences and infringements involving the conversion of material into digital or electronic form.