Astrophysical Distance Scale the JAGB Method: I. Calibration and a First Application Barry F
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Commission 27 of the Iau Information Bulletin
COMMISSION 27 OF THE I.A.U. INFORMATION BULLETIN ON VARIABLE STARS Nos. 2401 - 2500 1983 September - 1984 March EDITORS: B. SZEIDL AND L. SZABADOS, KONKOLY OBSERVATORY 1525 BUDAPEST, Box 67, HUNGARY HU ISSN 0374-0676 CONTENTS 2401 A POSSIBLE CATACLYSMIC VARIABLE IN CANCER Masaaki Huruhata 20 September 1983 2402 A NEW RR-TYPE VARIABLE IN LEO Masaaki Huruhata 20 September 1983 2403 ON THE DELTA SCUTI STAR BD +43d1894 A. Yamasaki, A. Okazaki, M. Kitamura 23 September 1983 2404 IQ Vel: IMPROVED LIGHT-CURVE PARAMETERS L. Kohoutek 26 September 1983 2405 FLARE ACTIVITY OF EPSILON AURIGAE? I.-S. Nha, S.J. Lee 28 September 1983 2406 PHOTOELECTRIC OBSERVATIONS OF 20 CVn Y.W. Chun, Y.S. Lee, I.-S. Nha 30 September 1983 2407 MINIMUM TIMES OF THE ECLIPSING VARIABLES AH Cep AND IU Aur Pavel Mayer, J. Tremko 4 October 1983 2408 PHOTOELECTRIC OBSERVATIONS OF THE FLARE STAR EV Lac IN 1980 G. Asteriadis, S. Avgoloupis, L.N. Mavridis, P. Varvoglis 6 October 1983 2409 HD 37824: A NEW VARIABLE STAR Douglas S. Hall, G.W. Henry, H. Louth, T.R. Renner 10 October 1983 2410 ON THE PERIOD OF BW VULPECULAE E. Szuszkiewicz, S. Ratajczyk 12 October 1983 2411 THE UNIQUE DOUBLE-MODE CEPHEID CO Aur E. Antonello, L. Mantegazza 14 October 1983 2412 FLARE STARS IN TAURUS A.S. Hojaev 14 October 1983 2413 BVRI PHOTOMETRY OF THE ECLIPSING BINARY QX Cas Thomas J. Moffett, T.G. Barnes, III 17 October 1983 2414 THE ABSOLUTE MAGNITUDE OF AZ CANCRI William P. Bidelman, D. Hoffleit 17 October 1983 2415 NEW DATA ABOUT THE APSIDAL MOTION IN THE SYSTEM OF RU MONOCEROTIS D.Ya. -
The Hubble Constant H0 --- Describing How Fast the Universe Is Expanding A˙ (T) H(T) = , A(T) = the Cosmic Scale Factor A(T)
Determining H0 and q0 from Supernova Data LA-UR-11-03930 Mian Wang Henan Normal University, P.R. China Baolian Cheng Los Alamos National Laboratory PANIC11, 25 July, 2011,MIT, Cambridge, MA Abstract Since 1929 when Edwin Hubble showed that the Universe is expanding, extensive observations of redshifts and relative distances of galaxies have established the form of expansion law. Mapping the kinematics of the expanding universe requires sets of measurements of the relative size and age of the universe at different epochs of its history. There has been decades effort to get precise measurements of two parameters that provide a crucial test for cosmology models. The two key parameters are the rate of expansion, i.e., the Hubble constant (H0) and the deceleration in expansion (q0). These two parameters have been studied from the exceedingly distant clusters where redshift is large. It is indicated that the universe is made up by roughly 73% of dark energy, 23% of dark matter, and 4% of normal luminous matter; and the universe is currently accelerating. Recently, however, the unexpected faintness of the Type Ia supernovae (SNe) at low redshifts (z<1) provides unique information to the study of the expansion behavior of the universe and the determination of the Hubble constant. In this work, We present a method based upon the distance modulus redshift relation and use the recent supernova Ia data to determine the parameters H0 and q0 simultaneously. Preliminary results will be presented and some intriguing questions to current theories are also raised. Outline 1. Introduction 2. Model and data analysis 3. -
AS1001: Galaxies and Cosmology Cosmology Today Title Current Mysteries Dark Matter ? Dark Energy ? Modified Gravity ? Course
AS1001: Galaxies and Cosmology Keith Horne [email protected] http://www-star.st-and.ac.uk/~kdh1/eg/eg.html Text: Kutner Astronomy:A Physical Perspective Chapters 17 - 21 Cosmology Title Today • Blah Current Mysteries Course Outline Dark Matter ? • Galaxies (distances, components, spectra) Holds Galaxies together • Evidence for Dark Matter • Black Holes & Quasars Dark Energy ? • Development of Cosmology • Hubble’s Law & Expansion of the Universe Drives Cosmic Acceleration. • The Hot Big Bang Modified Gravity ? • Hot Topics (e.g. Dark Energy) General Relativity wrong ? What’s in the exam? Lecture 1: Distances to Galaxies • Two questions on this course: (answer at least one) • Descriptive and numeric parts • How do we measure distances to galaxies? • All equations (except Hubble’s Law) are • Standard Candles (e.g. Cepheid variables) also in Stars & Elementary Astrophysics • Distance Modulus equation • Lecture notes contain all information • Example questions needed for the exam. Use book chapters for more details, background, and problem sets A Brief History 1860: Herchsel’s view of the Galaxy • 1611: Galileo supports Copernicus (Planets orbit Sun, not Earth) COPERNICAN COSMOLOGY • 1742: Maupertius identifies “nebulae” • 1784: Messier catalogue (103 fuzzy objects) • 1864: Huggins: first spectrum for a nebula • 1908: Leavitt: Cepheids in LMC • 1924: Hubble: Cepheids in Andromeda MODERN COSMOLOGY • 1929: Hubble discovers the expansion of the local universe • 1929: Einstein’s General Relativity • 1948: Gamov predicts background radiation from “Big Bang” • 1965: Penzias & Wilson discover Cosmic Microwave Background BIG BANG THEORY ADOPTED • 1975: Computers: Big-Bang Nucleosynthesis ( 75% H, 25% He ) • 1985: Observations confirm BBN predictions Based on star counts in different directions along the Milky Way. -
Galaxies – AS 3011
Galaxies – AS 3011 Simon Driver [email protected] ... room 308 This is a Junior Honours 18-lecture course Lectures 11am Wednesday & Friday Recommended book: The Structure and Evolution of Galaxies by Steven Phillipps Galaxies – AS 3011 1 Aims • To understand: – What is a galaxy – The different kinds of galaxy – The optical properties of galaxies – The hidden properties of galaxies such as dark matter, presence of black holes, etc. – Galaxy formation concepts and large scale structure • Appreciate: – Why galaxies are interesting, as building blocks of the Universe… and how simple calculations can be used to better understand these systems. Galaxies – AS 3011 2 1 from 1st year course: • AS 1001 covered the basics of : – distances, masses, types etc. of galaxies – spectra and hence dynamics – exotic things in galaxies: dark matter and black holes – galaxies on a cosmological scale – the Big Bang • in AS 3011 we will study dynamics in more depth, look at other non-stellar components of galaxies, and introduce high-redshift galaxies and the large-scale structure of the Universe Galaxies – AS 3011 3 Outline of lectures 1) galaxies as external objects 13) large-scale structure 2) types of galaxy 14) luminosity of the Universe 3) our Galaxy (components) 15) primordial galaxies 4) stellar populations 16) active galaxies 5) orbits of stars 17) anomalies & enigmas 6) stellar distribution – ellipticals 18) revision & exam advice 7) stellar distribution – spirals 8) dynamics of ellipticals plus 3-4 tutorials 9) dynamics of spirals (questions set after -
Measurements and Numbers in Astronomy Astronomy Is a Branch of Science
Name: ________________________________Lab Day & Time: ____________________________ Measurements and Numbers in Astronomy Astronomy is a branch of science. You will be exposed to some numbers expressed in SI units, large and small numbers, and some numerical operations such as addition / subtraction, multiplication / division, and ratio comparison. Let’s watch part of an IMAX movie called Cosmic Voyage. https://www.youtube.com/watch?v=xEdpSgz8KU4 Powers of 10 In Astronomy, we deal with numbers that describe very large and very small things. For example, the mass of the Sun is 1,990,000,000,000,000,000,000,000,000,000 kg and the mass of a proton is 0.000,000,000,000,000,000,000,000,001,67 kg. Such numbers are very cumbersome and difficult to understand. It is neater and easier to use the scientific notation, or the powers of 10 notation. For large numbers: For small numbers: 1 no zero = 10 0 10 1 zero = 10 1 0.1 = 1/10 Divided by 10 =10 -1 100 2 zero = 10 2 0.01 = 1/100 Divided by 100 =10 -2 1000 3 zero = 10 3 0.001 = 1/1000 Divided by 1000 =10 -3 Example used on real numbers: 1,990,000,000,000,000,000,000,000,000,000 kg -> 1.99X1030 kg 0.000,000,000,000,000,000,000,000,001,67 kg -> 1.67X10-27 kg See how much neater this is! Now write the following in scientific notation. 1. 40,000 2. 9,000,000 3. 12,700 4. 380,000 5. 0.017 6. -
A Magnetar Model for the Hydrogen-Rich Super-Luminous Supernova Iptf14hls Luc Dessart
A&A 610, L10 (2018) https://doi.org/10.1051/0004-6361/201732402 Astronomy & © ESO 2018 Astrophysics LETTER TO THE EDITOR A magnetar model for the hydrogen-rich super-luminous supernova iPTF14hls Luc Dessart Unidad Mixta Internacional Franco-Chilena de Astronomía (CNRS, UMI 3386), Departamento de Astronomía, Universidad de Chile, Camino El Observatorio 1515, Las Condes, Santiago, Chile e-mail: [email protected] Received 2 December 2017 / Accepted 14 January 2018 ABSTRACT Transient surveys have recently revealed the existence of H-rich super-luminous supernovae (SLSN; e.g., iPTF14hls, OGLE-SN14-073) that are characterized by an exceptionally high time-integrated bolometric luminosity, a sustained blue optical color, and Doppler- broadened H I lines at all times. Here, I investigate the effect that a magnetar (with an initial rotational energy of 4 × 1050 erg and 13 field strength of 7 × 10 G) would have on the properties of a typical Type II supernova (SN) ejecta (mass of 13.35 M , kinetic 51 56 energy of 1:32 × 10 erg, 0.077 M of Ni) produced by the terminal explosion of an H-rich blue supergiant star. I present a non-local thermodynamic equilibrium time-dependent radiative transfer simulation of the resulting photometric and spectroscopic evolution from 1 d until 600 d after explosion. With the magnetar power, the model luminosity and brightness are enhanced, the ejecta is hotter and more ionized everywhere, and the spectrum formation region is much more extended. This magnetar-powered SN ejecta reproduces most of the observed properties of SLSN iPTF14hls, including the sustained brightness of −18 mag in the R band, the blue optical color, and the broad H I lines for 600 d. -
Evolution of Thermally Pulsing Asymptotic Giant Branch Stars
The Astrophysical Journal, 822:73 (15pp), 2016 May 10 doi:10.3847/0004-637X/822/2/73 © 2016. The American Astronomical Society. All rights reserved. EVOLUTION OF THERMALLY PULSING ASYMPTOTIC GIANT BRANCH STARS. V. CONSTRAINING THE MASS LOSS AND LIFETIMES OF INTERMEDIATE-MASS, LOW-METALLICITY AGB STARS* Philip Rosenfield1,2,7, Paola Marigo2, Léo Girardi3, Julianne J. Dalcanton4, Alessandro Bressan5, Benjamin F. Williams4, and Andrew Dolphin6 1 Harvard-Smithsonian Center for Astrophysics, 60 Garden St., Cambridge, MA 02138, USA 2 Department of Physics and Astronomy G. Galilei, University of Padova, Vicolo dell’Osservatorio 3, I-35122 Padova, Italy 3 Osservatorio Astronomico di Padova—INAF, Vicolo dell’Osservatorio 5, I-35122 Padova, Italy 4 Department of Astronomy, University of Washington, Box 351580, Seattle, WA 98195, USA 5 Astrophysics Sector, SISSA, Via Bonomea 265, I-34136 Trieste, Italy 6 Raytheon Company, 1151 East Hermans Road, Tucson, AZ 85756, USA Received 2016 January 1; accepted 2016 March 14; published 2016 May 6 ABSTRACT Thermally pulsing asymptotic giant branch (TP-AGB) stars are relatively short lived (less than a few Myr), yet their cool effective temperatures, high luminosities, efficient mass loss, and dust production can dramatically affect the chemical enrichment histories and the spectral energy distributions of their host galaxies. The ability to accurately model TP-AGB stars is critical to the interpretation of the integrated light of distant galaxies, especially in redder wavelengths. We continue previous efforts to constrain the evolution and lifetimes of TP-AGB stars by modeling their underlying stellar populations. Using Hubble Space Telescope (HST) optical and near-infrared photometry taken of 12 fields of 10 nearby galaxies imaged via the Advanced Camera for Surveys Nearby Galaxy Survey Treasury and the near-infrared HST/SNAP follow-up campaign, we compare the model and observed TP- AGB luminosity functions as well as the ratio of TP-AGB to red giant branch stars. -
PHAS 1102 Physics of the Universe 3 – Magnitudes and Distances
PHAS 1102 Physics of the Universe 3 – Magnitudes and distances Brightness of Stars • Luminosity – amount of energy emitted per second – not the same as how much we observe! • We observe a star’s apparent brightness – Depends on: • luminosity • distance – Brightness decreases as 1/r2 (as distance r increases) • other dimming effects – dust between us & star Defining magnitudes (1) Thus Pogson formalised the magnitude scale for brightness. This is the brightness that a star appears to have on the sky, thus it is referred to as apparent magnitude. Also – this is the brightness as it appears in our eyes. Our eyes have their own response to light, i.e. they act as a kind of filter, sensitive over a certain wavelength range. This filter is called the visual band and is centred on ~5500 Angstroms. Thus these are apparent visual magnitudes, mv Related to flux, i.e. energy received per unit area per unit time Defining magnitudes (2) For example, if star A has mv=1 and star B has mv=6, then 5 mV(B)-mV(A)=5 and their flux ratio fA/fB = 100 = 2.512 100 = 2.512mv(B)-mv(A) where !mV=1 corresponds to a flux ratio of 1001/5 = 2.512 1 flux(arbitrary units) 1 6 apparent visual magnitude, mv From flux to magnitude So if you know the magnitudes of two stars, you can calculate mv(B)-mv(A) the ratio of their fluxes using fA/fB = 2.512 Conversely, if you know their flux ratio, you can calculate the difference in magnitudes since: 2.512 = 1001/5 log (f /f ) = [m (B)-m (A)] log 2.512 10 A B V V 10 = 102/5 = 101/2.5 mV(B)-mV(A) = !mV = 2.5 log10(fA/fB) To calculate a star’s apparent visual magnitude itself, you need to know the flux for an object at mV=0, then: mS - 0 = mS = 2.5 log10(f0) - 2.5 log10(fS) => mS = - 2.5 log10(fS) + C where C is a constant (‘zero-point’), i.e. -
The H and G Magnitude System for Asteroids
Meetings The BAA Observers’ Workshops The H and G magnitude system for asteroids This article is based on a presentation given at the Observers’ Workshop held at the Open University in Milton Keynes on 2007 February 24. It can be viewed on the Asteroids & Remote Planets Section website at http://homepage.ntlworld.com/ roger.dymock/index.htm When you look at an asteroid through the eyepiece of a telescope or on a CCD image it is a rather unexciting point of light. However by analysing a number of images, information on the nature of the object can be gleaned. Frequent (say every minute or few min- Figure 2. The inclined orbit of (23) Thalia at opposition. utes) measurements of magnitude over periods of several hours can be used to generate a lightcurve. Analysis of such a lightcurve Absolute magnitude, H: the V-band magnitude of an asteroid if yields the period, shape and pole orientation of the object. it were 1 AU from the Earth and 1 AU from the Sun and fully Measurements of position (astrometry) can be used to calculate illuminated, i.e. at zero phase angle (actually a geometrically the orbit of the asteroid and thus its distance from the Earth and the impossible situation). H can be calculated from the equation Sun at the time of the observations. These distances must be known H = H(α) + 2.5log[(1−G)φ (α) + G φ (α)], where: in order for the absolute magnitude, H and the slope parameter, G 1 2 φ (α) = exp{−A (tan½ α)Bi} to be calculated (it is common for G to be given a nominal value of i i i = 1 or 2, A = 3.33, A = 1.87, B = 0.63 and B = 1.22 0.015). -
The Distance to NGC 1316 \(Fornax
A&A 552, A106 (2013) Astronomy DOI: 10.1051/0004-6361/201220756 & c ESO 2013 Astrophysics The distance to NGC 1316 (Fornax A): yet another curious case,, M. Cantiello1,A.Grado2, J. P. Blakeslee3, G. Raimondo1,G.DiRico1,L.Limatola2, E. Brocato1,4, M. Della Valle2,6, and R. Gilmozzi5 1 INAF, Osservatorio Astronomico di Teramo, via M. Maggini snc, 64100 Teramo, Italy e-mail: [email protected] 2 INAF, Osservatorio Astronomico di Capodimonte, salita Moiariello, 80131 Napoli, Italy 3 Dominion Astrophysical Observatory, Herzberg Institute of Astrophysics, National Research Council of Canada, Victoria BC V82 3H3, Canada 4 INAF, Osservatorio Astronomico di Roma, via Frascati 33, Monte Porzio Catone, 00040 Roma, Italy 5 European Southern Observatory, Karl–Schwarzschild–Str. 2, 85748 Garching bei München, Germany 6 International Centre for Relativistic Astrophysics, Piazzale della Repubblica 2, 65122 Pescara, Italy Received 16 November 2012 / Accepted 14 February 2013 ABSTRACT Aims. The distance of NGC 1316, the brightest galaxy in the Fornax cluster, provides an interesting test for the cosmological distance scale. First, because Fornax is the second largest cluster of galaxies within 25 Mpc after Virgo and, in contrast to Virgo, has a small line-of-sight depth; and second, because NGC 1316 is the single galaxy with the largest number of detected Type Ia supernovae (SNe Ia), giving the opportunity to test the consistency of SNe Ia distances both internally and against other distance indicators. Methods. We measure surface brightness fluctuations (SBF) in NGC 1316 from ground- and space-based imaging data. The sample provides a homogeneous set of measurements over a wide wavelength interval. -
The Hertzsprung-Russell Diagram
PHY111 1 The HR Diagram THE HERTZSPRUNG -RUSSELL DIAGRAM THE AXES The Hertzsprung-Russell (HR) diagram is a plot of luminosity (total power output) against surface temperature , both on log scales. Since neither luminosity nor surface temperature is a directly observed quantity, real plots tend to use observable quantities that are related to luminosity and temperature. The table below gives common axis scales you may see in the lectures or in textbooks. Note that the x-axis runs from hot to cold, not from cold to hot! Axis Theoretical Observational x Teff (on log scale) Spectral class OBAFGKM or Colour index B – V, V – I or log 10 Teff y L/L⊙ (on log scale) Absolute visual magnitude MV (or other wavelengths) 1 or log 10 (L/L⊙) Apparent visual magnitude V (or other wavelengths) The symbol ⊙ means the Sun—i.e., the luminosity is measured in terms of the Sun’s luminosity, rather than in watts. Teff is effective temperature (the temperature of a blackbody of the same surface area and total power output). BRANCHES OF THE HR DIAGRAM This is a real HR diagram, of the globular cluster NGC1261, constructed using data from the HST. The horizontal line is a fit to the diagram assuming [Fe/H] = −1.35 branch (the heavy element content of the cluster is 4.5% of the Sun’s heavy element content), a distance red giant modulus of 16.15 (the absolute magnitude is found branch by subtracting 16.15 from the apparent magnitude) and an age of 12.0 Gyr. subgiant Reference: NEQ Paust et al, AJ 139 (2010) 476. -
The Distance to Andromeda
How to use the Virtual Observatory The Distance to Andromeda Florian Freistetter, ARI Heidelberg Introduction an can compare that value with the apparent magnitude m, which can be easily Measuring the distances to other celestial measured. Knowing, how bright the star is objects is difficult. For near objects, like the and how bright he appears, one can use moon and some planets, it can be done by the so called distance modulus: sending radio-signals and measure the time it takes for them to be reflected back to the m – M = -5 + 5 log r Earth. Even for near stars it is possible to get quite acurate distances by using the where r is the distance of the object parallax-method. measured in parsec (1 parsec is 3.26 lightyears or 31 trillion kilometers). But for distant objects, determining their distance becomes very difficult. From Earth, With this method, in 1923 Edwin Hubble we can only measure the apparant was able to observe Cepheids in the magnitude and not how bright they really Andromeda nebula and thus determine its are. A small, dim star that is close to the distance: it was indeed an object far outside Earth can appear to look the same as a the milky way and an own galaxy! large, bright star that is far away from Earth. Measuring the distance to As long as the early 20th century it was not Andrimeda with Aladin possible to resolve this major problem in distance determination. At this time, one To measure the distance to Andromeda was especially interested in determining the with Aladin, one first needs observational distance to the so called „nebulas“.