Accretion Disks Around Stars and the Process of Planet Formation
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Exploring Exoplanet Populations with NASA's Kepler Mission
SPECIAL FEATURE: PERSPECTIVE PERSPECTIVE SPECIAL FEATURE: Exploring exoplanet populations with NASA’s Kepler Mission Natalie M. Batalha1 National Aeronautics and Space Administration Ames Research Center, Moffett Field, 94035 CA Edited by Adam S. Burrows, Princeton University, Princeton, NJ, and accepted by the Editorial Board June 3, 2014 (received for review January 15, 2014) The Kepler Mission is exploring the diversity of planets and planetary systems. Its legacy will be a catalog of discoveries sufficient for computing planet occurrence rates as a function of size, orbital period, star type, and insolation flux.The mission has made significant progress toward achieving that goal. Over 3,500 transiting exoplanets have been identified from the analysis of the first 3 y of data, 100 planets of which are in the habitable zone. The catalog has a high reliability rate (85–90% averaged over the period/radius plane), which is improving as follow-up observations continue. Dynamical (e.g., velocimetry and transit timing) and statistical methods have confirmed and characterized hundreds of planets over a large range of sizes and compositions for both single- and multiple-star systems. Population studies suggest that planets abound in our galaxy and that small planets are particularly frequent. Here, I report on the progress Kepler has made measuring the prevalence of exoplanets orbiting within one astronomical unit of their host stars in support of the National Aeronautics and Space Admin- istration’s long-term goal of finding habitable environments beyond the solar system. planet detection | transit photometry Searching for evidence of life beyond Earth is the Sun would produce an 84-ppm signal Translating Kepler’s discovery catalog into one of the primary goals of science agencies lasting ∼13 h. -
Formation of TRAPPIST-1
EPSC Abstracts Vol. 11, EPSC2017-265, 2017 European Planetary Science Congress 2017 EEuropeaPn PlanetarSy Science CCongress c Author(s) 2017 Formation of TRAPPIST-1 C.W Ormel, B. Liu and D. Schoonenberg University of Amsterdam, The Netherlands ([email protected]) Abstract start to drift by aerodynamical drag. However, this growth+drift occurs in an inside-out fashion, which We present a model for the formation of the recently- does not result in strong particle pileups needed to discovered TRAPPIST-1 planetary system. In our sce- trigger planetesimal formation by, e.g., the streaming nario planets form in the interior regions, by accre- instability [3]. (a) We propose that the H2O iceline (r 0.1 au for TRAPPIST-1) is the place where tion of mm to cm-size particles (pebbles) that drifted ice ≈ the local solids-to-gas ratio can reach 1, either by from the outer disk. This scenario has several ad- ∼ vantages: it connects to the observation that disks are condensation of the vapor [9] or by pileup of ice-free made up of pebbles, it is efficient, it explains why the (silicate) grains [2, 8]. Under these conditions plan- TRAPPIST-1 planets are Earth mass, and it provides etary embryos can form. (b) Due to type I migration, ∼ a rationale for the system’s architecture. embryos cross the iceline and enter the ice-free region. (c) There, silicate pebbles are smaller because of col- lisional fragmentation. Nevertheless, pebble accretion 1. Introduction remains efficient and growth is fast [6]. (d) At approx- TRAPPIST-1 is an M8 main-sequence star located at a imately Earth masses embryos reach their pebble iso- distance of 12 pc. -
Water, Habitability, and Detectability Steve Desch
Water, Habitability, and Detectability Steve Desch PI, “Exoplanetary Ecosystems” NExSS team School of Earth and Space Exploration, Arizona State University with Ariel Anbar, Tessa Fisher, Steven Glaser, Hilairy Hartnett, Stephen Kane, Susanne Neuer, Cayman Unterborn, Sara Walker, Misha Zolotov Astrobiology Science Strategy NAS Committee, Beckmann Center, Irvine, CA (remotely), January 17, 2018 How to look for life on (Earth-like) exoplanets: find oxygen in their atmospheres How Earth-like must an exoplanet be for this to work? Seager et al. (2013) How to look for life on (Earth-like) exoplanets: find oxygen in their atmospheres Oxygen on Earth overwhelmingly produced by photosynthesizing life, which taps Sun’s energy and yields large disequilibrium signature. Caveats: Earth had life for billions of years without O2 in its atmosphere. First photosynthesis to evolve on Earth was anoxygenic. Many ‘false positives’ recognized because O2 has abiotic sources, esp. photolysis (Luger & Barnes 2014; Harman et al. 2015; Meadows 2017). These caveats seem like exceptions to the ‘rule’ that ‘oxygen = life’. How non-Earth-like can an exoplanet be (especially with respect to water content) before oxygen is no longer a biosignature? Part 1: How much water can terrestrial planets form with? Part 2: Are Aqua Planets or Water Worlds habitable? Can we detect life on them? Part 3: How should we look for life on exoplanets? Part 1: How much water can terrestrial planets form with? Theory says: up to hundreds of oceans’ worth of water Trappist-1 system suggests hundreds of oceans, especially around M stars Many (most?) planets may be Aqua Planets or Water Worlds How much water can terrestrial planets form with? Earth- “snow line” Standard Sun distance models of distance accretion suggest abundant water. -
Curriculum Vitae - 24 March 2020
Dr. Eric E. Mamajek Curriculum Vitae - 24 March 2020 Jet Propulsion Laboratory Phone: (818) 354-2153 4800 Oak Grove Drive FAX: (818) 393-4950 MS 321-162 [email protected] Pasadena, CA 91109-8099 https://science.jpl.nasa.gov/people/Mamajek/ Positions 2020- Discipline Program Manager - Exoplanets, Astro. & Physics Directorate, JPL/Caltech 2016- Deputy Program Chief Scientist, NASA Exoplanet Exploration Program, JPL/Caltech 2017- Professor of Physics & Astronomy (Research), University of Rochester 2016-2017 Visiting Professor, Physics & Astronomy, University of Rochester 2016 Professor, Physics & Astronomy, University of Rochester 2013-2016 Associate Professor, Physics & Astronomy, University of Rochester 2011-2012 Associate Astronomer, NOAO, Cerro Tololo Inter-American Observatory 2008-2013 Assistant Professor, Physics & Astronomy, University of Rochester (on leave 2011-2012) 2004-2008 Clay Postdoctoral Fellow, Harvard-Smithsonian Center for Astrophysics 2000-2004 Graduate Research Assistant, University of Arizona, Astronomy 1999-2000 Graduate Teaching Assistant, University of Arizona, Astronomy 1998-1999 J. William Fulbright Fellow, Australia, ADFA/UNSW School of Physics Languages English (native), Spanish (advanced) Education 2004 Ph.D. The University of Arizona, Astronomy 2001 M.S. The University of Arizona, Astronomy 2000 M.Sc. The University of New South Wales, ADFA, Physics 1998 B.S. The Pennsylvania State University, Astronomy & Astrophysics, Physics 1993 H.S. Bethel Park High School Research Interests Formation and Evolution -
Formation of the Solar System (Chapter 8)
Formation of the Solar System (Chapter 8) Based on Chapter 8 • This material will be useful for understanding Chapters 9, 10, 11, 12, 13, and 14 on “Formation of the solar system”, “Planetary geology”, “Planetary atmospheres”, “Jovian planet systems”, “Remnants of ice and rock”, “Extrasolar planets” and “The Sun: Our Star” • Chapters 2, 3, 4, and 7 on “The orbits of the planets”, “Why does Earth go around the Sun?”, “Momentum, energy, and matter”, and “Our planetary system” will be useful for understanding this chapter Goals for Learning • Where did the solar system come from? • How did planetesimals form? • How did planets form? Patterns in the Solar System • Patterns of motion (orbits and rotations) • Two types of planets: Small, rocky inner planets and large, gas outer planets • Many small asteroids and comets whose orbits and compositions are similar • Exceptions to these patterns, such as Earth’s large moon and Uranus’s sideways tilt Help from Other Stars • Use observations of the formation of other stars to improve our theory for the formation of our solar system • Use this theory to make predictions about the formation of other planetary systems Nebular Theory of Solar System Formation • A cloud of gas, the “solar nebula”, collapses inwards under its own weight • Cloud heats up, spins faster, gets flatter (disk) as a central star forms • Gas cools and some materials condense as solid particles that collide, stick together, and grow larger Where does a cloud of gas come from? • Big Bang -> Hydrogen and Helium • First stars use this -
University of Groningen Evaluating Galactic Habitability Using High
University of Groningen Evaluating galactic habitability using high-resolution cosmological simulations of galaxy formation Forgan, Duncan; Dayal, Pratika; Cockell, Charles; Libeskind, Noam Published in: International Journal of Astrobiology DOI: 10.1017/S1473550415000518 IMPORTANT NOTE: You are advised to consult the publisher's version (publisher's PDF) if you wish to cite from it. Please check the document version below. Document Version Final author's version (accepted by publisher, after peer review) Publication date: 2017 Link to publication in University of Groningen/UMCG research database Citation for published version (APA): Forgan, D., Dayal, P., Cockell, C., & Libeskind, N. (2017). Evaluating galactic habitability using high- resolution cosmological simulations of galaxy formation. International Journal of Astrobiology, 16(1), 60–73. https://doi.org/10.1017/S1473550415000518 Copyright Other than for strictly personal use, it is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), unless the work is under an open content license (like Creative Commons). The publication may also be distributed here under the terms of Article 25fa of the Dutch Copyright Act, indicated by the “Taverne” license. More information can be found on the University of Groningen website: https://www.rug.nl/library/open-access/self-archiving-pure/taverne- amendment. Take-down policy If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. Downloaded from the University of Groningen/UMCG research database (Pure): http://www.rug.nl/research/portal. -
Pulsar Physics Without Magnetars
Chin. J. Astron. Astrophys. Vol.8 (2008), Supplement, 213–218 Chinese Journal of (http://www.chjaa.org) Astronomy and Astrophysics Pulsar Physics without Magnetars Wolfgang Kundt Argelander-Institut f¨ur Astronomie der Universit¨at, Auf dem H¨ugel 71, D-53121 Bonn, Germany Abstract Magnetars, as defined some 15 yr ago, are inconsistent both with fundamental physics, and with the (by now) two observed upward jumps of the period derivatives (of two of them). Instead, the class of peculiar X-ray sources commonly interpreted as magnetars can be understood as the class of throttled pulsars, i.e. of pulsars strongly interacting with their CSM. This class is even expected to harbour the sources of the Cosmic Rays, and of all the (extraterrestrial) Gamma-Ray Bursts. Key words: magnetars — throttled pulsars — dying pulsars — cavity — low-mass disk 1 DEFINITION AND PROPERTIES OF THE MAGNETARS Magnetars have been defined by Duncan and Thompson some 15 years ago, as spinning, compact X-ray sources - probably neutron stars - which are powered by the slow decay of their strong magnetic field, of strength 1015 G near the surface, cf. (Duncan & Thompson 1992; Thompson & Duncan 1996). They are now thought to comprise the anomalous X-ray pulsars (AXPs), soft gamma-ray repeaters (SGRs), recurrent radio transients (RRATs), or ‘stammerers’, or ‘burpers’, and the ‘dim isolated neutron stars’ (DINSs), i.e. a large, fairly well defined subclass of all neutron stars, which has the following properties (Mereghetti et al. 2002): 1) They are isolated neutron stars, with spin periods P between 5 s and 12 s, and similar glitch behaviour to other neutron-star sources, which correlates with their X-ray bursting. -
New Herbig-Haro Objects in the L1617 and L1646 Dark Clouds
A&A 437, 169–175 (2005) Astronomy DOI: 10.1051/0004-6361:20052769 & c ESO 2005 Astrophysics New Herbig-Haro objects in the L1617 and L1646 dark clouds H. Wang1,2, B. Stecklum3, and Th. Henning2 1 Purple Mountain Observatory, Academia Sinica, Nanjing 210008, PR China e-mail: [email protected] 2 Max-Planck-Institut für Astronomie, Königstuhl 17, 69117 Heidelberg, Germany e-mail: [email protected] 3 Thüringer Landessternwarte Tautenburg, Sternwarte 5, 07778 Tautenburg, Germany e-mail: [email protected] Received 26 January 2005 / Accepted 25 February 2005 Abstract. Optical imaging towards L1617 and L1646 revealed three new Herbig-Haro (HH) objects, HH 182, 439, and 866. Spectroscopic observations of HH 182 A and 439 A confirmed their HH object nature. Molecular hydrogen v = 1–0 S(1) narrow band imaging revealed three H2 emission features in the HH 182 region which coincide with the optical emission. Based on the position angles of the different parts of the HH 111 flow and that of HH 182, HH 182 may be the outermost southeastern part of the giant HH 111 flow. One deeply embedded star is revealed in our near-infrared imaging of the HH 439 region. HH 439 A and the associated bow shock are probably driven by the newly detected embedded star. HH 439 B-D are probably driven by the Herbig AeBe star candidate GSC 04794-00827 (IRAS 06045-0554). The embedded source IRAS 06046-0603 is identified to be the exciting source of HH 866. Key words. Herbig-Haro objects – ISM: jets and outflows – ISM: individual objects: L1617 – ISM: individual objects: L1646 – stars: formation 1. -
Progenitors of Magnetars and Hyperaccreting Magnetized Disks
Feeding Compact Objects: Accretion on All Scales Proceedings IAU Symposium No. 290, 2012 c International Astronomical Union 2013 C. M. Zhang, T. Belloni, M. M´endez & S. N. Zhang, eds. doi:10.1017/S1743921312020340 Progenitors of Magnetars and Hyperaccreting Magnetized Disks Y. Xie1 andS.N.Zhang1,2 1 National Astronomical Observatories, Chinese Academy Of Sciences, Beijing, 100012, P. R.China email: [email protected] 2 Key Laboratory of Particle Astrophysics, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing, 100012, P. R. China email: [email protected] Abstract. We propose that a magnetar could be formed during the core collapse of massive stars or coalescence of two normal neutron stars, through collecting and inheriting the magnetic fields magnified by hyperaccreting disk. After the magnetar is born, its dipole magnetic fields in turn have a major influence on the following accretion. The decay of its toroidal field can fuel the persistent X-ray luminosity of either an SGR or AXP; however the decay of only the poloidal field is insufficient to do so. Keywords. Magnetar, accretion disk, gamma ray bursts, magnetic fields 1. Introduction Neutron stars (NSs) with magnetic field B stronger than the quantum critical value, 2 3 13 Bcr = m c /e ≈ 4.4 × 10 G, are called magnetars. Observationally, a magnetar may appear as a soft gamma-ray repeater (SGR) or an anomalous X-ray pulsar (AXP). It is believed that its persistent X-ray luminosity is powered by the consumption of their B- decay energy (e.g. Duncan & Thompson 1992; Paczynski 1992). However, the formation of strong B of a magnetar remains unresolved, and the possible explanations are divided into three classes: (i) B is generated by a convective dynamo (Duncan & Thompson 1992); (ii) B is essentially of fossil origin (e.g. -
Testing Quantum Gravity with LIGO and VIRGO
Testing Quantum Gravity with LIGO and VIRGO Marek A. Abramowicz1;2;3, Tomasz Bulik4, George F. R. Ellis5 & Maciek Wielgus1 1Nicolaus Copernicus Astronomical Center, ul. Bartycka 18, 00-716, Warszawa, Poland 2Physics Department, Gothenburg University, 412-96 Goteborg, Sweden 3Institute of Physics, Silesian Univ. in Opava, Bezrucovo nam. 13, 746-01 Opava, Czech Republic 4Astronomical Observatory Warsaw University, 00-478 Warszawa, Poland 5Mathematics Department, University of Cape Town, Rondebosch, Cape Town 7701, South Africa We argue that if particularly powerful electromagnetic afterglows of the gravitational waves bursts detected by LIGO-VIRGO will be observed in the future, this could be used as a strong observational support for some suggested quantum alternatives for black holes (e.g., firewalls and gravastars). A universal absence of such powerful afterglows should be taken as a sug- gestive argument against such hypothetical quantum-gravity objects. If there is no matter around, an inspiral-type coalescence (merger) of two uncharged black holes with masses M1, M2 into a single black hole with the mass M3 results in emission of grav- itational waves, but no electromagnetic radiation. The maximal amount of the gravitational wave 2 energy E=c = (M1 + M2) − M3 that may be radiated from a merger was estimated by Hawking [1] from the condition that the total area of all black hole horizons cannot decrease. Because the 2 2 2 horizon area is proportional to the square of the black hole mass, one has M3 > M2 + M1 . In the 1 1 case of equal initial masses M1 = M2 = M, this yields [ ], E 1 1 h p i = [(M + M ) − M ] < 2M − 2M 2 ≈ 0:59: (1) Mc2 M 1 2 3 M From advanced numerical simulations (see, e.g., [2–4]) one gets, in the case of comparable initial masses, a much more stringent energy estimate, ! EGRAV 52 M 2 ≈ 0:03; meaning that EGRAV ≈ 1:8 × 10 [erg]: (2) Mc M The estimate assumes validity of Einstein’s general relativity. -
MHD Accretion Disk Winds: the Key to AGN Phenomenology?
galaxies Review MHD Accretion Disk Winds: The Key to AGN Phenomenology? Demosthenes Kazanas NASA/Goddard Space Flight Center, 8800 Greenbelt Rd, Greenbelt, MD 20771, USA; [email protected]; Tel.: +1-301-286-7680 Received: 8 November 2018; Accepted: 4 January 2019; Published: 10 January 2019 Abstract: Accretion disks are the structures which mediate the conversion of the kinetic energy of plasma accreting onto a compact object (assumed here to be a black hole) into the observed radiation, in the process of removing the plasma’s angular momentum so that it can accrete onto the black hole. There has been mounting evidence that these structures are accompanied by winds whose extent spans a large number of decades in radius. Most importantly, it was found that in order to satisfy the winds’ observational constraints, their mass flux must increase with the distance from the accreting object; therefore, the mass accretion rate on the disk must decrease with the distance from the gravitating object, with most mass available for accretion expelled before reaching the gravitating object’s vicinity. This reduction in mass flux with radius leads to accretion disk properties that can account naturally for the AGN relative luminosities of their Optical-UV and X-ray components in terms of a single parameter, the dimensionless mass accretion rate. Because this critical parameter is the dimensionless mass accretion rate, it is argued that these models are applicable to accreting black holes across the mass scale, from galactic to extragalactic. Keywords: accretion disks; MHD winds; accreting black holes 1. Introduction-Accretion Disk Phenomenology Accretion disks are the generic structures associated with compact objects (considered to be black holes in this note) powered by matter accretion onto them. -
Chapter 9 Accretion Disks for Beginners
Chapter 9 Accretion Disks for Beginners When the gas being accreted has high angular momentum, it generally forms an accretion disk. If the gas conserves angular momentum but is free to radiate energy, it will lose energy until it is on a circular orbit of radius 2 Rc = j /(GM), where j is the specific angular momentum of the gas, and M is the mass of the accreting compact object. The gas will only be able to move inward from this radius if it disposes of part of its angular momentum. In an accretion disk, angular momentum is transferred by viscous torques from the inner regions of the disk to the outer regions. The importance of accretion disks was first realized in the study of binary stellar systems. Suppose that a compact object of mass Mc and a ‘normal’ star of mass Ms are separated by a distance a. The normal star (a main- sequence star, a giant, or a supergiant) is the source of the accreted matter, and the compact object is the body on which the matter accretes. If the two bodies are on circular orbits about their center of mass, their angular velocity will be 1/2 ~ G(Mc + Ms) Ω= 3 eˆ , (9.1) " a # wheree ˆ is the unit vector normal to the orbital plane. In a frame of reference that is corotating with the two stars, the equation of momentum conservation has the form ∂~u 1 +(~u · ∇~ )~u = − ∇~ P − 2Ω~ × ~u − ∇~ Φ , (9.2) ∂t ρ R 89 90 CHAPTER 9. ACCRETION DISKS FOR BEGINNERS Figure 9.1: Sections in the orbital plane of equipotential surfaces, for a binary with q = 0.2.