Chemical Evolution of the Galactic Bulge As Traced by Microlensed Dwarf and Subgiant Stars: II
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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. -
Astronomy with Small Telescopes
Astronomy With Small Telescopes Bohdan Paczy´nski Princeton University Observatory, Princeton, NJ 08544 [email protected] ABSTRACT The All Sky Automated Survey (ASAS) is monitoring all sky to about 14 mag with a cadence of about 1 day; it has discovered about 105 variable stars, most of them new. The instrument used for the survey had aperture of 7 cm. A search for planetary transits has lead to the discovery of about a dozen confirmed planets, so called ’hot Jupiters’, providing the information of planetary masses and radii. Most discoveries were done with telescopes with aperture of 10 cm. We propose a search for optical transients covering all sky with a cadence of 10 - 30 minutes and the limit of 12 - 14 mag, with an instant verification of all candidate events. The search will be made with a large number of 10 cm instruments, and the verification will be done with 30 cm instruments. We also propose a system to be located at the L1 point of the Earth - Sun system to detect ’killer asteroids’. With a limiting magnitude of about 18 mag it could detect 10 m boulders several hours prior to their impact, provide warning against Tunguska-like events, as well as to provide news about spectacular but harmless more modest impacts. Subject headings: techniques: photometric — surveys — celestial mechanics — mete- oroids — stars: variable — gamma rays: bursts arXiv:astro-ph/0609161v3 7 Nov 2006 1. Introduction The goal of this paper is to point out that there are many tasks for which small and even very small telescopes are not only useful, but even indispensable. -
Cosmological Narrative in the Synagogues of Late Roman-Byzantine Palestine
COSMOLOGICAL NARRATIVE IN THE SYNAGOGUES OF LATE ROMAN-BYZANTINE PALESTINE Bradley Charles Erickson A dissertation submitted to the faculty of the University of North Carolina at Chapel Hill in partial fulfillment of the requirements for the degree of Doctor of Philosophy in the Department of Religious Studies. Chapel Hill 2020 Approved by: Jodi Magness Zlatko Plese David Lambert Jennifer Gates-Foster Maurizio Forte © 2020 Bradley Charles Erickson ALL RIGHTS RESERVED ii ABSTRACT Bradley Charles Erickson: Cosmological Narrative in the Synagogues of Late Roman-Byzantine Palestine (Under the Direction of Jodi Magness) The night sky provided ancient peoples with a visible framework through which they could view and experience the divine. Ancient astronomers looked to the night sky for practical reasons, such as the construction of calendars by which time could evenly be divided, and for prognosis, such as the foretelling of future events based on the movements of the planets and stars. While scholars have written much about the Greco-Roman understanding of the night sky, few studies exist that examine Jewish cosmological thought in relation to the appearance of the Late Roman-Byzantine synagogue Helios-zodiac cycle. This dissertation surveys the ways that ancient Jews experienced the night sky, including literature of the Second Temple (sixth century BCE – 70 CE), rabbinic and mystical writings, and Helios-zodiac cycles in synagogues of ancient Palestine. I argue that Judaism joined an evolving Greco-Roman cosmology with ancient Jewish traditions as a means of producing knowledge of the earthly and heavenly realms. iii ACKNOWLEDGEMENTS I wish to express my sincere appreciation to my adviser, Dr. -
Tracing the Outer Structure of the Sagittarius Dwarf Galaxy: Detections at Angular Distances Between 10 and 34 Degrees ∗
Tracing the Outer Structure of the Sagittarius Dwarf Galaxy: Detections at Angular Distances Between 10 and 34 Degrees ∗ Mario Mateo1 e-mail: [email protected] Edward W. Olszewski2 e-mail: [email protected] Heather L. Morrison3 e-mail: [email protected] Received ; accepted ∗BasedonobservationsobtainedwiththeBlancoTelescopeatCTIO,whichisoperated by the National Optical Astronomy Observatory, under contract to AURA. 1Department of Astronomy, University of Michigan, 821 Dennison Bldg., Ann Arbor, MI 48109–1090 2Steward Observatory, 933 N. Cherry, University of Arizona, Tucson, AZ 85721-0065 3Cottrell Scholar of Research Corporation, and NSF Career Fellow; Department of Astronomy and Department of Physics, Case Western Reserve University, Cleveland OH 44106 –2– ABSTRACT We have obtained deep photometric data in 24 fields along the southeast extension of the major axis of the Sagittarius dwarf spheroidal (Sgr dSph) galaxy, and in four fields along the northwest extension. Using star counts at the expected position of the Sgr upper main-sequence within the resulting color-magnitude diagrams (CMDs), we unambiguously detect Sgr stars in the southeast over the range 10–34◦ from the galaxy’s center. If Sgr is symmetric, this implies a true major-axis diameter of at least 68◦, or nearly 30 kpc if all portions of Sgr are equally distant from the Sun. Star counts parallel to the galaxy’s minor-axis reveal that Sgr remains quite broad far from its center. This suggests that the outer portions of Sgr resemble a stream rather than an extension of the ellipsoidal inner regions of the galaxy. The inferred V-band surface brightness (SB) profile ranges from 27.3-30.5 mag arcsec−2 over this radial range and exhibits a change in slope ∼ 20◦ from the center of Sgr. -
OGLE 2004-BLG-254: a K3 III Galactic Bulge Giant Spatially Resolved by A
Astronomy & Astrophysics manuscript no. 4414arti c ESO 2018 January 9, 2018 OGLE 2004–BLG–254: a K3 III Galactic Bulge Giant spatially resolved by a single microlens⋆ A. Cassan1,2,3, J.-P. Beaulieu1,3, P. Fouqu´e1,4, S. Brillant1,5, M. Dominik1,6, J. Greenhill1,7, D. Heyrovsk´y8, K. Horne1,6, U.G. Jørgensen1,9, D. Kubas1,5, H.C. Stempels6, C. Vinter1,9, M.D. Albrow1,12, D. Bennett1,13, J.A.R. Caldwell1,14,15, J.J. Calitz1,16, K. Cook1,17, C. Coutures1,18, D. Dominis1,19, J. Donatowicz1,20, K. Hill1,7, M. Hoffman1,16, S. Kane1,21, J.-B. Marquette1,3, R. Martin1,22, P. Meintjes1,16, J. Menzies1,23, V.R. Miller12, K.R. Pollard1,12, K.C. Sahu1,14, J. Wambsganss1,2, A. Williams1,22, A. Udalski10,11, M.K. Szyma´nski10,11, M. Kubiak10,11, G. Pietrzy´nski10,11,24, I. Soszy´nski10,11,24, K. Zebru´n˙ 10,11, O. Szewczyk10,11, and Ł. Wyrzykowski10,11,25 (Affiliations can be found after the references) Received ¡date¿ / Accepted ¡date¿ ABSTRACT Aims. We present an analysis of OGLE 2004–BLG–254, a high-magnification (A 60) and relatively short duration (tE 13.2 days) microlensing event in which the source star, a Bulge K-giant, has been spatially resolved◦ ≃ by a point-like lens. We seek to determine≃ the lens and source distance, and provide a measurement of the linear limb-darkening coefficients of the source star in the I and R bands. We discuss the derived values of the latter and compare them to the classical theoretical laws, and furthermore examine the cases of already published microlensed GK-giants limb-darkening measurements. -
Cycle 12 Abstract Catalog
Cycle 12 Abstract Catalog Generated April 04, 2003 ================================================================================ Proposal Category: GO Scientific Category: ISM AND CIRCUMSTELLAR MATTER ID: 9718 Title: SMC Extinction Curve Towards a Quiescent Molecular Cloud PI: Francois Boulanger PI Institution: Institut d'Astrophysique Spatiale The lack of 2175 A bump in the SMC extinction curve is interpreted as an absence of small carbon grains. ISO Mid-IR observations support this interpretation by showing that PAH features are absent in the spectra of SMC and LMC massive star forming regions. However, the only ISO observation of an SMC quiescent molecular cloud shows all PAH features, indicating a PAH abundance relative to large dust grains similar to that of Milky Way clouds. We identified a reddened B2III star associated with this cloud. We propose to observe it with STIS. This observation will provide the first measure of the extinction properties of SMC dust away from star forming regions. It will allow us to disentangle the effects of metallicity and massive stars on the SMC extinction curve and dust composition and to assess the relevance of the SMC bump-free extinction curve to low metallicity and/or starburst galaxies in general. ================================================================================ Proposal Category: GO Scientific Category: STELLAR POPULATIONS ID: 9719 Title: Search For Metallicity Spreads in M31 Globular Clusters PI: Terry Bridges PI Institution: Anglo-Australian Observatory Our recent deep HST photometry of the M31 halo globular cluster (GC) Mayall~II, also called G1, has revealed a red-giant branch with a clear spread that we attribute to an intrinsic metallicity dispersion of at least 0.4 dex in [Fe/H]. -
25.DORN Groundbasedtelescopes Part1.Pdf
A primer on Distances in the Universe Image: Splung.com physics 5/19/11 Reinhold Dorn ESI 2011 2 5/19/11 Reinhold Dorn ESI 2011 3 Stellar magnitude – a measure of the brightness of stars Astronomers talk about two different kinds of magnitudes: apparent and absolute. The apparent magnitude, m, of a star expresses how bright it appears, as seen from the earth, ranked on the magnitude scale. Two factors affect the apparent magnitude: 1. How luminous the star is 2. How far away the star is from the earth. Absolute magnitude, M, expresses the brightness of a star as it would be ranked on the magnitude scale if it was placed 10 pc (32.6 ly) from the earth. Since all stars would be placed at the same distance, absolute magnitudes show differences in actual luminosities. Some astronomical objects and their apparent magnitudes from Earth 5/19/11 Reinhold Dorn ESI 2011 4 The Hertzsprung-Russell diagram Hertzsprung-Russell diagram by Richard Powell Image: Richard Powell The H-R Diagram is an extremely useful. It shows the changes that take place as a star evolves. Most stars are on the Main Sequence because that is where stars spend most of their lives, burning hydrogen to helium. As stars live out their lives, changes in the structure of the star are reflected in changes in stars temperatures, sizes and luminosities, which cause them to move in tracks on the H-R Diagram. 5/19/11 Reinhold Dorn ESI 2011 5 It is important to understand a basic fact how planets and stars orbit: The Barycenter - the common center of mass Two bodies with an extreme Two bodies with similar mass orbiting difference in mass orbiting around a around a common barycenter with common barycenter (i.e. -
Extrasolar Planets Topics to Be Covered
3/25/2013 Extrasolar planets Astronomy 9601 1 Topics to be covered • 12.1 Physics and sizes • 12.2 Detecting extrasolar planets • 12.3 Observations of exoplanets • 12.4 Exoplanet statistics • 12.5 Planets and Life 2 What is a planet? What is a star? • The composition of Jupiter closely resembles that of the Sun: who’s to say that Jupiter is not simply a “failed star” rather than a planet? • The discovery of low-mass binary stars would be interesting, but (perhaps) not as exciting as discovering new “true” planets. • Is there a natural boundary between planets and stars? 3 1 3/25/2013 Planets and brown dwarfs • A star of mass less than 8% Luminosity “bump” due to short- of the Sun (80x Jupiter’s lived deuterium burning mass) will never grow hot Steady luminosity due to H burning enough in its core to fuse hydrogen • This is used as the boundary between true stars and very large gas planets • Object s b el ow thi s mass are called brown dwarfs • The boundary between BD and planet is more controversial – some argue it should be based on formation – other choose 0.013 solar masses=13 Mj as the boundary, as objects below this mass will never reach even deuterium fusion 4 Nelson et al., 1986, AJ, 311, 226 5 Pulsar planets • In 1992, Wolszczan and Frail announced the discovery of a multi‐ Artist’s conception of the planet planet planetary system around the orbiting pulsar PSR B1257+12 millisecond pulsar PSR 1257+12 (an earlier announcement had been retracted). -
Observer's Handbook 1989
OBSERVER’S HANDBOOK 1 9 8 9 EDITOR: ROY L. BISHOP THE ROYAL ASTRONOMICAL SOCIETY OF CANADA CONTRIBUTORS AND ADVISORS Alan H. B atten, Dominion Astrophysical Observatory, 5071 W . Saanich Road, Victoria, BC, Canada V8X 4M6 (The Nearest Stars). L a r r y D. B o g a n , Department of Physics, Acadia University, Wolfville, NS, Canada B0P 1X0 (Configurations of Saturn’s Satellites). Terence Dickinson, Yarker, ON, Canada K0K 3N0 (The Planets). D a v id W. D u n h a m , International Occultation Timing Association, 7006 Megan Lane, Greenbelt, MD 20770, U.S.A. (Lunar and Planetary Occultations). A lan Dyer, A lister Ling, Edmonton Space Sciences Centre, 11211-142 St., Edmonton, AB, Canada T5M 4A1 (Messier Catalogue, Deep-Sky Objects). Fred Espenak, Planetary Systems Branch, NASA-Goddard Space Flight Centre, Greenbelt, MD, U.S.A. 20771 (Eclipses and Transits). M a r ie F i d l e r , 23 Lyndale Dr., Willowdale, ON, Canada M2N 2X9 (Observatories and Planetaria). Victor Gaizauskas, J. W. D e a n , Herzberg Institute of Astrophysics, National Research Council, Ottawa, ON, Canada K1A 0R6 (Solar Activity). R o b e r t F. G a r r i s o n , David Dunlap Observatory, University of Toronto, Box 360, Richmond Hill, ON, Canada L4C 4Y6 (The Brightest Stars). Ian H alliday, Herzberg Institute of Astrophysics, National Research Council, Ottawa, ON, Canada K1A 0R6 (Miscellaneous Astronomical Data). W illiam H erbst, Van Vleck Observatory, Wesleyan University, Middletown, CT, U.S.A. 06457 (Galactic Nebulae). Ja m e s T. H im e r, 339 Woodside Bay S.W., Calgary, AB, Canada, T2W 3K9 (Galaxies). -
1903Aj 23 . . . 22K 22 the Asteojsomic Al
22 THE ASTEOJSOMIC AL JOUENAL. Nos- 531-532 22K . Taking into account the smallness of the weights in- concerned. Through the use of these tables the positions . volved, the individual differences which make up the and motions of many stars not included in the present 23 groups in the preceding table agree^very well. catalogue can be brought into systematic harmony with it, and apparently without materially less accuracy for the in- dividual stars than could be reached by special compu- Tables of Systematic Correction for N2 and A. tations for these stars in conformity with the system of B. 1903AJ The results of the foregoing comparisons. have been This is especially true of the star-places computed by utilized to form tables of systematic corrections for ISr2, An, Dr. Auwers in the catalogues, Ai and As. As will be seen Ai and As. In right-ascension no distinction is necessary by reference to the catalogue the positions and motions of between the various catalogues published by Dr. Auwers, south polar stars taken from N2 agree better with the beginning with the Fundamental-G at alo g ; but in decli- results of this investigation than do those taken from As, nation the distinction between the northern, intermediate, which, in turn, are quoted from the Cape Catalogue for and southern catalogues must be preserved, so far as is 1890. SYSTEMATIC COBEECTIOEB : CEDEE OF DECLINATIONS. Eight-Ascensions ; Cokrections, ¿las and 100z//xtf. Declinations; Corrections, Æs and IOOzZ/x^. B — ISa B —A B —N2 B —An B —Ai âas 100 â[is âas 100 âgô âSs 100 -
Extrasolar Planets
Extrasolar planets Astronomy 9601 1 Topics to be covered • 12.1 Physics and sizes • 12.2 Detecting extrasolar planets • 12. 3 Observa tions o f exop lane ts • 12.4 Exoplanet statistics • 12.5 Planets and Life 2 What is a planet? What is a star? • The composition of Jupiter closely resembles that of the Sun: who’s to say that Jupppyiter is not simply a “failed star” rather than a planet? • The discovery of low-mass binary stars would be interesting, but (perhaps) not as exciting as discovering new “true” planets. • Is there a natural boundary between planets and stars? 3 Planets and brown dwarfs • A star of mass less than 8% Luminosity “bump” due to short- of the Sun (80x Jupiter’s lived deuterium burning mass) will never grow hot Steady luminosity due to H burning enough in its core to fuse hydrogen • This is used as the boundary between true stars and very large gas planets • Objects below this mass are called brown dwarfs • The boundary between BD and planet is more controversial – some argue it should be based on formation – other choose 0.013 solar masses=13 Mj as the boundary, as objects below this mass will never reach even deuterium fusion 4 Nelson et al., 1986, AJ, 311, 226 5 Pulsar planets • In 1992, Wolszczan and Frail announced the discovery of a multi‐ Artist’s conception of the planet planet planetary system around the orbiting pulsar PSR B1257+12 millisecond pulsar PSR 1257+12 (an earlier announcement had been retracted). • These were the first two extrasolar pltlanets confirme d to be discovere d, and thus the first multi‐planet extrasolar planetary system discovered, and the first pulsar planets discovered • However, these objects are not in planetary systems as we usually think of them 6 Worlds Beyond Our Sun • In 1995 a team of Swiss astronomers disco vered the first planet (in a non- pulsar system) outside our soltlar system, or biting a sun-like star called 51 Pegasi. -
Astrophysical Applications of Gravitational Microlensing
Astrophysical Applications of Gravitational Microlensing Dissertation Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Subo Dong, M.S. Graduate Program in Astronomy The Ohio State University 2009 Dissertation Committee: Professor Andrew Philip Gould, Advisor Professor Bernard Scott Gaudi Professor Krzysztof Zbigniew Stanek Copyright by Subo Dong 2009 ABSTRACT In this thesis, I present several astrophysical applications of Galactic and cosmological microlensing. The first few topics are on searching and characterizing extrasolar planets by means of high-magnification microlensing events. The detection efficiency analysis of the A 3000 event OGLE-2004-BLG-343 is presented. Due to max ∼ human error, intensive monitoring did not begin until 43 minutes after peak, at which point the magnification had fallen to A 1200. It is shown that, had a ∼ similar event been well sampled over the peak, it would have been sensitive to almost all Neptune-mass planets over a factor of 5 in projected separation and even would have had some sensitivity to Earth-mass planets. New algorithms optimized for fast evaluation of binary-lens models with finite-sources effects have been developed. These algorithms have enabled efficient and thorough parameter-space searches in modeling planetary high-magnification events. The detection of the cool, Jovian-mass planet MOA-2007-BLG-400Lb, discovered from an Amax = 628 event with severe finite-source effects, is reported. Detailed analysis yields a fairly precise planet/star mass ratio of q = (2.5+0.5) 10−3, while the planet/star −0.3 × ii projected separation is subject to a strong close/wide degeneracy.