Bibliographies, As Submitted by the Departments of the Carnegie Institution for Science July 1, 2013, to June 31, 2014
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Clusters of Galaxies…
Budapest University, MTA-Eötvös François Mernier …and the surprisesoftheir spectacularhotatmospheres Clusters ofgalaxies… K complex ) ⇤ Fe ) α [email protected] - Wallon Super - Wallon [email protected] Fe XXVI (Ly (/ Fe XXIV) L complex ) ) (incl. Ne) α α ) Fe ) ) α ) α α ) ) ) ) α ⇥ ) ) ) α α α α α α Si XIV (Ly Mg XII (Ly Ni XXVII / XXVIII Fe XXV (He S XVI (Ly O VIII (Ly Si XIII (He S XV (He Ca XIX (He Ca XX (Ly Fe XXV (He Cr XXIII (He Ar XVII (He Ar XVIII (Ly Mn XXIV (He Ca XIX / XX Yo u are h ere ! 1 km = 103 m Yo u are h ere ! (somewhere behind…) 107 m Yo u are h ere ! (and this is the Moon) 109 m ≃3.3 light seconds Yo u are h ere ! 1012 m ≃55.5 light minutes 1013 m 1014 m Yo u are h ere ! ≃4 light days 1013 m Yo u are h ere ! 1014 m 1017 m ≃10.6 light years 1021 m Yo u are h ere ! ≃106 000 light years 1 million ly Yo u are h ere ! The Local Group Andromeda (M31) 1 million ly Yo u are h ere ! The Local Group Triangulum (M33) 1 million ly Yo u are h ere ! The Local Group 10 millions ly The Virgo Supercluster Virgo cluster 10 millions ly The Virgo Supercluster M87 Virgo cluster 10 millions ly The Virgo Supercluster 2dFGRS Survey The large scale structure of the universe Abell 2199 (429 000 000 light years) Abell 2029 (1.1 billion light years) Abell 2029 (1.1 billion light years) Abell 1689 Abell 1689 (2.2 billion light years) Les amas de galaxies 53 Light emits at optical “colors”… …but also in infrared, radio, …and X-ray! Light emits at optical “colors”… …but also in infrared, radio, …and X-ray! Light emits at optical “colors”… -
Breakthrough Propulsion Study Assessing Interstellar Flight Challenges and Prospects
Breakthrough Propulsion Study Assessing Interstellar Flight Challenges and Prospects NASA Grant No. NNX17AE81G First Year Report Prepared by: Marc G. Millis, Jeff Greason, Rhonda Stevenson Tau Zero Foundation Business Office: 1053 East Third Avenue Broomfield, CO 80020 Prepared for: NASA Headquarters, Space Technology Mission Directorate (STMD) and NASA Innovative Advanced Concepts (NIAC) Washington, DC 20546 June 2018 Millis 2018 Grant NNX17AE81G_for_CR.docx pg 1 of 69 ABSTRACT Progress toward developing an evaluation process for interstellar propulsion and power options is described. The goal is to contrast the challenges, mission choices, and emerging prospects for propulsion and power, to identify which prospects might be more advantageous and under what circumstances, and to identify which technology details might have greater impacts. Unlike prior studies, the infrastructure expenses and prospects for breakthrough advances are included. This first year's focus is on determining the key questions to enable the analysis. Accordingly, a work breakdown structure to organize the information and associated list of variables is offered. A flow diagram of the basic analysis is presented, as well as more detailed methods to convert the performance measures of disparate propulsion methods into common measures of energy, mass, time, and power. Other methods for equitable comparisons include evaluating the prospects under the same assumptions of payload, mission trajectory, and available energy. Missions are divided into three eras of readiness (precursors, era of infrastructure, and era of breakthroughs) as a first step before proceeding to include comparisons of technology advancement rates. Final evaluation "figures of merit" are offered. Preliminary lists of mission architectures and propulsion prospects are provided. -
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. -
SEEDS Direct Imaging of the RV-Detected Companion to V450
Draft version September 5, 2018 A Preprint typeset using LTEX style emulateapj v. 01/23/15 SEEDS DIRECT IMAGING OF THE RV-DETECTED COMPANION TO V450 ANDROMEDAE, AND CHARACTERIZATION OF THE SYSTEM. K. G. He lminiak1,2, M. Kuzuhara3,4,5, K. Mede6, T. D. Brandt7,8, R. Kandori4, T. Suenaga4,9, N. Kusakabe5, N. Narita5,4,9,6, J. C. Carson10, T. Currie1, T. Kudo1, J. Hashimoto5, L. Abe11, E. Akiyama4, W. Brandner12, M. Feldt12, M. Goto13, C. A. Grady14,15,16, O. Guyon1,17, Y. Hayano1, M. Hayashi4, S. S. Hayashi1,9, T. Henning12, K. W. Hodapp18, M. Ishii4, M. Iye4, M. Janson19, G. R. Knapp20, J. Kwon6, T. Matsuo21, M. W. McElwain14, S. Miyama22, J.-I. Morino4, A. Moro-Martin12,23, T. Nishimura1, T. Ryu9,4, T.-S. Pyo1, E. Serabyn24, H. Suto4,5, R. Suzuki4, Y. H. Takahashi6,4, M. Takami25, N. Takato1, H. Terada4, C. Thalmann26, E. L. Turner20,27, M. Watanabe28, J. Wisniewski29, T. Yamada30, H. Takami4, T. Usuda4, and M. Tamura6,4,5 Draft version September 5, 2018 ABSTRACT We report the direct imaging detection of a low-mass companion to a young, moderately active star V450 And, that was previously identified with the radial velocity method. The companion was found in high-contrast images obtained with the Subaru Telescope equipped with the HiCIAO camera and AO188 adaptive optics system. From the public ELODIE and SOPHIE archives we extracted available high-resolution spectra and radial velocity (RV) measurements, along with RVs from the Lick planet search program. We combined our multi-epoch astrometry with these archival, partially unpublished RVs, and found that the companion is a low-mass star, not a brown dwarf, as previously suggested. -
THE MASSIVELY ACCRETING CLUSTER A2029 Group Matches the Peak of the Photometric Galaxy Den- Sity Map
Last updated:August 3, 2018 A Preprint typeset using LTEX style emulateapj v. 12/16/11 THE MASSIVELY ACCRETING CLUSTER A2029 Jubee Sohn1, Margaret J. Geller1, Stephen A. Walker2, Ian Dell’Antonio3, Antonaldo Diaferio4,5, Kenneth J. Rines6 1 Smithsonian Astrophysical Observatory, 60 Garden Street, Cambridge, MA 02138, USA 2 Astrophysics Science Division, X-ray Astrophysics Laboratory, Code 662, NASA Goddard Space Flight Center, Greenbelt, MD 20771, USA 3 Department of Physics, Brown University, Box 1843, Providence, RI 02912, USA 4 Universit`adi Torino, Dipartimento di Fisica, Torino, Italy 5 Istituto Nazionale di Fisica Nucleare (INFN), Sezione di Torino, Torino, Italy and 6 Department of Physics and Astronomy, Western Washington University, Bellingham, WA 98225, USA Last updated:August 3, 2018 ABSTRACT We explore the structure of galaxy cluster Abell 2029 and its surroundings based on intensive spec- troscopy along with X-ray and weak lensing observations. The redshift survey includes 4376 galaxies (1215 spectroscopic cluster members) within 40′of the cluster center; the redshifts are included here. Two subsystems, A2033 and a Southern Infalling Group (SIG) appear in the infall region based on the spectroscopy as well as on the weak lensing and X-ray maps. The complete redshift survey of A2029 also identifies at least 12 foreground and background systems (10 are extended X-ray sources) in the A2029 field; we include a census of their properties. The X-ray luminosities (LX ) – velocity dispersions (σcl) scaling relations for A2029, A2033, SIG, and the foreground/background systems are consistent with the known cluster scaling relations. The combined spectroscopy, weak lensing, and X-ray observations provide a robust measure of the masses of A2029, A2033, and SIG. -
X-Ray Emission from a Merger Remnant, NGC 7252,The “Atoms-For-Peace” Galaxy
X-ray emission from a merger remnant, NGC 7252,the \Atoms-for-Peace" galaxy Hisamitsu Awaki Department of Physics, Faculty of Science, Ehime University Hironori Matsumoto1 Department of Earth and Space Science, Osaka University, and Hiroshi Tomida Space Utilization Research Program, National Space Development Agency of Japan, ABSTRACT We observed a nearby merger remnant NGC 7252 with the X-ray satellite ASCA, 13 1 2 and detected X-ray emission with the X-ray flux of (1.8 0.3) 10− ergs s− cm− in ± × 40 1 the 0.5–10 keV band. This corresponds to the X-ray luminosity of 8.1 10 ergs s− . The X-ray emission is well described with a two-component model: a soft× component with kT =0:72 0.13 keV and a hard component with kT > 5:1 keV. Although NGC 7252 is referred± to as a dynamically young protoelliptical, the 0.5–4 keV luminosity of 40 1 the soft component is about 2 10 ergs s− , which is low for an early-type galaxy. The × ratio of LX=LFIR suggests that the soft component originated from the hot gas due to star formation. Its low luminosity can be explained by the gas ejection from the galaxy as galaxy winds. Our observation reveals the existence of hard X-ray emission with the 40 1 2–10 keV luminosity of 5.6 10 ergs s− . This may indicate the existence of nuclear activity or intermediate-mass× black hole in NGC 7252. Subject headings: galaxies: evolution — galaxies: individual (NGC 7252) — X-rays: galaxies 1Center for Space Research, Massachusetts Institute of Technology, 77 Massachusetts Avenue, NE80-6045, Cambridge, MA02139-4307, USA 1 1. -
![Arxiv:1808.00476V1 [Astro-Ph.SR] 1 Aug 2018 Big Ae Stars but Not for Several Herbig Be Stars (Fairlamb Et Al](https://docslib.b-cdn.net/cover/2783/arxiv-1808-00476v1-astro-ph-sr-1-aug-2018-big-ae-stars-but-not-for-several-herbig-be-stars-fairlamb-et-al-672783.webp)
Arxiv:1808.00476V1 [Astro-Ph.SR] 1 Aug 2018 Big Ae Stars but Not for Several Herbig Be Stars (Fairlamb Et Al
Astronomy & Astrophysics manuscript no. Vioque_et_al_2018 c ESO 2018 August 3, 2018 Gaia DR2 study of Herbig Ae/Be stars M. Vioque1; 2?, R. D. Oudmaijer1, D. Baines3, I. Mendigutía4, and R. Pérez-Martínez2 1 School of Physics and Astronomy, University of Leeds, Leeds LS2 9JT, UK. 2 Ingeniería de Sistemas para la Defensa de España (Isdefe), XMM/Newton Science Operations Centre, ESA-ESAC Campus, PO Box 78, 28691 Villanueva de la Cañada, Madrid, Spain. 3 Quasar Science Resources for ESA-ESAC, ESAC Science Data Center, PO Box 78, 28691 Villanueva de la Cañada, Madrid, Spain. 4 Centro de Astrobiología (CSIC-INTA), Departamento de Astrofísica, ESA-ESAC Campus, PO Box 78, 28691 Villanueva de la Cañada, Madrid, Spain. Accepted for publication in Astronomy & Astrophysics. ABSTRACT Aims. We use Gaia Data Release 2 (DR2) to place 252 Herbig Ae/Be stars in the HR diagram and investigate their characteristics and properties. Methods. For all known Herbig Ae/Be stars with parallaxes in Gaia DR2, we collected their atmospheric parameters and photometric and extinction values from the literature. To these data we added near- and mid-infrared photometry, collected Hα emission line properties such as equivalent widths and line profiles, and their binarity status. In addition, we developed a photometric variability indicator from Gaia’s DR2 information. Results. We provide masses, ages, luminosities, distances, photometric variabilities and infrared excesses homogeneously derived for the most complete sample of Herbig Ae/Be stars to date. We find that high mass stars have a much smaller infrared excess and have much lower optical variabilities compared to lower mass stars, with the break at around 7M .Hα emission is generally correlated with infrared excess, with the correlation being stronger for infrared emission at wavelengths tracing the hot dust closest to the star. -
Understanding the H2/HI Ratio in Galaxies 3
Mon. Not. R. Astron. Soc. 394, 1857–1874 (2009) Printed 6 August 2021 (MN LATEX style file v2.2) Understanding the H2/HI Ratio in Galaxies D. Obreschkow and S. Rawlings Astrophysics, Department of Physics, University of Oxford, Keble Road, Oxford, OX1 3RH, UK Accepted 2009 January 12 ABSTRACT galaxy We revisit the mass ratio Rmol between molecular hydrogen (H2) and atomic hydrogen (HI) in different galaxies from a phenomenological and theoretical viewpoint. First, the local H2- mass function (MF) is estimated from the local CO-luminosity function (LF) of the FCRAO Extragalactic CO-Survey, adopting a variable CO-to-H2 conversion fitted to nearby observa- 5 1 tions. This implies an average H2-density ΩH2 = (6.9 2.7) 10− h− and ΩH2 /ΩHI = 0.26 0.11 ± · galaxy ± in the local Universe. Second, we investigate the correlations between Rmol and global galaxy properties in a sample of 245 local galaxies. Based on these correlations we intro- galaxy duce four phenomenological models for Rmol , which we apply to estimate H2-masses for galaxy each HI-galaxy in the HIPASS catalog. The resulting H2-MFs (one for each model for Rmol ) are compared to the reference H2-MF derived from the CO-LF, thus allowing us to determine the Bayesian evidence of each model and to identify a clear best model, in which, for spi- galaxy ral galaxies, Rmol negatively correlates with both galaxy Hubble type and total gas mass. galaxy Third, we derive a theoretical model for Rmol for regular galaxies based on an expression for their axially symmetric pressure profile dictating the degree of molecularization. -
Nd AAS Meeting Abstracts
nd AAS Meeting Abstracts 101 – Kavli Foundation Lectureship: The Outreach Kepler Mission: Exoplanets and Astrophysics Search for Habitable Worlds 200 – SPD Harvey Prize Lecture: Modeling 301 – Bridging Laboratory and Astrophysics: 102 – Bridging Laboratory and Astrophysics: Solar Eruptions: Where Do We Stand? Planetary Atoms 201 – Astronomy Education & Public 302 – Extrasolar Planets & Tools 103 – Cosmology and Associated Topics Outreach 303 – Outer Limits of the Milky Way III: 104 – University of Arizona Astronomy Club 202 – Bridging Laboratory and Astrophysics: Mapping Galactic Structure in Stars and Dust 105 – WIYN Observatory - Building on the Dust and Ices 304 – Stars, Cool Dwarfs, and Brown Dwarfs Past, Looking to the Future: Groundbreaking 203 – Outer Limits of the Milky Way I: 305 – Recent Advances in Our Understanding Science and Education Overview and Theories of Galactic Structure of Star Formation 106 – SPD Hale Prize Lecture: Twisting and 204 – WIYN Observatory - Building on the 308 – Bridging Laboratory and Astrophysics: Writhing with George Ellery Hale Past, Looking to the Future: Partnerships Nuclear 108 – Astronomy Education: Where Are We 205 – The Atacama Large 309 – Galaxies and AGN II Now and Where Are We Going? Millimeter/submillimeter Array: A New 310 – Young Stellar Objects, Star Formation 109 – Bridging Laboratory and Astrophysics: Window on the Universe and Star Clusters Molecules 208 – Galaxies and AGN I 311 – Curiosity on Mars: The Latest Results 110 – Interstellar Medium, Dust, Etc. 209 – Supernovae and Neutron -
THE KINEMATICS and AGES of STARS in GLIESE's CATALOGUE 1. Introduction This Contribution Gives Some Results on the Kinematics An
THE KINEMATICS AND AGES OF STARS IN GLIESE'S CATALOGUE R. WIELEN Astronomisches Rechen-Institut, Heidelberg, F.R.G. 1. Introduction This contribution gives some results on the kinematics and ages of stars near the Sun. These results are mainly based on the catalogue of nearby stars compiled by Gliese (1957, 1969 and minor recent modifications). Table I shows the number of objects under consideration. While the old catalogue (1957) contained only stars with distances r up to 20 pc, the new edition (1969) includes many stars with slightly larger distances. In Table I, a 'system' is either a single star or a binary or a multiple system. The number of systems with known space velocities nearer than 20 pc has increased by about 30% from 1957 to 1969. The first edition of Gliese's catalogue (1957) has been analyzed in detail by Gliese (1956) and von Hoerner (1960). TABLE I Gliese's Catalogue of Nearby Stars Number Edition 1969 1957 All j-s=20pc r<20 pc Stars 1890 1277 1095 Systems 1529 1036 916 Systems with known space velocity 1131 770 598 Although Gliese's catalogue is the most complete collection of stars within 20 pc, this sample of stars is severely biased by selection effects and is not fully representative for all the nearby stars. Only the stars brighter than M„~ +7 are almost completely known within 20 pc. For the fainter stars, the following selection effects occur: (a) The southern sky is deficient in detected faint nearby stars; (b) Since most of the faint nearby stars are found by their high proper motions, the sample is deficient in stars with small tangential components of their space velocities (measured with respect to the Sun); (c) Due to incomplete detection, the apparent space density of faint stars decreases rapidly with increasing distance r, and this effect becomes stronger with increasing M„. -
On the Habitability of Our Universe
Chapter for the book Consolidation of Fine Tuning On the Habitability of Our Universe Abraham Loeb Astronomy department, Harvard University, 60 Garden Street, Cambridge, MA 02138, USA E-mail: [email protected] Abstract. Is life most likely to emerge at the present cosmic time near a star like the Sun? We consider the habitability of the Universe throughout cosmic history, and conservatively restrict our attention to the context of “life as we know it” and the standard cosmological model, ΛCDM. The habitable cosmic epoch started shortly after the first stars formed, about 30 Myr after the Big Bang, and will end about 10 Tyr from now, when all stars will die. We review the formation history of habitable planets and find that unless habitability around low mass stars is suppressed, life is most likely to exist near ∼ 0.1M stars ten trillion years from now. Spectroscopic searches for biosignatures in the atmospheres of transiting Earth-mass planets around low mass stars will determine whether present-day life is indeed premature or typical from a cosmic perspective. arXiv:1606.08926v2 [astro-ph.CO] 24 Nov 2016 Contents 1 Introduction2 2 The Habitable Epoch of the Early Universe4 2.1 Section Background4 2.2 First Planets4 2.3 Section Summary and Implications5 3 CEMP Stars: Possible Hosts to Carbon Planets in the Early Universe6 3.1 Section Background6 3.2 Star-forming environment of CEMP stars7 3.3 Orbital Radii of Potential Carbon Planets9 3.4 Mass-Radius Relationship for Carbon Planets 13 3.5 Section Summary and Implications 15 4 Water -
Planet Formation Phil Armitage
Planet Formation Phil Armitage Colorado è Stony Brook / Simons CCA overview • stone age planet formation – formation of planetary systems from a smooth radial distribution of km-scale planetesimals embedded in gas, with no migration • planetesimal • planetesimals formation or pebbles? • migration • gas accretion How do we form observed systems? Is there a timing problem? classical planet formation Adopt effective initial conditions: radially smooth distribution of small (100m – km) planetesimals embedded in gas, which acts to damp {e,i} but does not cause migration • growth phases: runaway, oligarchic final assembly / giant impacts • if fast enough final outcome is ~determined by stability M 1/3 r = p a Hill 3M ✓ ⇤ ◆ 1/4 tinstability = f(∆a/Mp ) • collisions make a small-N system more stable classical planet formation t / Myr 100 Ratio of collisions to scatterings is 10 f(vK / vesc), favors collisions for MSun at a ~ AU and less 1 “in situ” formation e 1 AU 2 AU 3 AU • disk with a few ME / AU at 1 AU will work • requirement of stability can hide a multitude of sins • many important but lesser constraints (small mass of Mars…) classical planet formation quasi-static envelope extends to rHill, rBondi core grows from accretion of planetesimals cooling is limited by grain opacity in radiative zone in the envelope “success” requires reaching Menv ~ Mcore ~ 5-20 ME within gas disk lifetime possible at few AU if the gravitational focusing factor 2 [1 + (vesc / σ) ] is large (small planetesimals) and κ low what’s wrong with this story? • major