When the Peas Jump Around the Pod: How Stellar Clustering Affects the Observed Correlations Between Planet Properties in Multi-Planet Systems
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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 -
RV Metric New Monday
A Science Metric for Direct Characterization of Known Radial-Velocity Exoplanets Robert A. Brown Space Telescope Science Institute [email protected] June 17, 2013 Abstract Known RV exoplanets are viewed as prime targets for a future high-contrast imaging mission, which may be able to detect and characterize these enigmatic objects in reflected starlight. To help define and differentiate the candidates for such a mission on the basis of scientific performance, and to help set realistic expectations, we develop a science metric, NRV, defined as the estimated number of planets that would be detected and characterized by such a mission. In this report, we estimate upper limits to NRV for missions with apertures in the range 1–2.4 m. We treat both star-shade and coronagraphic missions. 1. Introduction We define the science metric NRV to be the number of known RV exoplanets that satisfy four criteria: #1 permitted pointing: during observations, the angle between the host star and the sun (γ ) must be greater than the solar avoidance angle, γ > γ 1 and, for a star- shade mission, it must also be less than the angle at which the star shade appears illuminated, γ < γ 2 #2 systematic limit: the flux ratio of the planet to the host star, expressed in delta magnitudes ( Δmag ), must be better than the systematic limit in delta magnitudes ( Δmag0 ), i.e. Δmag < Δmag0 #3 wavelength: criteria #1–2 must be satisfied at all wavelengths deemed critical for planet detection and characterization, and particularly for the coronagraph, at the longest critical wavelength (λlc) #4 time: criteria #1–3 must be satisfied at some time during the mission for at least as long as the exposure time required for detection or characterization of a planet as faint as the systematic limit. -
AMD-Stability and the Classification of Planetary Systems
A&A 605, A72 (2017) DOI: 10.1051/0004-6361/201630022 Astronomy c ESO 2017 Astrophysics& AMD-stability and the classification of planetary systems? J. Laskar and A. C. Petit ASD/IMCCE, CNRS-UMR 8028, Observatoire de Paris, PSL, UPMC, 77 Avenue Denfert-Rochereau, 75014 Paris, France e-mail: [email protected] Received 7 November 2016 / Accepted 23 January 2017 ABSTRACT We present here in full detail the evolution of the angular momentum deficit (AMD) during collisions as it was described in Laskar (2000, Phys. Rev. Lett., 84, 3240). Since then, the AMD has been revealed to be a key parameter for the understanding of the outcome of planetary formation models. We define here the AMD-stability criterion that can be easily verified on a newly discovered planetary system. We show how AMD-stability can be used to establish a classification of the multiplanet systems in order to exhibit the planetary systems that are long-term stable because they are AMD-stable, and those that are AMD-unstable which then require some additional dynamical studies to conclude on their stability. The AMD-stability classification is applied to the 131 multiplanet systems from The Extrasolar Planet Encyclopaedia database for which the orbital elements are sufficiently well known. Key words. chaos – celestial mechanics – planets and satellites: dynamical evolution and stability – planets and satellites: formation – planets and satellites: general 1. Introduction motion resonances (MMR, Wisdom 1980; Deck et al. 2013; Ramos et al. 2015) could justify the Hill-type criteria, but the The increasing number of planetary systems has made it nec- results on the overlap of the MMR island are valid only for close essary to search for a possible classification of these planetary orbits and for short-term stability. -
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 -
Arxiv:2010.00015V3 [Hep-Ph] 26 Apr 2021 Galactic Halo Can Scatter with Exoplanets, Lose Energy, and Gles Are the Same Set of Planets, Without DM Heating
MIT-CTP/5230 SLAC-PUB-17556 Exoplanets as Sub-GeV Dark Matter Detectors Rebecca K. Leane1, 2, ∗ and Juri Smirnov3, 4, y 1Center for Theoretical Physics, Massachusetts Institute of Technology, Cambridge, MA 02139, USA 2SLAC National Accelerator Laboratory, Stanford University, Stanford, CA 94039, USA 3Center for Cosmology and AstroParticle Physics (CCAPP), The Ohio State University, Columbus, OH 43210, USA 4Department of Physics, The Ohio State University, Columbus, OH 43210, USA (Dated: April 27, 2021) We present exoplanets as new targets to discover Dark Matter (DM). Throughout the Milky Way, DM can scatter, become captured, deposit annihilation energy, and increase the heat flow within exoplanets. We estimate upcoming infrared telescope sensitivity to this scenario, finding actionable discovery or exclusion searches. We find that DM with masses above about an MeV can be probed with exoplanets, with DM-proton and DM-electron scattering cross sections down to about 10−37cm2, stronger than existing limits by up to six orders of magnitude. Supporting evidence of a DM origin can be identified through DM-induced exoplanet heating correlated with Galactic position, and hence DM density. This provides new motivation to measure the temperature of the billions of brown dwarfs, rogue planets, and gas giants peppered throughout our Galaxy. Introduction{Are we alone in the Universe? This ques- Exoplanet Temperatures tion has driven wide-reaching interest in discovering a 104 planet like our own. Regardless of whether or not we ever find alien life, the scientific advances from finding DM Heating and understanding other planets will be enormous. From a particle physics perspective, new celestial bodies pro- vide a vast playground to discover new physics. -
Survival of Exomoons Around Exoplanets 2
Survival of exomoons around exoplanets V. Dobos1,2,3, S. Charnoz4,A.Pal´ 2, A. Roque-Bernard4 and Gy. M. Szabo´ 3,5 1 Kapteyn Astronomical Institute, University of Groningen, 9747 AD, Landleven 12, Groningen, The Netherlands 2 Konkoly Thege Mikl´os Astronomical Institute, Research Centre for Astronomy and Earth Sciences, E¨otv¨os Lor´and Research Network (ELKH), 1121, Konkoly Thege Mikl´os ´ut 15-17, Budapest, Hungary 3 MTA-ELTE Exoplanet Research Group, 9700, Szent Imre h. u. 112, Szombathely, Hungary 4 Universit´ede Paris, Institut de Physique du Globe de Paris, CNRS, F-75005 Paris, France 5 ELTE E¨otv¨os Lor´and University, Gothard Astrophysical Observatory, Szombathely, Szent Imre h. u. 112, Hungary E-mail: [email protected] January 2020 Abstract. Despite numerous attempts, no exomoon has firmly been confirmed to date. New missions like CHEOPS aim to characterize previously detected exoplanets, and potentially to discover exomoons. In order to optimize search strategies, we need to determine those planets which are the most likely to host moons. We investigate the tidal evolution of hypothetical moon orbits in systems consisting of a star, one planet and one test moon. We study a few specific cases with ten billion years integration time where the evolution of moon orbits follows one of these three scenarios: (1) “locking”, in which the moon has a stable orbit on a long time scale (& 109 years); (2) “escape scenario” where the moon leaves the planet’s gravitational domain; and (3) “disruption scenario”, in which the moon migrates inwards until it reaches the Roche lobe and becomes disrupted by strong tidal forces. -
The 3D Secular Dynamics of Radial-Velocity-Detected Planetary Systems Mara Volpi, Arnaud Roisin, and Anne-Sophie Libert
A&A 626, A74 (2019) Astronomy https://doi.org/10.1051/0004-6361/201834896 & c ESO 2019 Astrophysics The 3D secular dynamics of radial-velocity-detected planetary systems Mara Volpi, Arnaud Roisin, and Anne-Sophie Libert NaXys, Department of Mathematics, University of Namur, Rempart de la Vierge 8, 5000 Namur, Belgium e-mail: [email protected] Received 17 December 2018 / Accepted 26 April 2019 ABSTRACT Aims. To date, more than 600 multi-planetary systems have been discovered. Due to the limitations of the detection methods, our knowledge of the systems is usually far from complete. In particular, for planetary systems discovered with the radial velocity (RV) technique, the inclinations of the orbital planes, and thus the mutual inclinations and planetary masses, are unknown. Our work aims to constrain the spatial configuration of several RV-detected extrasolar systems that are not in a mean-motion resonance. Methods. Through an analytical study based on a first-order secular Hamiltonian expansion and numerical explorations performed with a chaos detector, we identified ranges of values for the orbital inclinations and the mutual inclinations, which ensure the long-term stability of the system. Our results were validated by comparison with n-body simulations, showing the accuracy of our analytical approach up to high mutual inclinations (∼70◦−80◦). Results. We find that, given the current estimations for the parameters of the selected systems, long-term regular evolution of the spatial configurations is observed, for all the systems, (i) at low mutual inclinations (typically less than 35◦) and (ii) at higher mutual inclinations, preferentially if the system is in a Lidov-Kozai resonance. -
Arxiv:1411.4302V2 [Astro-Ph.SR] 5 Dec 2014
Astronomy & Astrophysics manuscript no. AgeAA c ESO 2018 July 24, 2018 Revising the ages of planet-hosting stars A. Bonfanti1; 2, S. Ortolani1; 2, G. Piotto1; 2, and V. Nascimbeni1; 2 1 Dipartimento di Fisica e Astronomia, Università degli Studi di Padova, Vicolo dell’Osservatorio 3, I-35122 Padova, Italy 2 Osservatorio Astronomico di Padova, INAF, Vicolo dell’Osservatorio 5, I-35122 Padova, Italy ABSTRACT Aims. This article aims to measure the age of planet-hosting stars (SWP) through stellar tracks and isochrones computed with the PAdova & TRieste Stellar Evolutionary Code (PARSEC). Methods. We developed algorithms based on two different techniques for determining the ages of field stars: isochrone placement and Bayesian estimation. Their application to a synthetic sample of coeval stars shows the intrinsic limits of each method. For instance, the Bayesian computation of the modal age tends to select the extreme age values in the isochrones grid. Therefore, we used the isochrone placement technique to measure the ages of 317 SWP. Results. We found that ∼ 6% of SWP have ages lower than 0.5 Gyr. The age distribution peaks in the interval [1.5, 2) Gyr, then it decreases. However, ∼ 7% of the stars are older than 11 Gyr. The Sun turns out to be a common star that hosts planets, when considering its evolutionary stage. Our SWP age distribution is less peaked and slightly shifted towards lower ages if compared with ages in the literature and based on the isochrone fit. In particular, there are no ages below 0.5 Gyr in the literature. 1. Introduction In this paper we focus on the ages derived by using isochrones. -
Predictions of Planets for 586 Exosystems and a Method for Predicting Planets in Multi-Planetary Exosystems Valeri Beck
Predictions of planets for 586 exosystems and a method for predicting planets in multi-planetary exosystems Valeri Beck To cite this version: Valeri Beck. Predictions of planets for 586 exosystems and a method for predicting planets in multi- planetary exosystems. 2019. hal-02050412v4 HAL Id: hal-02050412 https://hal.archives-ouvertes.fr/hal-02050412v4 Preprint submitted on 7 Aug 2019 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. Predictions of planets for 586 exosystems and a method for predicting planets in multi-planetary exosystems Valeri Beck*1 *Alfa Carbon® Beck, Berlin, Germany ABSTRACT We have applied a model of planetary system formation in the field of a standing sound wave (the ‘SSW-Model’) to the prediction of planets in 586 multi-planetary exosystems (384 bi- planetary, 127 tri-planetary and 75 exosystems with four or more confirmed planets). We have verified our predictions using transit-like events from the NASA Threshold-Crossing Event (TCE) catalogue, finding that more than 80% of these events are included in our list of exoplanet predictions. We describe a method for predicting the periods and semi-major axes of additional planets for exosystems with two or more confirmed planets. -
Revising the Ages of Planet-Hosting Stars⋆
A&A 575, A18 (2015) Astronomy DOI: 10.1051/0004-6361/201424951 & c ESO 2015 Astrophysics Revising the ages of planet-hosting stars? A. Bonfanti1;2, S. Ortolani1;2, G. Piotto1;2, and V. Nascimbeni1;2 1 Dipartimento di Fisica e Astronomia, Università degli Studi di Padova, Vicolo dell’Osservatorio 3, 35122 Padova, Italy e-mail: [email protected] 2 Osservatorio Astronomico di Padova, INAF, Vicolo dell’Osservatorio 5, 35122 Padova, Italy Received 10 September 2014 / Accepted 14 November 2014 ABSTRACT Aims. This article aims to measure the age of stars with planets (SWP) through stellar tracks and isochrones computed with the PAdova and TRieste Stellar Evolutionary Code (PARSEC). Methods. We developed algorithms based on two different techniques for determining the ages of field stars: isochrone placement and Bayesian estimation. Their application to a synthetic sample of coeval stars shows the intrinsic limits of each method. For instance, the Bayesian computation of the modal age tends to select the extreme age values in the isochrones grid. Therefore, we used the isochrone placement technique to measure the ages of 317 SWP. Results. We found that ∼6% of SWP have ages lower than 0.5 Gyr. The age distribution peaks in the interval [1.5, 2) Gyr, then it decreases. However, ∼7% of the stars are older than 11 Gyr. The Sun turns out to be a common star that hosts planets, when considering its evolutionary stage. Our SWP age distribution is less peaked and slightly shifted towards lower ages if compared with ages in the literature and based on the isochrone fit. -
Table A1. Planets Discovered by Measuring the Radial Velocities of the Parent Stars Before 17 Oct
Table A1. Planets discovered by measuring the radial velocities of the parent stars before 17 oct. 2017 Minimum detectable projective Upper Lower Minimum Orbital mass of the Orbital Projective error limit error limit Radius projective Duration of Mass of period for planet with period, mass of the of the of the of the (O-C), mass of the Group No. Planet observations, the star, the orbit the orbital days planet, projective projective star, m/s planet number days mʘ at 3R*, period equal mJ mass of the mass of the mʘ detectable days to the planet planet at 3R*, mE duration of observations, mE 1 Kepler-407 c 3000 12,6 6,3 6,3 1,00 1,01 – 2 BD+20 2457 c 621,99 1833 12,47 2,8 49 60,00 123,358 928,4 2282,4 1, 4 3 HD 87646 b 13,481 12,4 0,7 0,7 1,12 1,55 – 4 HIP 67537 b 2557 4419 11,1 0,4 1,1 2,41 8,69 8,0 16,501 57,3 369,2 1, 4 5 HD 220074 b 672,1 1360 11,1 1,8 1,8 1,2 49,7 57,40 192,485 585,5 1123,4 1, 4 6 HD 110014 b 835,5 2950 11,09 1 1 2,17 20,9 45,8 39,306 408,3 1722,5 1, 4 7 HD 1062701 b 2890 1484 11,0? 0,8 0,8 1,32 2,5 8 HD 114762 b 83,915 6901 10,98 0,09 0,09 0,83 1,24 27,40 0,912 36,8 721,6 1, 4 9 TYC 4282-00605-1 b 101,54 1203 10,78 0,12 0,12 0,97 16,2 23,02 40,492 121,2 375,4 1, 4 10 HD 38801 b 696,3 1143 10,7 0,5 0,5 1,36 2,53 6,5 2,077 15,9 130,7 1, 2, 3 11 BD-13 2130 b 714,3 10,6 2,4 – 12 HD 156846 b 359,555 2686 10,57 0,29 0,29 1,35 2,12 6,06 1,599 13,6 161,2 1, 3 13 11 Umi b 516 1287 10,50 2,47 2,47 1,80 24,08 27,5 53,003 239,3 692,9 1, 4 14 HD 219077 b 5501 4850 10,39 0,09 0,09 1,05 1,91 7,63 1,55 14,2 208,2 1, 3 15 18 Del b 993 -
Analysis of Angular Momentum in Planetary Systems and Host Stars
Analysis of Angular Momentum in Planetary Systems and Host Stars by Stacy Ann Irwin Bachelor of Science, Computer Science University of Houston 2000 Master of Science, Space Sciences Florida Institute of Technology 2009 A dissertation submitted to the College of Science at Florida Institute of Technology in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Space Sciences Melbourne, Florida July 2015 c Copyright 2015 Stacy Ann Irwin All Rights Reserved The author grants permission to make single copies We the undersigned committee hereby recommend that the attached document be accepted as fulfilling in part the requirements for the degree of Doctor of Philosophy in Space Sciences. \Analysis of Angular Momentum in Planetary Systems and Host Stars," a dissertation by Stacy Ann Irwin Samuel T. Durrance, Ph.D. Professor, Physics and Space Sciences Major Advisor Daniel Batcheldor, Ph.D. Associate Professor, Physics and Space Sciences Committee Member Darin Ragozzine, Ph.D. Assistant Professor, Physics and Space Sciences Committee Member Semen Koksal, Ph.D. Professor, Mathematical Sciences Outside Committee Member Daniel Batcheldor, Ph.D. Professor, Physics and Space Sciences Department Head Abstract Analysis of Angular Momentum in Planetary Systems and Host Stars by Stacy Ann Irwin Dissertation Advisor: Samuel T. Durrance, Ph.D. The spin angular momentum of single Main Sequence stars has long been shown to follow a primary power law of stellar mass, J M α, excluding stars of <2 solar masses. Lower mass / stars rotate more slowly with and have smaller moments of inertia, and as a result they contain much less spin angular momentum.