Transit Timing Analysis of the Hot Jupiters WASP-43B and WASP-46B and the Super Earth Gj1214b
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Predicting Exoplanet Observability in Time, Contrast, Separation, and Polarization, in Scattered Light
A&A 578, A59 (2015) Astronomy DOI: 10.1051/0004-6361/201424202 & c ESO 2015 Astrophysics Predicting exoplanet observability in time, contrast, separation, and polarization, in scattered light Guillaume Schworer1;2 and Peter G. Tuthill2 1 LESIA, Observatoire de Paris, CNRS/UMR 8109, UPMC, Université Paris Diderot, 5 place J. Janssen, 92195 Meudon, France e-mail: [email protected] 2 Sydney Institute for Astronomy (SIfA), School of Physics, The University of Sydney, NSW 2006, Australia Received 14 May 2014 / Accepted 14 March 2015 ABSTRACT Context. Polarimetry is one of the keys to enhanced direct imaging of exoplanets. Not only does it deliver a differential observable pro- viding extra contrast, but when coupled with spectroscopy, it also reveals valuable information on the exoplanetary atmospheric com- position. Nevertheless, angular separation and contrast ratio to the host-star make for extremely challenging observation. Producing detailed predictions for exactly how the expected signals should appear is of critical importance for the designs and observational strategies of tomorrow’s telescopes. Aims. We aim at accurately determining the magnitudes and evolution of the main observational signatures for imaging an exoplanet: separation, contrast ratio to the host-star and polarization as a function of the orbital geometry and the reflectance parameters of the exoplanet. Methods. These parameters were used to construct a polarized-reflectance model based on the input of orbital parameters and two albedo values. The model is able to calculate a variety of observational predictions for exoplanets at any orbital time. Results. The inter-dependency of the three main observational criteria – angular separation, contrast ratio, polarization – result in a complex time-evolution of the system. -
University of California Santa Cruz
UNIVERSITY OF CALIFORNIA SANTA CRUZ BENEATH THE SURFACE OF GIANT PLANETS: EVOLUTION, STRUCTURE, AND COMPOSITION A dissertation submitted in partial satisfaction of the requirements for the degree of DOCTOR OF PHILOSOPHY in ASTRONOMY AND ASTROPHYSICS by Neil L Kelly Miller March 2013 The Dissertation of Neil L Kelly Miller is approved: Jonathan Fortney, Chair Professor D. Lin Professor P. Garaud Professor P. Bodenheimer Tyrus Miller Vice Provost and Dean of Graduate Studies Copyright c by Neil L Kelly Miller 2013 Table of Contents List of Figures v List of Tables xii Abstract xiii Dedication xv Acknowledgments xvi 1 Introduction 1 1.1 TheSolarSystemGiantPlanets . 3 1.2 FromIndividualSystemstoSamples . 4 1.3 Physical Processes in the Evolution of Giant Planets . ........ 8 2 Coupled Thermal and Tidal Evolution of Giant Expolanets 14 2.1 Abstract.................................... 14 2.2 Introduction.................................. 15 2.3 Model:Introduction ............................. 21 2.4 Model:Implementation ........................... 23 2.5 GeneralExamples .............................. 29 2.6 Results..................................... 37 2.6.1 SpecificSystems ........................... 37 2.6.2 SummaryforSuite .......................... 47 ′ 2.6.3 High Qs cases............................. 56 2.7 Discussion&Conclusions . 59 3 Applications of Giant Planet Thermal Evolution Model 74 3.1 Introduction.................................. 74 3.2 CoRoT-2b: Young Planet With Potentially Tidally Inflated Radius . 75 3.3 CoRoT-7b: Potential Evaporative Mass Loss Scenario . ....... 78 3.3.1 EvaporativeMassLossModel. 80 iii 3.3.2 PlanetEvolution ........................... 82 3.4 Kepler11 ................................... 82 3.4.1 Formation and Compositions of Kepler 11 Planets . 82 4 Measuring the Heavy Element Composition of Giant Exoplanets with Lower Irradiation 86 4.1 Abstract.................................... 86 4.2 Introduction.................................. 87 4.3 ModelandMethod............................. -
Direct Measure of Radiative and Dynamical Properties of an Exoplanet Atmosphere
DIRECT MEASURE OF RADIATIVE AND DYNAMICAL PROPERTIES OF AN EXOPLANET ATMOSPHERE The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Wit, Julien de, et al. “DIRECT MEASURE OF RADIATIVE AND DYNAMICAL PROPERTIES OF AN EXOPLANET ATMOSPHERE.” The Astrophysical Journal, vol. 820, no. 2, Mar. 2016, p. L33. © 2016 The American Astronomical Society. As Published http://dx.doi.org/10.3847/2041-8205/820/2/L33 Publisher American Astronomical Society Version Final published version Citable link http://hdl.handle.net/1721.1/114269 Terms of Use Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. The Astrophysical Journal Letters, 820:L33 (6pp), 2016 April 1 doi:10.3847/2041-8205/820/2/L33 © 2016. The American Astronomical Society. All rights reserved. DIRECT MEASURE OF RADIATIVE AND DYNAMICAL PROPERTIES OF AN EXOPLANET ATMOSPHERE Julien de Wit1, Nikole K. Lewis2, Jonathan Langton3, Gregory Laughlin4, Drake Deming5, Konstantin Batygin6, and Jonathan J. Fortney4 1 Department of Earth, Atmospheric and Planetary Sciences, MIT, 77 Massachusetts Avenue, Cambridge, MA 02139, USA 2 Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD 21218, USA 3 Department of Physics, Principia College, Elsah, IL 62028, USA 4 Department of Astronomy and Astrophysics, University of California, Santa Cruz, CA 95064, USA 5 Department of Astronomy, University of Maryland at College Park, College Park, MD 20742, USA 6 Division of Geological and Planetary Sciences, California Institute of Technology, Pasadena, CA 91125, USA Received 2016 January 28; accepted 2016 February 18; published 2016 March 28 ABSTRACT Two decades after the discovery of 51Pegb, the formation processes and atmospheres of short-period gas giants remain poorly understood. -
The Rings and Inner Moons of Uranus and Neptune: Recent Advances and Open Questions
Workshop on the Study of the Ice Giant Planets (2014) 2031.pdf THE RINGS AND INNER MOONS OF URANUS AND NEPTUNE: RECENT ADVANCES AND OPEN QUESTIONS. Mark R. Showalter1, 1SETI Institute (189 Bernardo Avenue, Mountain View, CA 94043, mshowal- [email protected]! ). The legacy of the Voyager mission still dominates patterns or “modes” seem to require ongoing perturba- our knowledge of the Uranus and Neptune ring-moon tions. It has long been hypothesized that numerous systems. That legacy includes the first clear images of small, unseen ring-moons are responsible, just as the nine narrow, dense Uranian rings and of the ring- Ophelia and Cordelia “shepherd” ring ε. However, arcs of Neptune. Voyager’s cameras also first revealed none of the missing moons were seen by Voyager, sug- eleven small, inner moons at Uranus and six at Nep- gesting that they must be quite small. Furthermore, the tune. The interplay between these rings and moons absence of moons in most of the gaps of Saturn’s rings, continues to raise fundamental dynamical questions; after a decade-long search by Cassini’s cameras, sug- each moon and each ring contributes a piece of the gests that confinement mechanisms other than shep- story of how these systems formed and evolved. herding might be viable. However, the details of these Nevertheless, Earth-based observations have pro- processes are unknown. vided and continue to provide invaluable new insights The outermost µ ring of Uranus shares its orbit into the behavior of these systems. Our most detailed with the tiny moon Mab. Keck and Hubble images knowledge of the rings’ geometry has come from spanning the visual and near-infrared reveal that this Earth-based stellar occultations; one fortuitous stellar ring is distinctly blue, unlike any other ring in the solar alignment revealed the moon Larissa well before Voy- system except one—Saturn’s E ring. -
Abstracts of the 50Th DDA Meeting (Boulder, CO)
Abstracts of the 50th DDA Meeting (Boulder, CO) American Astronomical Society June, 2019 100 — Dynamics on Asteroids break-up event around a Lagrange point. 100.01 — Simulations of a Synthetic Eurybates 100.02 — High-Fidelity Testing of Binary Asteroid Collisional Family Formation with Applications to 1999 KW4 Timothy Holt1; David Nesvorny2; Jonathan Horner1; Alex B. Davis1; Daniel Scheeres1 Rachel King1; Brad Carter1; Leigh Brookshaw1 1 Aerospace Engineering Sciences, University of Colorado Boulder 1 Centre for Astrophysics, University of Southern Queensland (Boulder, Colorado, United States) (Longmont, Colorado, United States) 2 Southwest Research Institute (Boulder, Connecticut, United The commonly accepted formation process for asym- States) metric binary asteroids is the spin up and eventual fission of rubble pile asteroids as proposed by Walsh, Of the six recognized collisional families in the Jo- Richardson and Michel (Walsh et al., Nature 2008) vian Trojan swarms, the Eurybates family is the and Scheeres (Scheeres, Icarus 2007). In this theory largest, with over 200 recognized members. Located a rubble pile asteroid is spun up by YORP until it around the Jovian L4 Lagrange point, librations of reaches a critical spin rate and experiences a mass the members make this family an interesting study shedding event forming a close, low-eccentricity in orbital dynamics. The Jovian Trojans are thought satellite. Further work by Jacobson and Scheeres to have been captured during an early period of in- used a planar, two-ellipsoid model to analyze the stability in the Solar system. The parent body of the evolutionary pathways of such a formation event family, 3548 Eurybates is one of the targets for the from the moment the bodies initially fission (Jacob- LUCY spacecraft, and our work will provide a dy- son and Scheeres, Icarus 2011). -
Self-Organizing Systems in Planetary Physics: Harmonic Resonances Of
Self-Organizing Systems in Planetary Physics : Harmonic Resonances of Planet and Moon Orbits Markus J. Aschwanden1 1) Lockheed Martin, Solar and Astrophysics Laboratory, Org. A021S, Bldg. 252, 3251 Hanover St., Palo Alto, CA 94304, USA; e-mail: [email protected] ABSTRACT The geometric arrangement of planet and moon orbits into a regularly spaced pattern of distances is the result of a self-organizing system. The positive feedback mechanism that operates a self-organizing system is accomplished by harmonic orbit resonances, leading to long-term stable planet and moon orbits in solar or stellar systems. The distance pattern of planets was originally described by the empirical Titius-Bode law, and by a generalized version with a constant geometric progression factor (corresponding to logarithmic spacing). We find that the orbital periods Ti and planet distances Ri from the Sun are not consistent with logarithmic spacing, 2/3 2/3 but rather follow the quantized scaling (Ri+1/Ri) = (Ti+1/Ti) = (Hi+1/Hi) , where the harmonic ratios are given by five dominant resonances, namely (Hi+1 : Hi)=(3:2), (5 : 3), (2 : 1), (5 : 2), (3 : 1). We find that the orbital period ratios tend to follow the quantized harmonic ratios in increasing order. We apply this harmonic orbit resonance model to the planets and moons in our solar system, and to the exo-planets of 55 Cnc and HD 10180 planetary systems. The model allows us a prediction of missing planets in each planetary system, based on the quasi- regular self-organizing pattern of harmonic orbit resonance zones. We predict 7 (and 4) missing exo-planets around the star 55 Cnc (and HD 10180). -
ON the INCLINATION DEPENDENCE of EXOPLANET PHASE SIGNATURES Stephen R
The Astrophysical Journal, 729:74 (6pp), 2011 March 1 doi:10.1088/0004-637X/729/1/74 C 2011. The American Astronomical Society. All rights reserved. Printed in the U.S.A. ON THE INCLINATION DEPENDENCE OF EXOPLANET PHASE SIGNATURES Stephen R. Kane and Dawn M. Gelino NASA Exoplanet Science Institute, Caltech, MS 100-22, 770 South Wilson Avenue, Pasadena, CA 91125, USA; [email protected] Received 2011 December 2; accepted 2011 January 5; published 2011 February 10 ABSTRACT Improved photometric sensitivity from space-based telescopes has enabled the detection of phase variations for a small sample of hot Jupiters. However, exoplanets in highly eccentric orbits present unique opportunities to study the effects of drastically changing incident flux on the upper atmospheres of giant planets. Here we expand upon previous studies of phase functions for these planets at optical wavelengths by investigating the effects of orbital inclination on the flux ratio as it interacts with the other effects induced by orbital eccentricity. We determine optimal orbital inclinations for maximum flux ratios and combine these calculations with those of projected separation for application to coronagraphic observations. These are applied to several of the known exoplanets which may serve as potential targets in current and future coronagraph experiments. Key words: planetary systems – techniques: photometric 1. INTRODUCTION and inclination for a given eccentricity. We further calculate projected separations at apastron as a function of inclination The changing phases of an exoplanet as it orbits the host star and determine their correspondence with maximum flux ratio have long been considered as a means for their detection and locations. -
Astro Vol.7 Issue 4
NEWSLETTER Year 7, Issue 04 PSSP - News The First NASA Videoconference Prepared by Elzbieta Gwiazda-Szer On the 15th of January there was a videoconference between the Rota College (Izmir, Turkey), School4Child (Lodz, Poland) and NASA’s Marshall Space Flight Center in Huntsville, Alabama in the U.S.A.. It was a historical day for both schools since it was their first videoconference with a NASA Center. Our school prepared for that during the classes conducted by Ms. Elzbieta Gwiazda-Szer . The classes and videoconference’s theme was "Toys in Space". In class, students got familiar with Newton's three principles of dynamics, they learned about gravity and microgravity. In groups, students sought answers to questions concerning the behavior of their toys in space. Their considerations related to a football , a jump rope , a kendama and a paper boomerang . Some students have modified their toys in order to improve the fun efficiency in microgravity. Our students also had the opportunity to meet with their ePals, with whom they are in touch via emails. This is the third year we have been partners of the program PSSP - Partner School Science Program. The videoconferencing has been received with great enthusiasm by both our students and students from Turkey. Pages 1 Technology Lunar Time Lapse Panorama including Yutu Rover Image Credit: CNSA, Chinanews, Kenneth Kremer & Marco Di Lorenzo Where has the Yutu rover been on the Moon? Arriving in 2013 mid-December, the Chinese Yutu robotic rover has spent some of the past month and a half exploring Mare Imbrium on Earth's Moon. -
Filipiak Solar System Book
Our Solar System Mrs. Filipiak’s Class Our Solar System Mrs. Filipiak’s Class Sun ...............................................................................................7 Michael ........................................................................................7 Mercury ........................................................................................1 Denzel ..........................................................................................1 Mercury ........................................................................................3 Austin ...........................................................................................3 Mercury ........................................................................................5 Madison B ....................................................................................5 Venus ............................................................................................7 Shyla .............................................................................................7 Venus ............................................................................................9 Kenny ...........................................................................................9 Earth ..........................................................................................11 Kaleb ..........................................................................................11 Earth ..........................................................................................13 -
Resonant Moons of Neptune
EPSC Abstracts Vol. 13, EPSC-DPS2019-901-1, 2019 EPSC-DPS Joint Meeting 2019 c Author(s) 2019. CC Attribution 4.0 license. Resonant moons of Neptune Marina Brozović (1), Mark R. Showalter (2), Robert A. Jacobson (1), Robert S. French (2), Jack L. Lissauer (3), Imke de Pater (4) (1) Jet Propulsion Laboratory, California Institute of Technology, California, USA, (2) SETI Institute, California, USA, (3) NASA Ames Research Center, California, USA, (4) University of California Berkeley, California, USA Abstract We used integrated orbits to fit astrometric data of the 2. Methods regular moons of Neptune. We found a 73:69 inclination resonance between Naiad and Thalassa, the 2.1 Observations two innermost moons. Their resonant argument librates around 180° with an average amplitude of The astrometric data cover the period from 1981-2016, ~66° and a period of ~1.9 years. This is the first fourth- with the most significant amount of data originating order resonance discovered between the moons of the from the Voyager 2 spacecraft and HST. Voyager 2 outer planets. The resonance enabled an estimate of imaged all regular satellites except Hippocamp the GMs for Naiad and Thalassa, GMN= between 1989 June 7 and 1989 August 24. The follow- 3 -2 3 0.0080±0.0043 km s and GMT=0.0236±0.0064 km up observations originated from several Earth-based s-2. More high-precision astrometry of Naiad and telescopes, but the majority were still obtained by HST. Thalassa will help better constrain their masses. The [4] published the latest set of the HST astrometry GMs of Despina, Galatea, and Larissa are more including the discovery and follow up observations of difficult to measure because they are not in any direct Hippocamp. -
Detailed Chemical Compositions of the Wide Binary HD 80606/80607: Revised Stellar Properties and Constraints on Planet Formation?,?? F
A&A 614, A138 (2018) Astronomy https://doi.org/10.1051/0004-6361/201832701 & c ESO 2018 Astrophysics Detailed chemical compositions of the wide binary HD 80606/80607: revised stellar properties and constraints on planet formation?;?? F. Liu1, D. Yong2, M. Asplund2, S. Feltzing1, A. J. Mustill1, J. Meléndez3, I. Ramírez4, and J. Lin2 1 Lund Observatory, Department of Astronomy and Theoretical physics, Lund University, Box 43, 22100 Lund, Sweden e-mail: [email protected] 2 Research School of Astronomy and Astrophysics, Australian National University, Canberra, ACT 2611, Australia 3 Departamento de Astronomia do IAG/USP, Universidade de São Paulo, Rua do Matão 1226, São Paulo 05508-900, SP, Brazil 4 Tacoma Community College, 6501 S. 19th Street, Tacoma, WA 98466, USA Received 25 January 2018 / Accepted 25 February 2018 ABSTRACT Differences in the elemental abundances of planet-hosting stars in binary systems can give important clues and constraints about planet formation and evolution. In this study we performed a high-precision, differential elemental abundance analysis of a wide binary system, HD 80606/80607, based on high-resolution spectra with high signal-to-noise ratio obtained with Keck/HIRES. HD 80606 is known to host a giant planet with the mass of four Jupiters, but no planet has been detected around HD 80607 so far. We determined stellar parameters as well as abundances for 23 elements for these two stars with extremely high precision. Our main results are that (i) we confirmed that the two components share very similar chemical compositions, but HD 80606 is marginally more metal-rich than HD 80607, with an average difference of +0.013 ± 0.002 dex (σ = 0.009 dex); and (ii) there is no obvious trend between abundance differences and condensation temperature. -
PDS4 Context List
Target Context List Name Type LID 136108 HAUMEA Planet urn:nasa:pds:context:target:planet.136108_haumea 136472 MAKEMAKE Planet urn:nasa:pds:context:target:planet.136472_makemake 1989N1 Satellite urn:nasa:pds:context:target:satellite.1989n1 1989N2 Satellite urn:nasa:pds:context:target:satellite.1989n2 ADRASTEA Satellite urn:nasa:pds:context:target:satellite.adrastea AEGAEON Satellite urn:nasa:pds:context:target:satellite.aegaeon AEGIR Satellite urn:nasa:pds:context:target:satellite.aegir ALBIORIX Satellite urn:nasa:pds:context:target:satellite.albiorix AMALTHEA Satellite urn:nasa:pds:context:target:satellite.amalthea ANTHE Satellite urn:nasa:pds:context:target:satellite.anthe APXSSITE Equipment urn:nasa:pds:context:target:equipment.apxssite ARIEL Satellite urn:nasa:pds:context:target:satellite.ariel ATLAS Satellite urn:nasa:pds:context:target:satellite.atlas BEBHIONN Satellite urn:nasa:pds:context:target:satellite.bebhionn BERGELMIR Satellite urn:nasa:pds:context:target:satellite.bergelmir BESTIA Satellite urn:nasa:pds:context:target:satellite.bestia BESTLA Satellite urn:nasa:pds:context:target:satellite.bestla BIAS Calibrator urn:nasa:pds:context:target:calibrator.bias BLACK SKY Calibration Field urn:nasa:pds:context:target:calibration_field.black_sky CAL Calibrator urn:nasa:pds:context:target:calibrator.cal CALIBRATION Calibrator urn:nasa:pds:context:target:calibrator.calibration CALIMG Calibrator urn:nasa:pds:context:target:calibrator.calimg CAL LAMPS Calibrator urn:nasa:pds:context:target:calibrator.cal_lamps CALLISTO Satellite urn:nasa:pds:context:target:satellite.callisto