The Formation of Particles in the Universe
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Cosmicflows-3: Cosmography of the Local Void
Draft version May 22, 2019 Preprint typeset using LATEX style AASTeX6 v. 1.0 COSMICFLOWS-3: COSMOGRAPHY OF THE LOCAL VOID R. Brent Tully, Institute for Astronomy, University of Hawaii, 2680 Woodlawn Drive, Honolulu, HI 96822, USA Daniel Pomarede` Institut de Recherche sur les Lois Fondamentales de l'Univers, CEA, Universite' Paris-Saclay, 91191 Gif-sur-Yvette, France Romain Graziani University of Lyon, UCB Lyon 1, CNRS/IN2P3, IPN Lyon, France Hel´ ene` M. Courtois University of Lyon, UCB Lyon 1, CNRS/IN2P3, IPN Lyon, France Yehuda Hoffman Racah Institute of Physics, Hebrew University, Jerusalem, 91904 Israel Edward J. Shaya University of Maryland, Astronomy Department, College Park, MD 20743, USA ABSTRACT Cosmicflows-3 distances and inferred peculiar velocities of galaxies have permitted the reconstruction of the structure of over and under densities within the volume extending to 0:05c. This study focuses on the under dense regions, particularly the Local Void that lies largely in the zone of obscuration and consequently has received limited attention. Major over dense structures that bound the Local Void are the Perseus-Pisces and Norma-Pavo-Indus filaments sepa- rated by 8,500 km s−1. The void network of the universe is interconnected and void passages are found from the Local Void to the adjacent very large Hercules and Sculptor voids. Minor filaments course through voids. A particularly interesting example connects the Virgo and Perseus clusters, with several substantial galaxies found along the chain in the depths of the Local Void. The Local Void has a substantial dynamical effect, causing a deviant motion of the Local Group of 200 − 250 km s−1. -
Observing List
day month year Epoch 2000 local clock time: 23.98 Observing List for 23 7 2019 RA DEC alt az Constellation object mag A mag B Separation description hr min deg min 20 50 Andromeda Gamma Andromedae (*266) 2.3 5.5 9.8 yellow & blue green double star 2 3.9 42 19 28 69 Andromeda Pi Andromedae 4.4 8.6 35.9 bright white & faint blue 0 36.9 33 43 30 55 Andromeda STF 79 (Struve) 6 7 7.8 bluish pair 1 0.1 44 42 16 52 Andromeda 59 Andromedae 6.5 7 16.6 neat pair, both greenish blue 2 10.9 39 2 45 67 Andromeda NGC 7662 (The Blue Snowball) planetary nebula, fairly bright & slightly elongated 23 25.9 42 32.1 31 60 Andromeda M31 (Andromeda Galaxy) large sprial arm galaxy like the Milky Way 0 42.7 41 16 31 61 Andromeda M32 satellite galaxy of Andromeda Galaxy 0 42.7 40 52 32 60 Andromeda M110 (NGC205) satellite galaxy of Andromeda Galaxy 0 40.4 41 41 17 55 Andromeda NGC752 large open cluster of 60 stars 1 57.8 37 41 17 48 Andromeda NGC891 edge on galaxy, needle-like in appearance 2 22.6 42 21 45 69 Andromeda NGC7640 elongated galaxy with mottled halo 23 22.1 40 51 46 57 Andromeda NGC7686 open cluster of 20 stars 23 30.2 49 8 30 121 Aquarius 55 Aquarii, Zeta 4.3 4.5 2.1 close, elegant pair of yellow stars 22 28.8 0 -1 12 120 Aquarius 94 Aquarii 5.3 7.3 12.7 pale rose & emerald 23 19.1 -13 28 32 152 Aquarius M72 globular cluster 20 53.5 -12 32 31 151 Aquarius M73 Y-shaped asterism of 4 stars 20 59 -12 38 16 117 Aquarius NGC7606 Galaxy 23 19.1 -8 29 32 149 Aquarius NGC7009 Saturn Neb planetary nebula, large & bright pale green oval 21 4.2 -11 21.8 38 135 -
Rotating Wolf-Rayet Stars in a Post RSG/LBV Phase an Evolutionary Channel Towards Long-Duration Grbs?
A&A 547, A83 (2012) Astronomy DOI: 10.1051/0004-6361/201118664 & c ESO 2012 Astrophysics Rotating Wolf-Rayet stars in a post RSG/LBV phase An evolutionary channel towards long-duration GRBs? G. Gräfener1,J.S.Vink1, T. J. Harries2, and N. Langer3 1 Armagh Observatory, College Hill, Armagh BT61 9DG, UK 2 School of Physics and Astronomy, University of Exeter, Stocker Rd, Exeter EX4 4QL, UK 3 Argelander-Institut für Astronomie der Universität Bonn, Auf dem Hügel 71, 53121 Bonn, Germany Received 16 December 2011 / Accepted 3 October 2012 ABSTRACT Context. Wolf-Rayet (WR) stars with fast rotating cores are thought to be the direct progenitors of long-duration gamma-ray bursts (LGRBs). A well accepted evolutionary channel towards LGRBs is chemically-homogeneous evolution at low metallicities, which completely avoids a red supergiant (RSG), or luminous blue variable (LBV) phase. On the other hand, strong absorption features with velocities of several hundred km s−1 have been found in some LGRB afterglow spectra (GRB 020813 and GRB 021004), which have been attributed to dense circumstellar (CS) material that has been ejected in a previous RSG or LBV phase, and is interacting with a fast WR-type stellar wind. Aims. Here we investigate the properties of Galactic WR stars and their environment to identify similar evolutionary channels that may lead to the formation of LGRBs. Methods. We compile available information on the spectropolarimetric properties of 29 WR stars, the presence of CS ejecta for 172 WR stars, and the CS velocities in the environment of 34 WR stars in the Galaxy. -
Arxiv:2105.11583V2 [Astro-Ph.EP] 2 Jul 2021 Keck-HIRES, APF-Levy, and Lick-Hamilton Spectrographs
Draft version July 6, 2021 Typeset using LATEX twocolumn style in AASTeX63 The California Legacy Survey I. A Catalog of 178 Planets from Precision Radial Velocity Monitoring of 719 Nearby Stars over Three Decades Lee J. Rosenthal,1 Benjamin J. Fulton,1, 2 Lea A. Hirsch,3 Howard T. Isaacson,4 Andrew W. Howard,1 Cayla M. Dedrick,5, 6 Ilya A. Sherstyuk,1 Sarah C. Blunt,1, 7 Erik A. Petigura,8 Heather A. Knutson,9 Aida Behmard,9, 7 Ashley Chontos,10, 7 Justin R. Crepp,11 Ian J. M. Crossfield,12 Paul A. Dalba,13, 14 Debra A. Fischer,15 Gregory W. Henry,16 Stephen R. Kane,13 Molly Kosiarek,17, 7 Geoffrey W. Marcy,1, 7 Ryan A. Rubenzahl,1, 7 Lauren M. Weiss,10 and Jason T. Wright18, 19, 20 1Cahill Center for Astronomy & Astrophysics, California Institute of Technology, Pasadena, CA 91125, USA 2IPAC-NASA Exoplanet Science Institute, Pasadena, CA 91125, USA 3Kavli Institute for Particle Astrophysics and Cosmology, Stanford University, Stanford, CA 94305, USA 4Department of Astronomy, University of California Berkeley, Berkeley, CA 94720, USA 5Cahill Center for Astronomy & Astrophysics, California Institute of Technology, Pasadena, CA 91125, USA 6Department of Astronomy & Astrophysics, The Pennsylvania State University, 525 Davey Lab, University Park, PA 16802, USA 7NSF Graduate Research Fellow 8Department of Physics & Astronomy, University of California Los Angeles, Los Angeles, CA 90095, USA 9Division of Geological and Planetary Sciences, California Institute of Technology, Pasadena, CA 91125, USA 10Institute for Astronomy, University of Hawai`i, -
A Fuse Survey of the Rotation Rates of Very Massive Stars in the Small and Large Magellanic Clouds
The Astrophysical Journal, 700:844–858, 2009 July 20 doi:10.1088/0004-637X/700/1/844 C 2009. The American Astronomical Society. All rights reserved. Printed in the U.S.A. A FUSE SURVEY OF THE ROTATION RATES OF VERY MASSIVE STARS IN THE SMALL AND LARGE MAGELLANIC CLOUDS Laura R. Penny1 and Douglas R. Gies2 1 Department of Physics and Astronomy, The College of Charleston, Charleston, SC 29424, USA; [email protected] 2 Center for High Angular Resolution Astronomy and Department of Physics and Astronomy, Georgia State University, P.O. Box 4106, Atlanta, GA 30302-4106, USA; [email protected] Received 2009 February 3; accepted 2009 May 26; published 2009 July 6 ABSTRACT We present projected rotational velocity values for 97 Galactic, 55 SMC, and 106 LMC O-B type stars from archival FUSE observations. The evolved and unevolved samples from each environment are compared through the Kolmogorov–Smirnov test to determine if the distribution of equatorial rotational velocities is metallicity dependent for these massive objects. Stellar interior models predict that massive stars with SMC metallicity will have significantly reduced angular momentum loss on the main sequence compared to their Galactic counterparts. Our results find some support for this prediction but also show that even at Galactic metallicity, evolved and unevolved massive stars have fairly similar fractions of stars with large V sin i values. Macroturbulent broadening that is present in the spectral features of Galactic evolved massive stars is lower in the LMC and SMC samples. This suggests the processes that lead to macroturbulence are dependent upon metallicity. -
X-Ray Emission from Wolf-Rayet Stars
X-ray Emission from Wolf-Rayet Stars Steve Skinner1, Svet Zhekov2, Manuel Güdel3 Werner Schmutz4, Kimberly Sokal1 1CASA, Univ. of Colorado (USA) [email protected] 2Space Research Inst. (Bulgaria) and JILA/Univ. of Colorado (USA) 3ETH Zurich (Switzerland) 3PMOD (Switzerland) Abstract We present an overview of recent X-ray observations of Wolf-Rayet (WR) stars with XMM-Newton and Chandra. Observations of several WC-type (carbon-rich) WR stars without known companions have yielded only non-detections, implying they are either very feeble X-ray emitters or perhaps even X-ray quiet. In contrast, several apparently single WN2-6 stars have been detected, but data are sparse for later WN7-9 stars. Putatively single WN stars such as WR 134 have X-ray luminosities and spectra that are strikingly similar to some known WN + OB binaries such as WR 147, suggesting a similar emission mechanism. 1 X-rays from WR Stars: Overview 3 Single Nitrogen-rich WN Stars 4 Wolf-Rayet Binaries WR stars are the evolutionary descendants of massive O • Sensitive X-ray observations have now been obtained • High-resolution X-ray grating spectra have been ob- stars and are losing mass at very high rates. They are in ad- of several putatively single WN2-6 stars with XMM tained for a few binaries such as γ2 Vel (WC8 + vanced nuclear burning stages, approaching the end of their and Chandra. All but one were detected (Fig. 1). O7.5; Fig. 3) and WR 140 (WC7 + O4-5). CCD lives as supernovae. Strong X-rays have been detected from CCD spectra exist (Fig. -
Exoplanet.Eu Catalog Page 1 # Name Mass Star Name
exoplanet.eu_catalog # name mass star_name star_distance star_mass OGLE-2016-BLG-1469L b 13.6 OGLE-2016-BLG-1469L 4500.0 0.048 11 Com b 19.4 11 Com 110.6 2.7 11 Oph b 21 11 Oph 145.0 0.0162 11 UMi b 10.5 11 UMi 119.5 1.8 14 And b 5.33 14 And 76.4 2.2 14 Her b 4.64 14 Her 18.1 0.9 16 Cyg B b 1.68 16 Cyg B 21.4 1.01 18 Del b 10.3 18 Del 73.1 2.3 1RXS 1609 b 14 1RXS1609 145.0 0.73 1SWASP J1407 b 20 1SWASP J1407 133.0 0.9 24 Sex b 1.99 24 Sex 74.8 1.54 24 Sex c 0.86 24 Sex 74.8 1.54 2M 0103-55 (AB) b 13 2M 0103-55 (AB) 47.2 0.4 2M 0122-24 b 20 2M 0122-24 36.0 0.4 2M 0219-39 b 13.9 2M 0219-39 39.4 0.11 2M 0441+23 b 7.5 2M 0441+23 140.0 0.02 2M 0746+20 b 30 2M 0746+20 12.2 0.12 2M 1207-39 24 2M 1207-39 52.4 0.025 2M 1207-39 b 4 2M 1207-39 52.4 0.025 2M 1938+46 b 1.9 2M 1938+46 0.6 2M 2140+16 b 20 2M 2140+16 25.0 0.08 2M 2206-20 b 30 2M 2206-20 26.7 0.13 2M 2236+4751 b 12.5 2M 2236+4751 63.0 0.6 2M J2126-81 b 13.3 TYC 9486-927-1 24.8 0.4 2MASS J11193254 AB 3.7 2MASS J11193254 AB 2MASS J1450-7841 A 40 2MASS J1450-7841 A 75.0 0.04 2MASS J1450-7841 B 40 2MASS J1450-7841 B 75.0 0.04 2MASS J2250+2325 b 30 2MASS J2250+2325 41.5 30 Ari B b 9.88 30 Ari B 39.4 1.22 38 Vir b 4.51 38 Vir 1.18 4 Uma b 7.1 4 Uma 78.5 1.234 42 Dra b 3.88 42 Dra 97.3 0.98 47 Uma b 2.53 47 Uma 14.0 1.03 47 Uma c 0.54 47 Uma 14.0 1.03 47 Uma d 1.64 47 Uma 14.0 1.03 51 Eri b 9.1 51 Eri 29.4 1.75 51 Peg b 0.47 51 Peg 14.7 1.11 55 Cnc b 0.84 55 Cnc 12.3 0.905 55 Cnc c 0.1784 55 Cnc 12.3 0.905 55 Cnc d 3.86 55 Cnc 12.3 0.905 55 Cnc e 0.02547 55 Cnc 12.3 0.905 55 Cnc f 0.1479 55 -
Interstellarum 85 • Dezember/Januar 2013 1 Inhalt
Editorial fokussiert Liebe Leserinnen und Leser, wissen Sie schon, was Sie am 21. Dezember tun werden? Wahrschein- lich werden Sie auf der Jagd nach letzten Geschenken durch die Geschäfte ziehen oder einen Glühwein auf dem Weihnachtsmarkt trinken. Geht es nach vielen Paranoikern im Internet, wird dieser Tag aber weniger beschau- lich enden – nichts weniger als der Weltuntergang ist angekündigt. Nun . t könnte uns diese unsinnige Prophezeiung so wenig interessieren wie viele g andere zuvor, doch diesmal wird die Astronomie als Schreckgespenst miss- braucht: Ein mythischer »Planet X« soll sich uns nähern, die anderen Pla- neten die Erde aus ihrer Bahn reißen, die Sonne sich mit dem Zentrum der Milchstraße »synchronisieren«, und zu allem Überfl uss »endet« auch noch ist untersa g der Kalender der Maya. Was sich hinter dieser wüsten Ankündigung ver- Ronald Stoyan, Chefredakteur birgt, haben Oliver Debus und Oliver Dreißigacker recherchiert (Seite 12). reitun Dass viele Menschen diese Ankündigungen tatsächlich glauben, berichtet b Florian Freistetter in einem Interview auf interstellarum.de. Jupiter steht nicht nur bestens platziert am Abendhimmel, sondern auch im Zentrum dieses Heftes. Neben Details zur aktuellen Oppositions- stellung (Seite 18) und Neuigkeiten von seiner veränderlichen Wolkenober- fl äche (Seite 23), bringt dieses Heft eine ausführliche Anleitung zur Beob- achtung des Riesenplaneten (Seite 34). Außerdem erklärt Peter M. Oden in seinem Beitrag, wie man aus Webcam-Aufnahmen Rotations-Animationen der Planeten erstellt (Seite 52). Nutzen Sie den idealen Stand von Jupiter für eigene Versuche! Sind Sie Astrofotograf – oder gerade dabei, einer zu werden? Dann sollten Sie unbedingt an unserem neuen Fotowettbewerb teilnehmen, zu dem wir mit der Firma Astrosysteme Austria (ASA) zusammen einladen: In den Kategorien Einsteiger und Experten sind Preise im Gesamtwert von über 15000 Euro ausgelobt – so viel gab es noch bei keinem astro- nur zu privaten Zwecken. -
Star Formation in Ring Galaxies Susan C
East Tennessee State University Digital Commons @ East Tennessee State University Undergraduate Honors Theses Student Works 5-2016 Star Formation in Ring Galaxies Susan C. Olmsted East Tennessee State Universtiy Follow this and additional works at: https://dc.etsu.edu/honors Part of the Astrophysics and Astronomy Commons, and the Physics Commons Recommended Citation Olmsted, Susan C., "Star Formation in Ring Galaxies" (2016). Undergraduate Honors Theses. Paper 322. https://dc.etsu.edu/honors/ 322 This Honors Thesis - Open Access is brought to you for free and open access by the Student Works at Digital Commons @ East Tennessee State University. It has been accepted for inclusion in Undergraduate Honors Theses by an authorized administrator of Digital Commons @ East Tennessee State University. For more information, please contact [email protected]. Star Formation in Ring Galaxies Susan Olmsted Honors Thesis May 5, 2016 Student: Susan Olmsted: ______________________________________ Mentor: Dr. Beverly Smith: ____________________________________ Reader 1: Dr. Mark Giroux: ____________________________________ Reader 2: Dr. Michele Joyner: __________________________________ 1 Abstract: Ring galaxies are specific types of interacting galaxies in which a smaller galaxy has passed through the center of the disk of another larger galaxy. The intrusion of the smaller galaxy causes the structure of the larger galaxy to compress as the smaller galaxy falls through, and to recoil back after the smaller galaxy passes through, hence the ring-like shape. In our research, we studied the star-forming regions of a sample of ring galaxies and compared to those of other interacting galaxies and normal galaxies. Using UV, optical, and IR archived images in twelve wavelengths from three telescopes, we analyzed samples of star-forming regions in ring and normal spiral galaxies using photometry. -
The VLT-FLAMES Tarantula Survey III
A&A 530, L14 (2011) Astronomy DOI: 10.1051/0004-6361/201117043 & c ESO 2011 Astrophysics Letter to the Editor The VLT-FLAMES Tarantula Survey III. A very massive star in apparent isolation from the massive cluster R136 J. M. Bestenlehner1,J.S.Vink1, G. Gräfener1, F. Najarro2,C.J.Evans3, N. Bastian4,5, A. Z. Bonanos6, E. Bressert5,7,8, P.A. Crowther9,E.Doran9, K. Friedrich10, V.Hénault-Brunet11, A. Herrero12,13,A.deKoter14,15, N. Langer10, D. J. Lennon16, J. Maíz Apellániz17,H.Sana14, I. Soszynski18, and W. D. Taylor11 1 Armagh Observatory, College Hill, Armagh BT61 9DG, UK e-mail: [email protected] 2 Centro de Astrobiología (CSIC-INTA), Ctra. de Torrejón a Ajalvir km-4, 28850 Torrejón de Ardoz, Madrid, Spain 3 UK Astronomy Technology Centre, Royal Observatory Edinburgh, Blackford Hill, Edinburgh, EH9 3HJ, UK 4 Excellence Cluster Universe, Boltzmannstr. 2, 85748 Garching, Germany 5 School of Physics, University of Exeter, Stocker Road, Exeter EX4 4QL, UK 6 Institute of Astronomy & Astrophysics, National Observatory of Athens, I. Metaxa & Vas. Pavlou Street, P. Penteli 15236, Greece 7 European Southern Observatory, Karl-Schwarzschild-Strasse 2, 87548 Garching bei München, Germany 8 Harvard-Smithsonian CfA, 60 Garden Street, Cambridge, MA 02138, USA 9 Dept. of Physics & Astronomy, Hounsfield Road, University of Sheffield, S3 7RH, UK 10 Argelander-Institut für Astronomie der Universität Bonn, Auf dem Hügel 71, 53121 Bonn, Germany 11 SUPA, IfA, University of Edinburgh, Royal Observatory Edinburgh, Blackford Hill, Edinburgh, EH9 3HJ, UK 12 Departamento -
A Code to Measure Stellar Atmospheric Parameters and Their Covariance from Spectra
MNRAS 467, 971–984 (2017) doi:10.1093/mnras/stx144 Advance Access publication 2017 January 19 ZASPE: a code to measure stellar atmospheric parameters and their covariance from spectra Rafael Brahm,1,2‹ Andres´ Jordan,´ 1,2 Joel Hartman3 and Gasp´ ar´ Bakos3†‡ 1 Instituto de Astrof´ısica, Facultad de F´ısica, Pontificia Universidad Catolica´ de Chile, Av. Vicuna˜ Mackenna 4860, 7820436 Macul, Santiago, Chile Downloaded from https://academic.oup.com/mnras/article-abstract/467/1/971/2929275 by Princeton University user on 28 November 2018 2Millennium Institute of Astrophysics, Santiago, Chile 3Department of Astrophysical Sciences, Princeton University, Princeton, NJ 08544, USA Accepted 2017 January 17. Received 2017 January 13; in original form 2015 December 7 ABSTRACT We describe the Zonal Atmospheric Stellar Parameters Estimator (ZASPE), a new algorithm, and its associated code, for determining precise stellar atmospheric parameters and their uncertainties from high-resolution echelle spectra of FGK-type stars. ZASPE estimates stellar atmospheric parameters by comparing the observed spectrum against a grid of synthetic spectra only in the most sensitive spectral zones to changes in the atmospheric parameters. Realistic uncertainties in the parameters are computed from the data itself, by taking into account the systematic mismatches between the observed spectrum and the best-fitting synthetic one. The covariances between the parameters are also estimated in the process. ZASPE can in principle use any pre-calculated grid of synthetic spectra, but unbiased grids are required to obtain accurate parameters. We tested the performance of two existing libraries, and we concluded that neither is suitable for computing precise atmospheric parameters. -
The HR Diagram
Name_______________________ Class_______________________ Date_______________________ Assignment #10 – The H-R Diagram A star is a delicately balanced ball of gas, fighting between two impulses: gravity, which wants to squeeze the gas all down to a single point, and radiation pressure, which wants to blast all the gas out to infinity. These two opposite forces balance out in a process called Hydrostatic Equilibrium, and keep the gas at a stable, fairly constant size. The radiation itself is due to the fusion of protons in the star's core – a process that produces huge amounts of energy. In class we've examined the most important properties of stars: their temperatures, colors and brightnesses. Now let's see if we can find some relationships between these stellar properties. We know that hotter stars are brighter, as described by the Stefan-Boltzmann Law, and we know that the hotter stars are also bluer, as described by Wien's Law. The H-R diagram is a way of displaying an important relationship between a star's Absolute Magnitude (or Luminosity), and its Spectral Type (or temperature). Remember, Absolute Magnitude is how bright a star would appear to be, if it were 10 parsecs away. Luminosity is how much total energy a star gives off per second. As we studied in a previous exercise, Spectral Type is a system of classifying stars by temperature, from hottest (type O) to coldest (type M). Each letter in the Spectral Type list (O, B, A, F, G, K, and M) is further subdivided into 10 steps, numbered 0 through 9, to make finer distinctions between stars.