Col-Ossos: Z-Band Photometry Reveals Three Distinct Tno Surface Types Identifying Cold Classical Tno Surfaces
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Col-OSSOS: Compositional Homogeneity of Three Kuiper Belt Binaries Michael Marsset, Wesley Fraser, Michele Bannister, Megan Schwamb, Rosemary Pike, Susan Benecchi, J
Col-OSSOS: Compositional Homogeneity of Three Kuiper Belt Binaries Michael Marsset, Wesley Fraser, Michele Bannister, Megan Schwamb, Rosemary Pike, Susan Benecchi, J. Kavelaars, Mike Alexandersen, Ying-Tung Chen, Brett Gladman, et al. To cite this version: Michael Marsset, Wesley Fraser, Michele Bannister, Megan Schwamb, Rosemary Pike, et al.. Col- OSSOS: Compositional Homogeneity of Three Kuiper Belt Binaries. The Planetary Science Journal, IOP Science, 2020, 1 (1), pp.16. 10.3847/PSJ/ab8cc0. hal-02884321 HAL Id: hal-02884321 https://hal.archives-ouvertes.fr/hal-02884321 Submitted on 17 Dec 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Distributed under a Creative Commons Attribution| 4.0 International License The Planetary Science Journal, 1:16 (9pp), 2020 June https://doi.org/10.3847/PSJ/ab8cc0 © 2020. The Author(s). Published by the American Astronomical Society. Col-OSSOS: Compositional Homogeneity of Three Kuiper Belt Binaries Michaël Marsset1,2 , Wesley C. Fraser2 , Michele T. Bannister3 , Megan E. Schwamb2,4 , Rosemary E Pike5,6 , -
Guide to the Extended Versions of MPC Data Files Based on the MPCORB Format
Guide to the Extended Versions of MPC Data Files Based on the MPCORB Format Last updated: 2016/04/19 by J.L. Galache Introduction The Minor Planet Center (MPC) has been providing the orbits of minor planets in the form of a file, MPCORB.DAT, since the mid '90s (1990s, not 1890s). Back then there were only a few thousand known asteroids, compared to the several hundred thousand of today, so a flat text file was the appropriate way to circulate these data. It was also a time when most orbit computations were programmed in Fortran, which ingested data no other way. MPCORB.DAT has therefore always been, and continues to be, a fixed-width file (see Table 1 for the current format description1). In fact, all original data files available on the MPC website are flat text files (even the orbits files provided for planetarium-type/sky simulation software packages are simply text files of varying format2). In the early years of the 2010s, possibly due to the rising popularity of the scripting language Python amongst astronomers, and an increased interest from developers wanting to write asteroid-themed tools, requests were received to provide data in other, easier to parse formats, e.g., JSON, CSV, SQL, etc. At the same time, astronomers and developers alike wanted more information than was currently been provided in MPCORB.DAT; information that did exist on the MPC website in other, often hard to find, files. Here was an opportunity to add some new data to existing files, while also making them available in other formats. -
1 Resonant Kuiper Belt Objects
Resonant Kuiper Belt Objects - a Review Renu Malhotra Lunar and Planetary Laboratory, The University of Arizona, Tucson, AZ, USA Email: [email protected] Abstract Our understanding of the history of the solar system has undergone a revolution in recent years, owing to new theoretical insights into the origin of Pluto and the discovery of the Kuiper belt and its rich dynamical structure. The emerging picture of dramatic orbital migration of the planets driven by interaction with the primordial Kuiper belt is thought to have produced the final solar system architecture that we live in today. This paper gives a brief summary of this new view of our solar system's history, and reviews the astronomical evidence in the resonant populations of the Kuiper belt. Introduction Lying at the edge of the visible solar system, observational confirmation of the existence of the Kuiper belt came approximately a quarter-century ago with the discovery of the distant minor planet (15760) Albion (formerly 1992 QB1, Jewitt & Luu 1993). With the clarity of hindsight, we now recognize that Pluto was the first discovered member of the Kuiper belt. The current census of the Kuiper belt includes more than 2000 minor planets at heliocentric distances between ~30 au and ~50 au. Their orbital distribution reveals a rich dynamical structure shaped by the gravitational perturbations of the giant planets, particularly Neptune. Theoretical analysis of these structures has revealed a remarkable dynamic history of the solar system. The story is as follows (see Fernandez & Ip 1984, Malhotra 1993, Malhotra 1995, Fernandez & Ip 1996, and many subsequent works). -
The Minor Planets
The Minor Planets Swinburne Astronomy Online 3D PDF c SAO 2012 The Minor Planets c Swinburne Astronomy Online 2012 1 Description 1.1 Minor planets Our view of the Solar System has changed dramatically over the past 15 years with the discovery of new classes of small bodies. Mi- nor planets are another name for asteroids, or celestial bodies that orbit the Sun that are not otherwise classed as planets or comets. Generally, minor planets are relatively small rocky bodies, while comets are icy bodies that become active when their orbits carry them close to the Sun. (An \active" comet exhibits a large coma and a long tail.) The minor planets can be classified by their orbital characteristics. In this 3D PDF, we have included 5 classes of minor planets: (1) the Near Earth Asteroids (NEAs), (2) the main belt asteroids, (3) the Trojan asteroids of Jupiter, (4) the Centaurs, and (5) the Trans-Neptunian Objects (TNOs). The dataset used comes from the Minor Planets Centre. As of 19 November 2012, there were 9,346 NEAs (comprising 732 Atens, 4686 Apollos and 3928 Amors); 581,613 main belt asteroids; 5,407 jovian Trojans; 330 Centaurs; and 1,150 TNOs. (Note than in this 3D PDF, we have only included 11,678 main belt asteroids.) • The Near Earth Asteroids have perihelion distances of less than 1.3 AU, and include the following sub-classes: { Atens have aphelion distances greater than 0.983 AU, and semi-major axes less than 1 AU { Apollos have perihelion distances less than 1.017 AU, and semi-major axes greater than 1 AU { Amors have perihelion distances between 1.017 and 1.3 AU and semi-major axes greater than 1 AU • The main belt asteroids reside between the orbits of Mars and Jupiter, with most of the asteroids orbiting between about 2.1 AU and 3.3 AU. -
Template for Two-Page Abstracts in Word 97 (PC)
3rd WORKSHOP ON BINARIES IN THE SOLAR SYSTEM Hawaii, the Big Island (USA). June 30 – July 2, 2013 POPULATION OF SMALL ASTEROID SYSTEMS - WE ARE STILL IN A SURVEY PHASE. P. Pravec, P. Scheirich, P. Kušnirák, K. Hornoch, A. Galád, Astronomical Institute AS CR, Fričova 298, 251 65 Ondřejov, Czech Republic, [email protected]. Introduction: Despite major achievements ob- tively. Arlon and (32039) both show two rotational tained during the past 15 years, our knowledge of the lightcurve components with shorter periods (5.15 and population and properties of small binary and multiple 18.2 h for Arlon, and 3.3 or 6.6 and 11.1 h for 32039), asteroid systems is still far from advanced. There is a but Iwamoto shows what appears to be a synchronous numerous indirect evidence that most small asteroid rotation lightcurve - very curious, considering its esti- systems were formed by rotational fission of cohesion- mated tidal synchronization time much longer than the less parent asteroids that were spun up to the critical age of the Solar System. The satellites of all the three frequency presumably by YORP, but details of the systems are large, with D2/D1 between 0.5 and 1. Have process are lacking. Furthermore, as we proceed with the three unusual systems been formed by rotational observations of more and more asteroids, we find new fission like the majority of (closer) systems with typi- significant things that we did not know before. We will cally smaller satellites that we predominantly observe? review a few such observations. How were they moved to their current relatively wide Primaries of asteroid pairs being binary (or ter- orbits? Given their placement in the Hic sunt leones nary) themselves: The case of (3749) Balam was gap of the Porb-D1 space where both the photometric identified by Vokrouhlický [1, and references therein] . -
The Onset of Chaos in Permanently Deformed Binaries from Spin–Orbit and Spin–Spin Coupling
The Astrophysical Journal, 913:31 (19pp), 2021 May 20 https://doi.org/10.3847/1538-4357/abf248 © 2021. The American Astronomical Society. All rights reserved. The Onset of Chaos in Permanently Deformed Binaries from Spin–Orbit and Spin–Spin Coupling Darryl Seligman1 and Konstantin Batygin2 1 Dept. of the Geophysical Sciences, University of Chicago, Chicago, IL 60637, USA; [email protected] 2 Division of Geological and Planetary Sciences, Caltech, Pasadena, CA 91125, USA Received 2020 September 16; revised 2021 March 22; accepted 2021 March 24; published 2021 May 21 Abstract Permanently deformed objects in binary systems can experience complex rotation evolution, arising from the extensively studied effect of spin–orbit coupling as well as more nuanced dynamics arising from spin–spin interactions. The ability of an object to sustain an aspheroidal shape largely determines whether or not it will exhibit nontrivial rotational behavior. In this work, we adopt a simplified model of a gravitationally interacting primary and satellite pair, where each body’s quadrupole moment is approximated by two diametrically opposed point masses. After calculating the net gravitational torque on the satellite from the primary, as well as the associated equations of motion, we employ a Hamiltonian formalism that allows for a perturbative treatment of the spin–orbit and retrograde and prograde spin–spin coupling states. By analyzing the resonances individually and collectively, we determine the criteria for resonance overlap and the onset of chaos, as a function of orbital and geometric properties of the binary. We extend the 2D planar geometry to calculate the obliquity evolution. This calculation indicates that satellites in spin–spin resonances undergo precession when inclined out of the plane, but they do not tumble. -
Col-OSSOS: Colors of the Interstellar Planetesimal 1I/Oumuamua
DRAFT VERSION DECEMBER 7, 2017 Typeset using LATEX twocolumn style in AASTeX61 COL-OSSOS: COLORS OF THE INTERSTELLAR PLANETESIMAL 1I/‘OUMUAMUA MICHELE T. BANNISTER,1 MEGAN E. SCHWAMB,2 WESLEY C. FRASER,1 MICHAEL MARSSET,1 ALAN FITZSIMMONS,1 SUSAN D. BENECCHI,3 PEDRO LACERDA,1 ROSEMARY E. PIKE,4 J. J. KAVELAARS,5, 6 ADAM B. SMITH,2 SUNNY O. STEWART,2 SHIANG-YU WANG,7 AND MATTHEW J. LEHNER7, 8, 9 1Astrophysics Research Centre, School of Mathematics and Physics, Queen’s University Belfast, Belfast BT7 1NN, United Kingdom 2Gemini Observatory, Northern Operations Center, 670 North A’ohoku Place, Hilo, HI 96720, USA 3Planetary Science Institute, 1700 East Fort Lowell, Suite 106, Tucson, AZ 85719, USA 4Institute for Astronomy and Astrophysics, Academia Sinica; 11F AS/NTU, National Taiwan University, 1 Roosevelt Rd., Sec. 4, Taipei 10617, Taiwan 5Herzberg Astronomy and Astrophysics Research Centre, National Research Council of Canada, 5071 West Saanich Rd, Victoria, British Columbia V9E 2E7, Canada 6Department of Physics and Astronomy, University of Victoria, Elliott Building, 3800 Finnerty Rd, Victoria, BC V8P 5C2, Canada 7Institute of Astronomy and Astrophysics, Academia Sinica; 11F of AS/NTU Astronomy-Mathematics Building, Nr. 1 Roosevelt Rd., Sec. 4, Taipei 10617, Taiwan 8Department of Physics and Astronomy, University of Pennsylvania, 209 S. 33rd St., Philadelphia, PA 19104, USA 9Harvard-Smithsonian Center for Astrophysics, 60 Garden St., Cambridge, MA 02138, USA (Received 2017 November 16; Revised 2017 December 4; Accepted 2017 December 6) Submitted to ApJL ABSTRACT The recent discovery by Pan-STARRS1 of 1I/2017 U1 (‘Oumuamua), on an unbound and hyperbolic orbit, offers a rare oppor- tunity to explore the planetary formation processes of other stars, and the effect of the interstellar environment on a planetesimal surface. -
Collision Probabilities in the Edgeworth-Kuiper Belt
Draft version April 30, 2021 Typeset using LATEX default style in AASTeX63 Collision Probabilities in the Edgeworth-Kuiper belt Abedin Y. Abedin,1 JJ Kavelaars,1 Sarah Greenstreet,2, 3 Jean-Marc Petit,4 Brett Gladman,5 Samantha Lawler,6 Michele Bannister,7 Mike Alexandersen,8 Ying-Tung Chen,9 Stephen Gwyn,1 and Kathryn Volk10 1National Research Council of Canada, Herzberg Astronomy and Astrophysics, 5071 West Saanich Road, Victoria, BC V9E 2E7, Canada 2B612 Asteroid Institute, 20 Sunnyside Avenue, Suite 427, Mill Valley, CA 94941, USA 3DIRAC Center, Department of Astronomy, University of Washington, 3910 15th Avenue NE, Seattle, WA 98195, USA 4Institut UTINAM, CNRS-UMR 6213, Universit´eBourgogne Franche Comt´eBP 1615, 25010 Besan¸conCedex, France 5Department of Physics and Astronomy, 6224 Agricultural Road, University of British Columbia, Vancouver, British Columbia, Canada 6Campion College and the Department of Physics, University of Regina, Regina SK, S4S 0A2, Canada 7University of Canterbury, Christchurch, New Zealand 8Minor Planet Center, Smithsonian Astrophysical Observatory, 60 Garden Street, Cambridge, MA 02138, US 9Academia Sinica Institute of Astronomy and Astrophysics, Taiwan 10Lunar and Planetary Laboratory, University of Arizona: Tucson, AZ, USA Submitted to AJ ABSTRACT Here, we present results on the intrinsic collision probabilities, PI , and range of collision speeds, VI , as a function of the heliocentric distance, r, in the trans-Neptunian region. The collision speed is one of the parameters, that serves as a proxy to a collisional outcome e.g., complete disruption and scattering of fragments, or formation of crater, where both processes are directly related to the impact energy. We utilize an improved and de-biased model of the trans-Neptunian object (TNO) region from the \Outer Solar System Origins Survey" (OSSOS). -
Why Pluto Is Not a Planet Anymore Or How Astronomical Objects Get Named
3 Why Pluto Is Not a Planet Anymore or How Astronomical Objects Get Named Sethanne Howard USNO retired Abstract Everywhere I go people ask me why Pluto was kicked out of the Solar System. Poor Pluto, 76 years a planet and then summarily dismissed. The answer is not too complicated. It starts with the question how are astronomical objects named or classified; asks who is responsible for this; and ends with international treaties. Ultimately we learn that it makes sense to demote Pluto. Catalogs and Names WHO IS RESPONSIBLE for naming and classifying astronomical objects? The answer varies slightly with the object, and history plays an important part. Let us start with the stars. Most of the bright stars visible to the naked eye were named centuries ago. They generally have kept their old- fashioned names. Betelgeuse is just such an example. It is the eighth brightest star in the northern sky. The star’s name is thought to be derived ,”Yad al-Jauzā' meaning “the Hand of al-Jauzā يد الجوزاء from the Arabic i.e., Orion, with mistransliteration into Medieval Latin leading to the first character y being misread as a b. Betelgeuse is its historical name. The star is also known by its Bayer designation − ∝ Orionis. A Bayeri designation is a stellar designation in which a specific star is identified by a Greek letter followed by the genitive form of its parent constellation’s Latin name. The original list of Bayer designations contained 1,564 stars. The Bayer designation typically assigns the letter alpha to the brightest star in the constellation and moves through the Greek alphabet, with each letter representing the next fainter star. -
Nomenclature in the Outer Solar System 43
Gladman et al.: Nomenclature in the Outer Solar System 43 Nomenclature in the Outer Solar System Brett Gladman University of British Columbia Brian G. Marsden Harvard-Smithsonian Center for Astrophysics Christa VanLaerhoven University of British Columbia We define a nomenclature for the dynamical classification of objects in the outer solar sys- tem, mostly targeted at the Kuiper belt. We classify all 584 reasonable-quality orbits, as of May 2006. Our nomenclature uses moderate (10 m.y.) numerical integrations to help classify the current dynamical state of Kuiper belt objects as resonant or nonresonant, with the latter class then being subdivided according to stability and orbital parameters. The classification scheme has shown that a large fraction of objects in the “scattered disk” are actually resonant, many in previously unrecognized high-order resonances. 1. INTRODUCTION 1.2. Classification Outline Dynamical nomenclature in the outer solar system is For small-a comets, historical divisions are rather arbi- complicated by the reality that we are dealing with popu- trary (e.g., based on orbital period), although recent classi- lations of objects that may have orbital stability times that fications take relative stability into account by using the Tis- are either moderately short (millions of years or less), ap- serand parameter (Levison, 1996) to separate the rapidly preciable fractions of the age of the solar system, or ex- depleted Jupiter-family comets (JFCs) from the longer-lived tremely stable (longer than the age of the solar -
Enabling Effective Exoplanet / Planetary Collaborative Science a White Paper for the Planetary Science and Astrobiology Decadal Survey 2023-2032
Enabling Effective Exoplanet / Planetary Collaborative Science A White Paper for the Planetary Science and Astrobiology Decadal Survey 2023-2032 Mark S. Marley ([email protected] 650-604-0805 NASA Ames Research Center (ARC), Moffett Field CA, USA) Co-authors: Chester ‘Sonny’ Harman (NASA Ames Research Center); Heidi B. Hammel (AURA) Paul K. Byrne (NCSU); Jonathan Fortney (University of California, Santa Cruz); Alberto Accomazzi (Center for Astrophysics | Harvard & Smithsonian); Sarah E. Moran (JHU Earth & Planetary Sciences); M. J. Way (NASA Goddard Institute for Space Studies); Jessie L. Christiansen (NASA Exoplanet Science Inst./IPAC-Caltech); Noam R. Izenberg (JHU Applied Physics Laboratory); Timothy Holt (Univ. of Southern Queensland); Sanaz Vahidinia (BAERI - NASA Ames Research Center); Erika Kohler (NASA Goddard Space Flight Center); Karalee K. Brugman (Arizona State Univ.) Co-signers: Kathleen Mandt (Johns Hopkins Univ. APL); Victoria Meadows (U. Washington); Sarah Horst (JHU); Edwin Kite (University of Chicago); Dawn Gelino (NASA Exoplanet Science Institute/IPAC-Caltech); Britney Schmidt (Georgia Tech); Niki Parenteau (NASA ARC); Giada Arney (NASA GSFC); Julie Moses (SSI); Michael Line (Ariz. State U.); Kimberly Bott (UCR); Leigh N. Fletcher (U. of Leicester); Sarah Stewart (UC Davis); Tim Lichtenberg (Univ. of Oxford); Giada Arney (NASA GSFC); Channon Visscher (Space Science Institute; Dordt University); David Sing (JHU); Nancy Chanover (NMSU); Abel Méndez (Planetary Hab. Lab., UPR); Ed Rivera-Valentín (LPI); Tiffany Kataria (JPL); Chuanfei Dong (Princeton U.); Ryan MacDonald (Cornell U.); Sang- Heon Dan Shim (Ariz. State U.); Sarah Casewell (University of Leicester); Courtney Dressing (UC Berkeley); Aki Roberge (NASA GSFC); Emily Rickman (Univ. of Geneva); Joshua Lothringer (JHU); Ishan Mishra (Cornell Univ.); Ludmila Carone (Max Planck Inst. -
Arxiv:2001.11605V1 [Astro-Ph.EP] 30 Jan 2020 Formation Process from Systems Other Than Our Own
Draft version February 3, 2020 Typeset using LATEX twocolumn style in AASTeX63 Interstellar comet 2I/Borisov as seen by MUSE: C2, NH2 and red CN detections Michele T. Bannister,1, 2 Cyrielle Opitom,3, 4 Alan Fitzsimmons,1 Youssef Moulane,3, 5, 6 Emmanuel Jehin,5 Darryl Seligman,7 Philippe Rousselot,8 Matthew M. Knight,9, 10 Michael Marsset,11 Megan E. Schwamb,1 Aurelie´ Guilbert-Lepoutre,12 Laurent Jorda,13 Pierre Vernazza,13 and Zouhair Benkhaldoun6 1Astrophysics Research Centre, School of Mathematics and Physics, Queen's University Belfast, Belfast BT7 1NN, United Kingdom 2School of Physical and Chemical Sciences { Te Kura Mat¯u,University of Canterbury, Private Bag 4800, Christchurch 8140, New Zealand 3ESO (European Southern Observatory) - Alonso de Cordova 3107, Vitacura, Santiago Chile 4Institute for Astronomy, University of Edinburgh, Royal Observatory, Edinburgh EH9 3HJ, UK 5STAR Institute, Universit´ede Li`ege,All´eedu 6 aout, 19C, 4000 Li`ege,Belgium 6Oukaimeden Observatory, Cadi Ayyad University, Marrakech, Morocco 7Department of Astronomy, Yale University, 52 Hillhouse Ave., New Haven, CT 06517 8Institut UTINAM UMR 6213, CNRS, Univ. Bourgogne Franche-Comt, OSU THETA, BP 1615, 25010 Besanon Cedex, France 9Department of Physics, United States Naval Academy, 572C Holloway Rd, Annapolis, MD 21402, USA 10University of Maryland, Department of Astronomy, College Park, MD 20742, USA 11Department of Earth, Atmospheric and Planetary Sciences, MIT, 77 Massachusetts Avenue, Cambridge, MA 02139, USA 12Laboratoire de G´eologie de Lyon, LGL-TPE, UMR 5276 CNRS / Universit´ede Lyon / Universit´eClaude Bernard Lyon 1 / ENS Lyon, 69622 Villeurbanne, France 13Aix Marseille Univ, CNRS, LAM, Laboratoire d'Astrophysique de Marseille, Marseille, France (Received 29 Jan 2020; Revised; Accepted) Submitted to ApJ Letters ABSTRACT We report the clear detection of C2 and of abundant NH2 in the first prominently active interstellar comet, 2I/Borisov.