Astronomy and Astrophysics

Total Page:16

File Type:pdf, Size:1020Kb

Astronomy and Astrophysics Astronomy and Astrophysics Observing the On-going Formation of Planets and its Effects on Their Parent Discs Mr Matthew Alexander Willson Submitted by Mr Matthew Alexander Willson to the University of Exeter as a thesis for the degree of Doctor of Philosophy in Physics, June, 2017. This thesis is available for Library use on the understanding that it is copyright material and that no quotation from the thesis may be published without proper acknowledgement. I certify that all material in this thesis which is not my own work has been identified and that no material has previously been submitted and approved for the award of a degree by this or any other University. Signed: . M Willson Date: 07/09/2017 Abstract As the number of known exoplanetary systems has grown, it has become increasing ap- parent that our current understanding of planet formation is insufficient to explain the broad but distinct distributions of planets and planetary systems we observe. In particular, constructing a co- herent model of planetary formation and migration within a circumstellar disc which is capable of producing both hot Jupiters or Solar System-like planetary system is high challenging. Resolved observations of where planets form and how they influence their parent discs provides essential information for tackling this important question. A promising technique for detecting close-in companions is Sparse Aperture Masking (SAM). The technique uses a mask to transform a single aperture telescope into a compact interferometric array capable of reliably detecting point sources at the diffraction limit or closer to a bright star with superior contrasts than extreme AO systems at the cost of smaller fields of view. Applying image reconstruction techniques to the interferometric information allows an observer to recover detailed structure in the circumstellar material. In this thesis I present work on the interpretation of SAM interferometry data on protoplan- etary discs through the simulation of a number of scenarios expected to be commonly seen, and the application of this technique to a number of objects. Analysing data taken as part of a SAM survey of transitional and pre-transitional discs using the Keck-II/NIRC2 instrument, I detected three companion candidates within the discs of DM Tau, LkHα 330, and TW Hya, and resolved a gap in the disc around FP Tau as indicated by flux from the disc rim. The location of all three of the companions detected as part of the survey are positioned in interesting regions of their parent discs. The candidate, LkHα 330 b is a potentially cavity opening companion due to its close radial proximity to the inner rim of the outer disc. DM Tau b is located immediately outside of a ring of dusty material largely responsible for the NIR comment of the disc SED, similar to TW Hya b located in a shallow gap in the dust disc outside another ring of over-dense dusty material which bounds a deep but narrow gap. Both of these companion candidates maybe migrating cores which are feeding from the enriched ring of material. I conducted a more extensive study of the pre-transitional disc, V1247 Ori, covering three epochs and the H-, K- and L-wavebands. Complementary observations with VLT/SPHERE in Hα and continuum plus SMA observations in CO (2-1) and continuum were performed. The orientation and geometry of the outer disc was recovered with the SMA data and determine the direction of rotation. We image the inner rim of the outer disc in L-band SAM data, recovering the rim in all three epochs. Combining all three data sets together we form a detailed image of the rim. In H- and K-band SAM data we observe the motion of a close-in companion candidate. This motion was found to be too large to be adequately explained through a near-circular Keplerian orbit within the plane of the disc around the central star. Hence an alternate hypothesis had to be developed. I postulated that the fitted position of the companion maybe influenced by the emission from the disc rim seen in the L-band SAM data. I constructed a suite of model SAM data sets of a companion and a disc rim and found that under the right conditions the fitted separation of a companion will be larger than the true separation. Under these conditions we find the motion of 2 the companion candidate to be consistent with a near-circular Keplerian orbit within the plane of the disc at a semi-major axis of ∼6 au. The Hα data lack the necessary resolution to confirm the companion as an accreting body, but through the high contrast sensitivities enabled by the state of the art SPHERE instrument I was able to rule out any other accreting body within the gap, unless deeply embedded by the sparse population of MIR emitting dust grains previously inferred to reside within the gap. Through the combination of SAM and SMA data we constrain the 3-D orientation of the disc, and through multi-wavelength SAM observation identify a close- in companion potentially responsible for the gap clearing and asymmetric arm structures seen in previous observations of this target. During my PhD I have contributed to the field of planet formation through the identification of four new candidate protoplanets observed in the discs of pre-main sequence stars. To do so I have quantified the confidence levels of companion fits to SAM data sets and formed synthetic data from models of asymmetric structures seen in these discs. I have described for the first time the effects of extended sources of emission on the fitted results of companion searches within interferometric data sets. I have combined SAM data sets from two separate telescopes with different apertures and masks to produce reconstructed image of an illuminated disc rim with superior uv-coverage. I have used the expertise I have developed in this field to contribute to a number of other studies, including the study of the young star TYC 8241 2652 1, resulting in the rejection of a sub-stellar companion as the cause of the rapid dispersal of the star‘s disc. The companion candidates I have identified here should be followed up to confirm their presence and nature as accreting protoplanets. Objects such as these will provide the opportunity for more detailed study of the process of planet formation in the near future with the next generation of instruments in the JWST and E-ELT. Contents 1 Introduction 14 1.1 Background . 14 2 Star formation and disc evolution 17 2.1 Introduction . 17 2.2 Star formation paradigm . 17 2.2.1 Initial collapse . 19 2.2.2 Formation of a protostar . 20 2.2.3 Pre-main sequence evolution . 21 2.2.4 Formation of the circumstellar disc . 22 2.2.5 Angular momentum evolution . 22 2.3 Protoplanetary disks . 29 2.3.1 Classical . 29 2.3.2 Transitional/Pre-transitional . 31 2.4 Observational constraints on structure . 33 2.4.1 Spectral energy distribution model fitting . 33 2.4.2 Spectroscopic constraints . 35 2.4.3 Sub-millimeter and radio continuum long baseline interferometry . 36 2.4.4 Optical imaging . 37 2.4.5 Variability . 42 2.4.6 Disc clearing mechanisms . 45 2.4.7 Non-dynamical disc clearing mechanisms . 45 2.4.8 Dynamical disc clearing mechanisms . 47 2.5 Chapter Summary . 49 3 Planet formation and protoplanets 50 3.1 Introduction . 50 3.2 Planet formation theory . 50 3.2.1 From dust particles to pebbles . 51 3.2.2 From pebbles to planetesimals . 53 3.2.3 From planetesimals to planetary cores . 56 3.2.4 Giant planet formation . 61 3.3 Circumplanetary discs . 64 3 CONTENTS 4 3.4 Planet-disc dynamical interaction . 67 3.5 Planet-planet dynamical interaction . 70 3.6 Protoplanets . 72 3.6.1 Observational properties . 72 3.6.2 Previous protoplanet observations . 73 3.7 Chapter summary . 79 4 High angular resolution imaging techniques 82 4.1 Introduction . 82 4.2 Single-aperture imaging . 83 4.2.1 Principles of single aperture imaging . 83 4.2.2 Adaptive optics imaging . 85 4.3 Interferometric Imaging . 87 4.3.1 Principles of Interferometry . 87 4.3.2 Observables . 94 4.3.3 Calibrators . 97 4.3.4 Sparse Aperture Masking (SAM) . 98 4.4 Chapter summary . 99 5 Image reconstruction algorithms 101 5.1 Introduction . 101 5.2 Bayesian approach . 103 5.2.1 The likelihood function . 104 5.2.2 The regularisation function . 105 5.2.3 Regularisation weight parameter, µ .................... 107 5.3 Separating star from environment . 108 5.4 Employed image reconstruction algorithm . 109 5.5 Chapter summary . 109 6 Simulation of aperture masking observables 111 6.1 Introduction . 111 6.2 Generating synthetic observations . 111 6.2.1 Degeneracies between derived model parameters . 113 6.3 Numerical simulations of companion and disc scenarios . 114 6.3.1 Small-separation/unresolved companion scenario . 114 6.3.2 Marginally resolved companion scenario . 115 6.3.3 Fully-resolved companion scenario . 116 6.3.4 Asymmetries arising from a disc wall . 116 6.3.5 Asymmetries arising from disc inhomogeneities . 119 6.3.6 The effect on the position of a companion in the presence of a disc . 119 6.4 Summary . 122 CONTENTS 5 7 Keck-II/NIRC2 Pre-Transitional Disk Survey 123 7.1 Context . 123 7.2 Target selection . 124 7.3 Observations . 124 7.4 Results . 127 7.4.1 Detection statistics . 129 7.4.2 Degeneracies . 132 7.4.3 DM Tau . 132 7.4.4 FP Tau . 137 7.4.5 LkHα 330.................................
Recommended publications
  • Imaging Giant Protoplanets with the Elts
    Astro2020 Science White Paper Imaging Giant Protoplanets with the ELTs Thematic Areas: Planetary Systems Star and Planet Formation Formation and Evolution of Compact Objects Cosmology and Fundamental Physics Stars and Stellar Evolution Resolved Stellar Populations and their Environments Galaxy Evolution Multi-Messenger Astronomy and Astrophysics Principal Author: Name: Steph Sallum Institution: University of California, Santa Cruz Email: [email protected] Phone: (831) 459-4820 Co-authors: Vanessa Bailey (Jet Propulsion Laboratory, California Inst. of Technology) Rebecca Bernstein (Carnegie Observatories) Alan Boss (Carnegie Institution) Brendan Bowler (The University of Texas at Austin) Laird Close (University of Arizona) Thayne Currie (NASA-Ames Research Center) Ruobing Dong (University of Victoria) Catherine Espaillat (Boston University) Michael P. Fitzgerald (University of California, Los Angeles) Katherine B. Follette (Amherst College) Jonathan Fortney (University of California, Santa Cruz) Yasuhiro Hasegawa (Jet Propulsion Laboratory, California Inst. of Technology) Hannah Jang-Condell (University of Wyoming) Nemanja Jovanovic (California Inst. of Technology) Stephen R. Kane (University of California, Riverside) Quinn Konopacky (University of California, San Diego) Michael Liu (University of Hawaii) Julien Lozi (National Astronomical Observatory of Japan) Jared Males (University of Arizona) Dimitri Mawet (California Inst. of Technology / Jet Propulsion Laboratory) Benjamin Mazin (University of California, Santa Barbara) Max
    [Show full text]
  • The Subsurface Habitability of Small, Icy Exomoons J
    A&A 636, A50 (2020) Astronomy https://doi.org/10.1051/0004-6361/201937035 & © ESO 2020 Astrophysics The subsurface habitability of small, icy exomoons J. N. K. Y. Tjoa1,?, M. Mueller1,2,3, and F. F. S. van der Tak1,2 1 Kapteyn Astronomical Institute, University of Groningen, Landleven 12, 9747 AD Groningen, The Netherlands e-mail: [email protected] 2 SRON Netherlands Institute for Space Research, Landleven 12, 9747 AD Groningen, The Netherlands 3 Leiden Observatory, Leiden University, Niels Bohrweg 2, 2300 RA Leiden, The Netherlands Received 1 November 2019 / Accepted 8 March 2020 ABSTRACT Context. Assuming our Solar System as typical, exomoons may outnumber exoplanets. If their habitability fraction is similar, they would thus constitute the largest portion of habitable real estate in the Universe. Icy moons in our Solar System, such as Europa and Enceladus, have already been shown to possess liquid water, a prerequisite for life on Earth. Aims. We intend to investigate under what thermal and orbital circumstances small, icy moons may sustain subsurface oceans and thus be “subsurface habitable”. We pay specific attention to tidal heating, which may keep a moon liquid far beyond the conservative habitable zone. Methods. We made use of a phenomenological approach to tidal heating. We computed the orbit averaged flux from both stellar and planetary (both thermal and reflected stellar) illumination. We then calculated subsurface temperatures depending on illumination and thermal conduction to the surface through the ice shell and an insulating layer of regolith. We adopted a conduction only model, ignoring volcanism and ice shell convection as an outlet for internal heat.
    [Show full text]
  • 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).
    [Show full text]
  • Exoplanet.Eu Catalog Page 1 # Name Mass Star Name
    exoplanet.eu_catalog # name mass star_name star_distance star_mass OGLE-2016-BLG-1469L b 13.6 OGLE-2016-BLG-1469L 4500.0 0.048 11 Com b 19.4 11 Com 110.6 2.7 11 Oph b 21 11 Oph 145.0 0.0162 11 UMi b 10.5 11 UMi 119.5 1.8 14 And b 5.33 14 And 76.4 2.2 14 Her b 4.64 14 Her 18.1 0.9 16 Cyg B b 1.68 16 Cyg B 21.4 1.01 18 Del b 10.3 18 Del 73.1 2.3 1RXS 1609 b 14 1RXS1609 145.0 0.73 1SWASP J1407 b 20 1SWASP J1407 133.0 0.9 24 Sex b 1.99 24 Sex 74.8 1.54 24 Sex c 0.86 24 Sex 74.8 1.54 2M 0103-55 (AB) b 13 2M 0103-55 (AB) 47.2 0.4 2M 0122-24 b 20 2M 0122-24 36.0 0.4 2M 0219-39 b 13.9 2M 0219-39 39.4 0.11 2M 0441+23 b 7.5 2M 0441+23 140.0 0.02 2M 0746+20 b 30 2M 0746+20 12.2 0.12 2M 1207-39 24 2M 1207-39 52.4 0.025 2M 1207-39 b 4 2M 1207-39 52.4 0.025 2M 1938+46 b 1.9 2M 1938+46 0.6 2M 2140+16 b 20 2M 2140+16 25.0 0.08 2M 2206-20 b 30 2M 2206-20 26.7 0.13 2M 2236+4751 b 12.5 2M 2236+4751 63.0 0.6 2M J2126-81 b 13.3 TYC 9486-927-1 24.8 0.4 2MASS J11193254 AB 3.7 2MASS J11193254 AB 2MASS J1450-7841 A 40 2MASS J1450-7841 A 75.0 0.04 2MASS J1450-7841 B 40 2MASS J1450-7841 B 75.0 0.04 2MASS J2250+2325 b 30 2MASS J2250+2325 41.5 30 Ari B b 9.88 30 Ari B 39.4 1.22 38 Vir b 4.51 38 Vir 1.18 4 Uma b 7.1 4 Uma 78.5 1.234 42 Dra b 3.88 42 Dra 97.3 0.98 47 Uma b 2.53 47 Uma 14.0 1.03 47 Uma c 0.54 47 Uma 14.0 1.03 47 Uma d 1.64 47 Uma 14.0 1.03 51 Eri b 9.1 51 Eri 29.4 1.75 51 Peg b 0.47 51 Peg 14.7 1.11 55 Cnc b 0.84 55 Cnc 12.3 0.905 55 Cnc c 0.1784 55 Cnc 12.3 0.905 55 Cnc d 3.86 55 Cnc 12.3 0.905 55 Cnc e 0.02547 55 Cnc 12.3 0.905 55 Cnc f 0.1479 55
    [Show full text]
  • The Effect of Close-In Giant Planets' Evolution on Tidal-Induced Migration of Exomoons
    MNRAS 000, 1–9 (2017) Preprint 2 December 2019 Compiled using MNRAS LATEX style file v3.0 The effect of close-in giant planets’ evolution on tidal-induced migration of exomoons J. A. Alvarado-Montes⋆, Jorge I. Zuluaga and Mario Sucerquia Solar, Earth and Planetary Physics Group (SEAP) Computational Physics and Astrophysics Group (FACom) Instituto de F´ısica - FCEN, Universidad de Antioquia, Colombia Calle 70 No. 52-21, Medell´ın, Colombia Accepted 2017 July 8. Received 2017 July 8; in original form 2017 April 6 ABSTRACT Hypothetical exomoons around close-in giant planets may migrate inwards and/or outwards in virtue of the interplay of the star, planet and moon tidal interactions. These processes could be responsible for the disruption of lunar systems, the collision of moons with planets or could provide a mechanism for the formation of exorings. Several models have been developed to determine the fate of exomoons when subject to the tidal effects of their host planet. None of them have taken into account the key role that planetary evolution could play in this process. In this paper we put together numerical models of exomoon tidal-induced orbital evolution, results of planetary evo- lution and interior structure models, to study the final fate of exomoons around evolv- ing close-in gas giants. We have found that planetary evolution significantly affects not only the time-scale of exomoon migration but also its final fate. Thus, if any change in planetary radius, internal mass distribution and rotation occurs in time-scales lower or comparable to orbital evolution, exomoon may only migrate outwards and prevent tidal disruption or a collision with the planet.
    [Show full text]
  • 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.
    [Show full text]
  • SAG-12 Astrometry for Exoplanet Detection
    SAG-12 Astrometry for exoplanet detection Closeout SAG-12: Chair Eduardo Bendek Contributions from: S. Mark Ammons, Rus Belikov, David Bennett, Jim Breckinridge, O. Guyon, A. Gould, T. Henry, S. Hildebrandt, J. Kuhn, V. Makarov, F. Malbet, M. Shao, J. Sahlmann, Shapiro, A. Sozzetti, D. Spergel. 1 ExoPag 15, Grapevine TX, January 2nd 2017 Image Credit: NASA Ames Kepler 186f SAG-12 Closeout 1) Review answers set by the SAG goals: • What is the scientific potential of astrometry for different precision levels? • What are the technical limitations to achieving astrometry of a given precision? • Identify mission concepts that are well suited for astrometry, including synergy with European ones. • Study potential synergies with ground based observatories 2) Deliverable: • Written report • Other requests? ExoPag 15, Grapevine TX, January 2nd 2017 Astrometry science and Link to NASA Roadmaps NASA Science plan 2014, “Discover and study planets around other stars, and explore whether they could harbor life” pg. 74, => Mass measurements are necessary to answer this question Astrophysics 2010– New Worlds, New Horizons in Astronomy and Astrophysics • “search for nearby, habitable, rocky or terrestrial planets with liquid water and oxygen… “ pg. 11, 2020 Vision chapter => Mass measurements are necessary • “Stars will then be targeted that are sufficiently close to Earth that the light of the companion planets can be separated from the glare of the parent star and studied” pg. 39 paragraph 1, On the threshold chapter => Focus on nearby stars, which is compatible with direct imaging and astrometry • “the plan for the coming decade is to perform the necessary target reconnaissance surveys to inform next-generation mission designs while simultaneously completing the technology development to bring the goals within reach.” pg.
    [Show full text]
  • FY13 High-Level Deliverables
    National Optical Astronomy Observatory Fiscal Year Annual Report for FY 2013 (1 October 2012 – 30 September 2013) Submitted to the National Science Foundation Pursuant to Cooperative Support Agreement No. AST-0950945 13 December 2013 Revised 18 September 2014 Contents NOAO MISSION PROFILE .................................................................................................... 1 1 EXECUTIVE SUMMARY ................................................................................................ 2 2 NOAO ACCOMPLISHMENTS ....................................................................................... 4 2.1 Achievements ..................................................................................................... 4 2.2 Status of Vision and Goals ................................................................................. 5 2.2.1 Status of FY13 High-Level Deliverables ............................................ 5 2.2.2 FY13 Planned vs. Actual Spending and Revenues .............................. 8 2.3 Challenges and Their Impacts ............................................................................ 9 3 SCIENTIFIC ACTIVITIES AND FINDINGS .............................................................. 11 3.1 Cerro Tololo Inter-American Observatory ....................................................... 11 3.2 Kitt Peak National Observatory ....................................................................... 14 3.3 Gemini Observatory ........................................................................................
    [Show full text]
  • Exoplanet.Eu Catalog Page 1 Star Distance Star Name Star Mass
    exoplanet.eu_catalog star_distance star_name star_mass Planet name mass 1.3 Proxima Centauri 0.120 Proxima Cen b 0.004 1.3 alpha Cen B 0.934 alf Cen B b 0.004 2.3 WISE 0855-0714 WISE 0855-0714 6.000 2.6 Lalande 21185 0.460 Lalande 21185 b 0.012 3.2 eps Eridani 0.830 eps Eridani b 3.090 3.4 Ross 128 0.168 Ross 128 b 0.004 3.6 GJ 15 A 0.375 GJ 15 A b 0.017 3.6 YZ Cet 0.130 YZ Cet d 0.004 3.6 YZ Cet 0.130 YZ Cet c 0.003 3.6 YZ Cet 0.130 YZ Cet b 0.002 3.6 eps Ind A 0.762 eps Ind A b 2.710 3.7 tau Cet 0.783 tau Cet e 0.012 3.7 tau Cet 0.783 tau Cet f 0.012 3.7 tau Cet 0.783 tau Cet h 0.006 3.7 tau Cet 0.783 tau Cet g 0.006 3.8 GJ 273 0.290 GJ 273 b 0.009 3.8 GJ 273 0.290 GJ 273 c 0.004 3.9 Kapteyn's 0.281 Kapteyn's c 0.022 3.9 Kapteyn's 0.281 Kapteyn's b 0.015 4.3 Wolf 1061 0.250 Wolf 1061 d 0.024 4.3 Wolf 1061 0.250 Wolf 1061 c 0.011 4.3 Wolf 1061 0.250 Wolf 1061 b 0.006 4.5 GJ 687 0.413 GJ 687 b 0.058 4.5 GJ 674 0.350 GJ 674 b 0.040 4.7 GJ 876 0.334 GJ 876 b 1.938 4.7 GJ 876 0.334 GJ 876 c 0.856 4.7 GJ 876 0.334 GJ 876 e 0.045 4.7 GJ 876 0.334 GJ 876 d 0.022 4.9 GJ 832 0.450 GJ 832 b 0.689 4.9 GJ 832 0.450 GJ 832 c 0.016 5.9 GJ 570 ABC 0.802 GJ 570 D 42.500 6.0 SIMP0136+0933 SIMP0136+0933 12.700 6.1 HD 20794 0.813 HD 20794 e 0.015 6.1 HD 20794 0.813 HD 20794 d 0.011 6.1 HD 20794 0.813 HD 20794 b 0.009 6.2 GJ 581 0.310 GJ 581 b 0.050 6.2 GJ 581 0.310 GJ 581 c 0.017 6.2 GJ 581 0.310 GJ 581 e 0.006 6.5 GJ 625 0.300 GJ 625 b 0.010 6.6 HD 219134 HD 219134 h 0.280 6.6 HD 219134 HD 219134 e 0.200 6.6 HD 219134 HD 219134 d 0.067 6.6 HD 219134 HD
    [Show full text]
  • Abstracts of Extreme Solar Systems 4 (Reykjavik, Iceland)
    Abstracts of Extreme Solar Systems 4 (Reykjavik, Iceland) American Astronomical Society August, 2019 100 — New Discoveries scope (JWST), as well as other large ground-based and space-based telescopes coming online in the next 100.01 — Review of TESS’s First Year Survey and two decades. Future Plans The status of the TESS mission as it completes its first year of survey operations in July 2019 will bere- George Ricker1 viewed. The opportunities enabled by TESS’s unique 1 Kavli Institute, MIT (Cambridge, Massachusetts, United States) lunar-resonant orbit for an extended mission lasting more than a decade will also be presented. Successfully launched in April 2018, NASA’s Tran- siting Exoplanet Survey Satellite (TESS) is well on its way to discovering thousands of exoplanets in orbit 100.02 — The Gemini Planet Imager Exoplanet Sur- around the brightest stars in the sky. During its ini- vey: Giant Planet and Brown Dwarf Demographics tial two-year survey mission, TESS will monitor more from 10-100 AU than 200,000 bright stars in the solar neighborhood at Eric Nielsen1; Robert De Rosa1; Bruce Macintosh1; a two minute cadence for drops in brightness caused Jason Wang2; Jean-Baptiste Ruffio1; Eugene Chiang3; by planetary transits. This first-ever spaceborne all- Mark Marley4; Didier Saumon5; Dmitry Savransky6; sky transit survey is identifying planets ranging in Daniel Fabrycky7; Quinn Konopacky8; Jennifer size from Earth-sized to gas giants, orbiting a wide Patience9; Vanessa Bailey10 variety of host stars, from cool M dwarfs to hot O/B 1 KIPAC, Stanford University (Stanford, California, United States) giants. 2 Jet Propulsion Laboratory, California Institute of Technology TESS stars are typically 30–100 times brighter than (Pasadena, California, United States) those surveyed by the Kepler satellite; thus, TESS 3 Astronomy, California Institute of Technology (Pasadena, Califor- planets are proving far easier to characterize with nia, United States) follow-up observations than those from prior mis- 4 Astronomy, U.C.
    [Show full text]
  • 272 — 16 August 2015 Editor: Bo Reipurth ([email protected]) List of Contents
    THE STAR FORMATION NEWSLETTER An electronic publication dedicated to early stellar/planetary evolution and molecular clouds No. 272 — 16 August 2015 Editor: Bo Reipurth ([email protected]) List of Contents The Star Formation Newsletter Interview ...................................... 3 My Favorite Object ............................ 6 Editor: Bo Reipurth [email protected] Perspective ................................... 12 Technical Editor: Eli Bressert Abstracts of Newly Accepted Papers .......... 17 [email protected] Abstracts of Newly Accepted Major Reviews . 48 Technical Assistant: Hsi-Wei Yen New Jobs ..................................... 50 [email protected] Meetings ..................................... 52 Editorial Board Summary of Upcoming Meetings ............. 53 Joao Alves Alan Boss Jerome Bouvier Lee Hartmann Thomas Henning Cover Picture Paul Ho Jes Jorgensen The ∼2 Myr young cluster Westerlund 2 is among Charles J. Lada the most massive known in the Milky Way, with at Thijs Kouwenhoven least a dozen O stars and several Wolf-Rayet stars. Michael R. Meyer It is located towards Carina at a distance of about Ralph Pudritz 6,000 pc. The near-infrared image is about 4.3 pc Luis Felipe Rodr´ıguez wide, and was obtained with WFC3 on HST. Ewine van Dishoeck Hubble 25th Anniversary image. Courtesy STScI. Hans Zinnecker The Star Formation Newsletter is a vehicle for fast distribution of information of interest for as- tronomers working on star and planet formation and molecular clouds. You can submit material for the following sections: Abstracts of recently Submitting your abstracts accepted papers (only for papers sent to refereed journals), Abstracts of recently accepted major re- Latex macros for submitting abstracts views (not standard conference contributions), Dis- and dissertation abstracts (by e-mail to sertation Abstracts (presenting abstracts of new [email protected]) are appended to Ph.D dissertations), Meetings (announcing meet- each Call for Abstracts.
    [Show full text]
  • The Excited Spin State of Dimorphos Resulting from the DART Impact
    Highlights The Excited Spin State of Dimorphos Resulting from the DART Impact Harrison F. Agrusa,Ioannis Gkolias,Kleomenis Tsiganis,Derek C. Richardson,Alex J. Meyer,Daniel J. Scheeres,Matija Ćuk,Seth A. Jacobson,Patrick Michel,Özgür Karatekin,Andrew F. Cheng,Masatoshi Hirabayashi,Yun Zhang,Eugene G. Fahnestock,Alex B. Davis • High-fidelity numerical codes are essential for modeling the long-term spin evolution • DART may excite Dimorphos’ spin, leading to attitude instability and chaotic tumbling • Dimorphos is especially prone to unstable rotation about its long axis • A chaotic spin state will affect the system’s BYORP and tidal evolution • ESA’s Hera mission may be able to place constraints on the system’s tidal parameters arXiv:2107.07996v2 [astro-ph.EP] 29 Jul 2021 The Excited Spin State of Dimorphos Resulting from the DART Impact a < b b a Harrison F. Agrusa , , Ioannis Gkolias , Kleomenis Tsiganis , Derek C. Richardson , Alex c c d e f J. Meyer , Daniel J. Scheeres , Matija Ćuk , Seth A. Jacobson , Patrick Michel , g h i f Özgür Karatekin , Andrew F. Cheng , Masatoshi Hirabayashi , Yun Zhang , Eugene j j G. Fahnestock and Alex B. Davis aDepartment of Astronomy, University of Maryland, College Park, MD, USA bDepartment of Physics, Aristotle University of Thessaloniki, GR 54124 Thessaloniki, Greece cSmead Department of Aerospace Engineering Sciences, University of Colorado Boulder, Boulder, CO, USA dCarl Sagan Center, SETI Institute, Mountain View, CA, USA eDepartment of Earth and Environmental Sciences, Michigan State University,
    [Show full text]