JWST/Nirspec Prospects on Transneptunian Objects
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A Deeper Look at the Colors of the Saturnian Irregular Satellites Arxiv
A deeper look at the colors of the Saturnian irregular satellites Tommy Grav Harvard-Smithsonian Center for Astrophysics, MS51, 60 Garden St., Cambridge, MA02138 and Instiute for Astronomy, University of Hawaii, 2680 Woodlawn Dr., Honolulu, HI86822 [email protected] James Bauer Jet Propulsion Laboratory, California Institute of Technology 4800 Oak Grove Dr., MS183-501, Pasadena, CA91109 [email protected] September 13, 2018 arXiv:astro-ph/0611590v2 8 Mar 2007 Manuscript: 36 pages, with 11 figures and 5 tables. 1 Proposed running head: Colors of Saturnian irregular satellites Corresponding author: Tommy Grav MS51, 60 Garden St. Cambridge, MA02138 USA Phone: (617) 384-7689 Fax: (617) 495-7093 Email: [email protected] 2 Abstract We have performed broadband color photometry of the twelve brightest irregular satellites of Saturn with the goal of understanding their surface composition, as well as their physical relationship. We find that the satellites have a wide variety of different surface colors, from the negative spectral slopes of the two retrograde satellites S IX Phoebe (S0 = −2:5 ± 0:4) and S XXV Mundilfari (S0 = −5:0 ± 1:9) to the fairly red slope of S XXII Ijiraq (S0 = 19:5 ± 0:9). We further find that there exist a correlation between dynamical families and spectral slope, with the prograde clusters, the Gallic and Inuit, showing tight clustering in colors among most of their members. The retrograde objects are dynamically and physically more dispersed, but some internal structure is apparent. Keywords: Irregular satellites; Photometry, Satellites, Surfaces; Saturn, Satellites. 3 1 Introduction The satellites of Saturn can be divided into two distinct groups, the regular and irregular, based on their orbital characteristics. -
" Tnos Are Cool": a Survey of the Trans-Neptunian Region VI. Herschel
Astronomy & Astrophysics manuscript no. classicalTNOsManuscript c ESO 2012 April 4, 2012 “TNOs are Cool”: A survey of the trans-Neptunian region VI. Herschel⋆/PACS observations and thermal modeling of 19 classical Kuiper belt objects E. Vilenius1, C. Kiss2, M. Mommert3, T. M¨uller1, P. Santos-Sanz4, A. Pal2, J. Stansberry5, M. Mueller6,7, N. Peixinho8,9 S. Fornasier4,10, E. Lellouch4, A. Delsanti11, A. Thirouin12, J. L. Ortiz12, R. Duffard12, D. Perna13,14, N. Szalai2, S. Protopapa15, F. Henry4, D. Hestroffer16, M. Rengel17, E. Dotto13, and P. Hartogh17 1 Max-Planck-Institut f¨ur extraterrestrische Physik, Postfach 1312, Giessenbachstr., 85741 Garching, Germany e-mail: [email protected] 2 Konkoly Observatory of the Hungarian Academy of Sciences, 1525 Budapest, PO Box 67, Hungary 3 Deutsches Zentrum f¨ur Luft- und Raumfahrt e.V., Institute of Planetary Research, Rutherfordstr. 2, 12489 Berlin, Germany 4 LESIA-Observatoire de Paris, CNRS, UPMC Univ. Paris 06, Univ. Paris-Diderot, France 5 Stewart Observatory, The University of Arizona, Tucson AZ 85721, USA 6 SRON LEA / HIFI ICC, Postbus 800, 9700AV Groningen, Netherlands 7 UNS-CNRS-Observatoire de la Cˆote d’Azur, Laboratoire Cassiope´e, BP 4229, 06304 Nice Cedex 04, France 8 Center for Geophysics of the University of Coimbra, Av. Dr. Dias da Silva, 3000-134 Coimbra, Portugal 9 Astronomical Observatory of the University of Coimbra, Almas de Freire, 3040-04 Coimbra, Portugal 10 Univ. Paris Diderot, Sorbonne Paris Cit´e, 4 rue Elsa Morante, 75205 Paris, France 11 Laboratoire d’Astrophysique de Marseille, CNRS & Universit´ede Provence, 38 rue Fr´ed´eric Joliot-Curie, 13388 Marseille Cedex 13, France 12 Instituto de Astrof´ısica de Andaluc´ıa (CSIC), Camino Bajo de Hu´etor 50, 18008 Granada, Spain 13 INAF – Osservatorio Astronomico di Roma, via di Frascati, 33, 00040 Monte Porzio Catone, Italy 14 INAF - Osservatorio Astronomico di Capodimonte, Salita Moiariello 16, 80131 Napoli, Italy 15 University of Maryland, College Park, MD 20742, USA 16 IMCCE, Observatoire de Paris, 77 av. -
With JWST: Science Justification and Observational Requirements
Observing Outer Planet Satellites (except Titan) with JWST: Science Justification and Observational Requirements Laszlo Keszthelyi1, Will Grundy2, John Stansberry3, Anand Sivaramakrishnan3, Deepashri Thatte3, Murthy Gudipati4, Constantine Tsang5, Alexandra Greenbaum6, Chima McGruder7 1U.S. Geological Survey, Astrogeology Science Center, 2255 N. Gemini Dr., Flagstaff, AZ 86001. ([email protected]) 2Lowell Observatory, 1400 W. Mars Hill Rd., Flagstaff, AZ 86001. ([email protected]) 3Space Telescope Science Institute, 3700 San Martin Dr., Baltimore, MD 21218. ([email protected]; [email protected]; [email protected]) 4California Institute of Technology, Jet Propulsion Laboratory, 4800 Oak Grove Dr., Pasadena, CA 91109. ([email protected]) 5Southwest Research Institute, Department of Space Studies, 1050 Walnut St., Suite 300, Boulder, CO 80302. ([email protected]) 6 Department of Physics and Astronomy, 3400 N. Charles Street, Baltimore, MD 21218. ([email protected]) 7Department of Physics & Astronomy, 1408 Circle Drive, Knoxville, TN 37996. ([email protected]) ABSTRACT The James Webb Space Telescope (JWST) will allow observations with a unique combination of spectral, spatial, and temporal resolution for the study of outer planet satellites within our Solar System. We highlight the infrared spectroscopy of icy moons and temporal changes on geologically active satellites as two particularly valuable avenues of scientific inquiry. While some care must be taken to avoid saturation issues, JWST has observation modes that should provide excellent infrared data for such studies. KEYWORDS Solar System Astronomical Techniques 1. Introduction Starting in 2018, the James Webb Space Telescope (JWST) is expected to provide a groundbreaking new tool for astronomical observations, including planetary satellites as close as Phobos and Deimos. -
Arxiv:2001.00125V1 [Astro-Ph.EP] 1 Jan 2020
Draft version January 3, 2020 Typeset using LATEX default style in AASTeX61 SIZE AND SHAPE CONSTRAINTS OF (486958) ARROKOTH FROM STELLAR OCCULTATIONS Marc W. Buie,1 Simon B. Porter,1 et al. 1Southwest Research Institute 1050 Walnut St., Suite 300, Boulder, CO 80302 USA To be submitted to Astronomical Journal, Version 1.1, 2019/12/30 ABSTRACT We present the results from four stellar occultations by (486958) Arrokoth, the flyby target of the New Horizons extended mission. Three of the four efforts led to positive detections of the body, and all constrained the presence of rings and other debris, finding none. Twenty-five mobile stations were deployed for 2017 June 3 and augmented by fixed telescopes. There were no positive detections from this effort. The event on 2017 July 10 was observed by SOFIA with one very short chord. Twenty-four deployed stations on 2017 July 17 resulted in five chords that clearly showed a complicated shape consistent with a contact binary with rough dimensions of 20 by 30 km for the overall outline. A visible albedo of 10% was derived from these data. Twenty-two systems were deployed for the fourth event on 2018 Aug 4 and resulted in two chords. The combination of the occultation data and the flyby results provides a significant refinement of the rotation period, now estimated to be 15.9380 ± 0.0005 hours. The occultation data also provided high-precision astrometric constraints on the position of the object that were crucial for supporting the navigation for the New Horizons flyby. This work demonstrates an effective method for obtaining detailed size and shape information and probing for rings and dust on distant Kuiper Belt objects as well as being an important source of positional data that can aid in spacecraft navigation that is particularly useful for small and distant bodies. -
New Constraints on the Membership of the T Dwarf S Ori 70 in the Σ Orionis Cluster
A&A 477, 895–900 (2008) Astronomy DOI: 10.1051/0004-6361:20078600 & c ESO 2008 Astrophysics New constraints on the membership of the T dwarf S Ori 70 in the σ Orionis cluster M. R. Zapatero Osorio1,V.J.S.Béjar1,G.Bihain1,2, E. L. Martín1,3,R.Rebolo1,2, I. Villó-Pérez4, A. Díaz-Sánchez5, A. Pérez Garrido5, J. A. Caballero6, T. Henning6, R. Mundt6, D. Barrado y Navascués7, and C. A. L. Bailer-Jones6 1 Instituto de Astrofísica de Canarias, 38200 La Laguna, Tenerife, Spain e-mail: [email protected] 2 Consejo Superior de Investigaciones Científicas, Spain 3 University of Central Florida, Department of Physics, PO Box 162385, Orlando, FL 32816, USA 4 Departamento de Electrónica, Universidad Politécnica de Cartagena, 30202 Cartagena, Spain 5 Departamento de Física Aplicada, Universidad Politécnica de Cartagena, 30202 Cartagena, Spain 6 Max-Planck Institut für Astronomie, Königstuhl 17, 69117 Heidelberg, Germany 7 LAEFF-INTA, PO 50727, 28080 Madrid, Spain Received 2 September 2007 / Accepted 10 October 2007 ABSTRACT Aims. The nature of S Ori 70 (S Ori J053810.1−023626), a faint mid-T type object found towards the direction of the young σ Orionis cluster, is still under debate. We intend to find out whether it is a field brown dwarf or a 3-Myr old planetary-mass member of the cluster. Methods. We report on near-infrared JHKs and mid-infrared [3.6] and [4.5] IRAC/Spitzer photometry recently obtained for S Ori 70. The new near-infrared images (taken 3.82 yr after the discovery data) allowed us to derive the first proper motion measurement for this object. -
Quaoar from Multi-Chord Stellar Occultations
The Astrophysical Journal, 773:26 (13pp), 2013 August 10 doi:10.1088/0004-637X/773/1/26 C 2013. The American Astronomical Society. All rights reserved. Printed in the U.S.A. THE SIZE, SHAPE, ALBEDO, DENSITY, AND ATMOSPHERIC LIMIT OF TRANSNEPTUNIAN OBJECT (50000) QUAOAR FROM MULTI-CHORD STELLAR OCCULTATIONS F. Braga-Ribas1,2,28, B. Sicardy2,3,J.L.Ortiz4, E. Lellouch2, G. Tancredi5, J. Lecacheux2, R. Vieira-Martins1,6,7, J. I. B. Camargo1, M. Assafin7, R. Behrend8,F.Vachier6, F. Colas6, N. Morales4, A. Maury9, M. Emilio10,A.Amorim11, E. Unda-Sanzana12, S. Roland5, S. Bruzzone5, L. A. Almeida13, C. V. Rodrigues13, C. Jacques14, R. Gil-Hutton15, L. Vanzi16,A.C.Milone13, W. Schoenell4,11, R. Salvo5, L. Almenares5,E.Jehin17, J. Manfroid17, S. Sposetti18, P. Tanga19, A. Klotz20, E. Frappa21, P. Cacella22, J. P. Colque12, C. Neves10, E. M. Alvarez23, M. Gillon17, E. Pimentel14, B. Giacchini14, F. Roques2, T. Widemann2, V. S. Magalhaes˜ 13, A. Thirouin4, R. Duffard4, R. Leiva16, I. Toledo24, J. Capeche5, W. Beisker25, J. Pollock26,C.E.Cedeno˜ Montana˜ 13, K. Ivarsen27, D. Reichart27, J. Haislip27, and A. Lacluyze27 1 Observatorio´ Nacional, Rio de Janeiro, Brazil; [email protected] 2 Observatoire de Paris, LESIA, F-92195 Meudon, France 3 Universite´ Pierre et Marie Curie, F-75252 Paris, France 4 Instituto de Astrof´ısica de Andaluc´ıa-CSIC, E-18080 Granada, Spain 5 Observatorio Astronomico Los Molinos, Montevideo U-12400, Uruguay 6 Observatoire de Paris, IMCCE, F-75014 Paris, France 7 Observatorio´ do Valongo/UFRJ, Rio de Janeiro, Brazil 8 Observatoire -
Chord Direction in Asteroid Occultations: Effect of Earth Rotation and Orientation Combined with Asteroid Relative Velocity
Chord direction in asteroid occultations: Effect of Earth rotation and orientation combined with asteroid relative velocity Frank Freestar8n This report conveys why the chord measured as an asteroid occults a star depends on many parameters related to the observer’s location on the rotating Earth. Several factors are at work: Earth rotation and tilt as seen by the asteroid, observer latitude and proximity to the Earth’s limb (i.e. the altitude of the asteroid in the observer’s sky), and relative velocity of the asteroid to the Earth. Retrograde (apparent westward at 12 km/s) 18 km/s Stationary Stationary Direct (eastward, slow) Asteroid Direct (eastward, slow) 0.5 km/s rotation at equator, 0 at poles 30 km/s Earth View from North pole Direct (apparent eastward at 48 km/s) Figure 1. Basic geometry of orbits and rotation with associated velocities. The figure above shows the orbital and rotational components that dominate the motion of an asteroid during an occultation. The Earth orbits counter-clockwise at 30 km/s, while farther away main-belt asteroids orbit in the same direction at about 18 km/s. At opposition the asteroid appears to be moving westward (retrograde) at 12 km/s relative to a stationary Earth. On the other side of the sun, the asteroid appears to move eastward at 48 km/s. Near opposition, approximately 54 degrees either side, the asteroid appears to stop its east-west motion because its relative motion is in the direction of Earth. On either side near that stationary point, the asteroid will appear to be moving slowly relative to the stars. -
Visible and Near-Infrared Colors of Transneptunian Objects and Centaurs from the Second ESO Large Program
A&A 493, 283–290 (2009) Astronomy DOI: 10.1051/0004-6361:200810561 & c ESO 2008 Astrophysics Visible and near-infrared colors of Transneptunian objects and Centaurs from the second ESO large program F. E. DeMeo1, S. Fornasier1,2, M. A. Barucci1,D.Perna1,3,4, S. Protopapa5, A. Alvarez-Candal1, A. Delsanti1, A. Doressoundiram1, F. Merlin1, and C. de Bergh1 1 LESIA, Observatoire de Paris, 92195 Meudon Principal Cedex, France e-mail: [email protected] 2 Université de Paris 7 Denis Diderot, Paris, France 3 INAF – Osservatorio Astronomico di Roma, via Frascati 33, 00040 Monte Porzio Catone, Italy 4 Università di Roma Tor Vergata, via della Ricerca Scientifica 1, 00133 Roma, Italy 5 Max Planck Institute for Solar System Research, Lindau, Germany Received 10 July 2008 / Accepted 9 October 2008 ABSTRACT Aims. We investigate color properties and define or check taxonomic classifications of objects observed in our survey. Methods. All observations were performed between October 2006 and September 2007 at the European Southern Observatory 8 m Very Large Telescope, UT1 and UT2 at the Paranal Observatory in Chile. For visible photometry, we used the FORS1 instrument, and for near-infrared, ISAAC. Taxonomic classifications from the Barucci system were assigned using G-mode analysis. Results. We present photometric observations of 23 TNOs and Centaurs, nine of which have never been previously observed. Eighteen of these objects were assigned taxonomic classifications: six BB, four BR, two RR, and six that are given two or more categories due to insufficient data. Three objects that had been previously observed and classified, changed classes most likely due to surface vari- ation: 26375 (1999 DE9), 28978 (Ixion), and 32532 (Thereus). -
Mass of the Kuiper Belt · 9Th Planet PACS 95.10.Ce · 96.12.De · 96.12.Fe · 96.20.-N · 96.30.-T
Celestial Mechanics and Dynamical Astronomy manuscript No. (will be inserted by the editor) Mass of the Kuiper Belt E. V. Pitjeva · N. P. Pitjev Received: 13 December 2017 / Accepted: 24 August 2018 The final publication ia available at Springer via http://doi.org/10.1007/s10569-018-9853-5 Abstract The Kuiper belt includes tens of thousands of large bodies and millions of smaller objects. The main part of the belt objects is located in the annular zone between 39.4 au and 47.8 au from the Sun, the boundaries correspond to the average distances for orbital resonances 3:2 and 2:1 with the motion of Neptune. One-dimensional, two-dimensional, and discrete rings to model the total gravitational attraction of numerous belt objects are consid- ered. The discrete rotating model most correctly reflects the real interaction of bodies in the Solar system. The masses of the model rings were determined within EPM2017—the new version of ephemerides of planets and the Moon at IAA RAS—by fitting spacecraft ranging observations. The total mass of the Kuiper belt was calculated as the sum of the masses of the 31 largest trans-neptunian objects directly included in the simultaneous integration and the estimated mass of the model of the discrete ring of TNO. The total mass −2 is (1.97 ± 0.30) · 10 m⊕. The gravitational influence of the Kuiper belt on Jupiter, Saturn, Uranus and Neptune exceeds at times the attraction of the hypothetical 9th planet with a mass of ∼ 10 m⊕ at the distances assumed for it. -
Thermal Measurements
Physical characterization of Kuiper belt objects from stellar occultations and thermal measurements Pablo Santos-Sanz & the SBNAF team [email protected] Stellar occultations Simple method to: -Obtain high precision sizes/shapes (unc. ~km) -Detect/characterize atmospheres/rings… -Obtain albedo, density… -Improve the orbit of the body …this looks like very nice but...the reality is harder (at least for TNOs and Centaurs) EPSC2017, Riga, Latvia, 20 Sep. 2017 Stellar occultations Titan 10 mas Quaoar 0.033 arsec Diameter of 1 Euro (33 mas) Pluto coin at 140 km Eris Charon Makemake Pablo Santos-Sanz EPSC2017, Riga, Latvia, 20 Sep. 2017 Stellar occultations ~25 occultations by 15 TNOs (+ Pluto/Charon + Chariklo + Chiron + 2002 GZ32) Namaka Dysnomia Ixion Hi’iaka Pluto Haumea Eris Chiron 2007 UK126 Chariklo Vanth 2014 MU69 2002 GZ32 2003 VS2 2002 KX14 2002 TX300 2003 AZ84 2005 TV189 Stellar occultations: Eris & Chariklo Eris: 6 November 2010 Chariklo: 3 June 2014 • Size ~ Plutón • It has rings! • Albedo= 96% 3 • Density= 2.5 g/cm Danish 1.54-m telescope (La Silla) • Atmosphere < 1nbar (10-4 x Pluto) Eris’ radius Pluto’s radius 1163±6 km 1188.3±1.6 km (Nimmo et al. 2016) Braga-Ribas et al. 2014 (Nature) Sicardy et al. 2011 (Nature) EPSC2017, Riga, Latvia, 20 Sep. 2017 Stellar occultations: Makemake 23 April 2011 Geometric Albedo = 77% (betwen Pluto and Eris) Possible local atmosphere! Ortiz et al. 2012 (Nature) EPSC2017, Riga, Latvia, 20 Sep. 2017 Stellar occultations: latest “catches” 2007 UK : 15 November 2014 2003 AZ84: 8 Jan. 2011 single, 3 Feb. 126 2012 multi, 2 Dec. -
(50000) Quaoar, See Quaoar (90377) Sedna, See Sedna 1992 QB1 267
Index (50000) Quaoar, see Quaoar Apollo Mission Science Reports 114 (90377) Sedna, see Sedna Apollo samples 114, 115, 122, 1992 QB1 267, 268 ap-value, 3-hour, conversion from Kp 10 1996 TL66 268 arcade, post-eruptive 24–26 1998 WW31 274 Archimedian spiral 11 2000 CR105 269 Arecibo observatory 63 2000 OO67 277 Ariel, carbon dioxide ice 256–257 2003 EL61 270, 271, 273, 274, 275, 286, astrometric detection, of extrasolar planets – mass 273 190 – satellites 273 Atlas 230, 242, 244 – water ice 273 Bartels, Julius 4, 8 2003 UB313 269, 270, 271–272, 274, 286 – methane 271–272 Becquerel, Antoine Henry 3 – orbital parameters 271 Biermann, Ludwig 5 – satellite 272 biomass, from chemolithoautotrophs, on Earth 169 – spectroscopic studies 271 –, – on Mars 169 2005 FY 269, 270, 272–273, 286 9 bombardment, late heavy 68, 70, 71, 77, 78 – atmosphere 273 Borealis basin 68, 71, 72 – methane 272–273 ‘Brown Dwarf Desert’ 181, 188 – orbital parameters 272 brown dwarfs, deuterium-burning limit 181 51 Pegasi b 179, 185 – formation 181 Alfvén, Hannes 11 Callisto 197, 198, 199, 200, 204, 205, 206, ALH84001 (martian meteorite) 160 207, 211, 213 Amalthea 198, 199, 200, 204–205, 206, 207 – accretion 206, 207 – bright crater 199 – compared with Ganymede 204, 207 – density 205 – composition 204 – discovery by Barnard 205 – geology 213 – discovery of icy nature 200 – ice thickness 204 – evidence for icy composition 205 – internal structure 197, 198, 204 – internal structure 198 – multi-ringed impact basins 205, 211 – orbit 205 – partial differentiation 200, 204, 206, -
Occultations of HIP and UCAC2 Stars Downto 15M by Large TNO in 2004
Astronomy Letters, 2004, vol. 30. Translated from Pis’ma v Astronomicheskij Zhurnal. Occultations of HIP and UCAC2 stars downto 15m by large TNO in 2004-2014 © 2004 D.V. Denissenko Space Research Institute (IKI), Moscow, Russia Received 27 February 2004 Occultations of stars brighter than 15m by largest TNOs are predicted. Search was performed using the following catalogues: Hipparcos; Tycho2 with coordinates of 2838666 stars taken from UCAC2 (Herald, 2003); UCAC2 (Zacharias et al., 2003) with 16356096 stars between 12.00 and 14.99 mag to the north from -45 declination. Predictions were made for 17 largest numbered transneptunian asteroids, recently discovered 2004 DW and 4 known binary Kuiper Belt objects. 64 events occuring at solar elongation of 30° and more are selected, including exceptionally rare occultation m of 6.5 star by double (66652) 1999 RZ253 on 2007 October 4th. Observations of these events by all available means are extremely important since they can provide unique information about the size of TNOs and improve their orbits dramatically. INTRODUCTION OCCULTATIONS BY TNO Over 800 Transneptunian Objects (TNO) are TNOs are typically at 30-50 AU distances discovered since 1992 with 67 of them being from the Earth corresponding to 0.2"-0.3" numbered and 7 having proper names as of parallax. This means that occultation will February 2004. No reliable measurements only happen somewhere on the Earth if the of their sizes have been obtained so far. geocentric path of the object passes within Angular sizes even of the largest objects are 200-300 mas from the star. Combined with arXiv:astro-ph/0403002 28 Feb 2004 about 0.04"±0.01" (Quaoar) which is at the a very slow angular motion of TNO (0.1-1 limit of Hubble Space Telescope resolution.